Soil characterization by diffusion measurements by Truman Winfield Massee A thesis submitted to the Graduate Faculty in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY in Crop and Soil Science Montana State University © Copyright by Truman Winfield Massee (1973) Abstract: A mathematical derivation from diffusion theory was applied to soil diffusive flow to an exchange resin sink. The measured flux was used to estimate some factors influencing soil fertility. These included initial (before diffusive flow) solution phosphorus and potassium concentration, adsorbed concentration, buffer capacity, soil impedance values, soil solution concentration changes with time of diffusion, and quantity of fertilizer needed to bring about predetermined flux rates. At least two diffusion measurements were needed for each soil. One was needed from an unspiked portion (no fertilizer or chloride added) and one from a spiked portion. Reasonable precision was obtained in measuring impedance factors from determining the quantity of added chloride that diffused, and resulting values were similar to ones previously published. The calculated solution and adsorbed quantities of potassium (from diffusion) were usually nearly the same as were measured from routine chemical methods determining solution and labile amounts. There was variation in the quantity of calculated solution and adsorbed phosphorus from diffusion methods depending on the quantity of spiking done. This variation was believed to be associated with non-linear adsorption isotherms as were depicted from the chemical extractions done. Plant uptake of phosphorus on various soils fairly well Correlated with diffusive flux from these soils, while potassium-plant correlations were much better. A potential was evident for estimating fertilizer needs from diffusion flux measurements, expe-cially for potassium. S O IL C H A R A C T E R IZ A T IO N B Y D IF F U S IO N M E A S U R E M E N T S by T R U M A N W IN F IE L D M A S S E D A t h e s i s s u b m i t t e d to th e G r a d u a t e F a c u l t y in p a r t i a l f u l f i l l m e n t o f th e r e q u i r e m e n t s f o r th e d e g r e e of D O C T O R O F P H IL O S O P H Y in C r o p a n d S o il S c ie n c e . A p p ro v e d : f t , H e a d , M a jo r D e p a rtm e n t M O N T A N A S T A T E U N IV E R S IT Y B o z e m a n ^ M o n ta n a A u g u s t, 1 9 7 3 ABSTRACT A m a t h e m a t i c a l d e r i v a t i o n f r o m d if f u s io n t h e o r y w a s a p p l ie d to s o i l d if f u s iv e flo w to a n e x c h a n g e r e s i n s in k . The m e a s u re d f lu x w a s u s e d to e s t i m a t e s o m e f a c t o r s i n f l u e n c in g s o i l f e r t i l i t y . T h e s e in c lu d e d i n i t i a l ( b e f o r e d if f u s iv e flo w ) s o lu ti o n p h o s p h o r u s an d p o ta s s iu m c o n c e n tra tio n , a d s o rb e d c o n c e n tra tio n , b u ffe r c a p a ­ c i t y , s o i l im p e d a n c e v a l u e s , s o i l s o lu ti o n c o n c e n t r a t i o n c h a n g e s w ith t i m e o f d i f f u s io n , a n d q u a n t ity o f f e r t i l i z e r n e e d e d to b r i n g a b o u t p r e d e t e r m i n e d f lu x r a t e s . A t l e a s t tw o d if f u s io n m e a s u r e ­ m e n ts w e re n e e d e d fo r e a c h s o il. O ne w a s n e e d e d f r o m a n un­ s p ik e d p o r t i o n (no f e r t i l i z e r o r c h l o r i d e a d d e d ) a n d o n e f r o m a s p ik e d p o r t i o n . R e a s o n a b l e p r e c i s i o n w a s o b ta in e d in m e a s u r i n g im p e d a n c e f a c t o r s f r o m d e t e r m i n i n g th e q u a n t i t y o f a d d e d c h l o r i d e t h a t d if ­ f u s e d , a n d r e s u l t i n g v a l u e s w e r e s i m i l a r to o n e s p r e v i o u s l y p u b lis h e d . T h e c a l c u l a t e d s o lu ti o n a n d a d s o r b e d q u a n t i t i e s o f p o t a s s i u m ( f r o m d if f u s io n ) w e r e u s u a l l y n e a r l y th e s a m e a s w e r e m e a s u r e d f r o m r o u t i n e c h e m i c a l m e th o d s d e t e r m i n i n g s o lu ti o n a n d la b ile a m o u n ts . T h e r e w a s v a r i a t i o n in th e q u a n tity o f c a l c u l a t e d s o l u t i o n a n d a d s o r b e d p h o s p h o r u s f r o m d if f u s io n m e th o d s d e p e n d in g o n th e q u a n t ity o f s p ik in g d o n e . T h is v a r i a t i o n w a s b e l ie v e d to b e a s s o c i a t e d w ith n o n - l i n e a r a d s o r p t i o n i s o t h e r m s a s w e r e d e p ic te d f r o m th e c h e m i c a l e x t r a c t i o n s d o n e . P l a n t u p ta k e o f p h o s p h o r u s o n v a r i o u s s o i l s f a i r l y w e ll C o r ­ r e l a t e d w ith d if f u s iv e f lu x f r o m t h e s e s o i l s , w h ile p o t a s s l u m - p l a n t c o rre la tio n s w e re m uch b e tte r. A p o te n tia l w a s e v id e n t f o r e s t i ­ m a t i n g f e r t i l i z e r n e e d s f r o m d if f u s io n f lu x m e a s u r e m e n t s , e s p e ­ c ia lly fo r p o ta s s iu m . ii ACKNOW LEDGEM ENTS T h e l i s t i n g o f p e r s o n s w h o c o n t r i b u t e d to t h i s s tu d y i s le n g th y , a n d s p a c e d o e s n o t a llo w a d e t a i l e d d e s c r i p t i o n o f e a c h i n d i v i d u a l r s c o n trib u tio n . E v e n s o , th e a u t h o r g r e a t f u l l y a c k n l w l e d g e s t h e i r a s s i s t a n c e a n d e x p r e s s e s h i s a p p r e c i a t i o n a n d g r a t i t u d e w ith th e a l p h a ­ b e t i c a l l i s t i n g s o f th e f o llo w in g p e r s o n s , p l a c e d u n d e r s e v e r a l g e n e r a l ■ <* s u b je c t m a tte r c a te g o r ie s . . M y G r a d u a te C o m m itte e : ■ D r s . C . S c o tt C o o p e r , A . H a y d e n F e r g u s o n , R a l p h A . O ls e n , J a m e s R . S im s , a n d E a r l O. S k o g le y ( C h a i r m a n ) , a l l o f M o n ta n a S t a t e U n i v e r s i t y . A d v ic e o n d if f u s io n t h e o r y a n d a p p l ic a t io n : D rs. W. D o ra l K e m p e r, C o lo ra d o S ta te U n iv e r s ity ; P h illip L o w , P u r d u e ' U n i v e r s i t y ; R o b e r t L . N i c k e l s o n , M o n ta n a S t a t e U n i v e r s i t y ; S t e r l i n g R . O ls e n , ■A R S - USD A , F o r t C o l l i n s , C o lo r a d o ; P h i l l i p H . N y e , O x f o r d U n i v e r s i t y ; a n d R o n a ld E . P h i l l i p s , U n i v e r s i t y o f K e n tu c k y . L a b o ra to ry an d Shop A s s is ta n c e : A s a e l D ilw o r th , A R S - USD A , K i m b e r l y , I d a h o ; J e a n n e E a r l , M u r ta u g h , I d a h o ; C l a r e n c e I - H a y d e n , A R S -U S D A , K i m b e r l y , I d a h o ; m y f a m i l y - - B e v ­ e r l y , R a c h e l, R e b e c c a , a n d D a n i e l M a s s e e , T w in F a l l s , I d a h o ; a n d H a r o l d W a g g o n e r , A R S - USD A , K i m b e r l y , Id a h o . 1 S o ils c o l l e c t i o n a n d i d e n t i f i c a t i o n : S te v e n B o o th , C a l i f o r n i a r e s i d e n t ; A . L . B la c k , A R S - USD A , S id n e y , M o n ta n a , C h a r l e s C a s e , S C S - U SD A , G o o d in g , I d a h o ; D r . W i l l i a m iv R. G ill, A R S - U SD A , A u b u r n , A l a b a m a ; R o n a ld G i t h e n s , J u n c t io n C ity , O re g o n , F a r m e r ; R o b e rt H agenow , f a r m e r ; D r e D o r d o n H u n tin g to n , I n d ia n a U n iv e rs ity of C a lifo rn ia ; A lv in Kfohl, I l l i n o i s f a r m e r ; H e r b e r t K o h l, I l l i n o i s f a r m e r ; I a n d G e o r g e E e O t t e , S C S - U SD A , H i l l s b o r o , O r e g o n . R e s i n T e c h n o lo g y ; W o rk s, S t, M a th e m a tic s : D r e W a lte r D e a n , M a llin c k ro d t C h e m ic a l L o u i s ,. M i s s o u r i . C h a r le s B ro c k w a y , • U n iv e rs ity o f Id a h o ; D r, R o b e rt B ur m an . A R S - U SD A , U n i v e r s i t y o f W y o m in g ; H , K im b e rly , Id ah o ; D r. W. R. v e r s it y o f W isc o n s in ; P e d ro H e rn a n d e z , B en J , P ra tt, A R S - U SD A , K im b e rly , D a le F i s h e r , G a rd n e r, U n i­ U n i v e r s i t y o f Idah o ; Id a h o ; a n d J o s de S o n n e v il le , ■ U n i v e r s i t y o f I d a h o . M a n u s c rip t re v ie w : W a r r e n W . R a s m u s s e n , A R S - U SD A , K im b e rly , Id a h o . M a n u s c r i p t ty p i n g : / D o ris A d a m s , Jero m e, T w in F a l l s , I d a h o ; a n d D a la W a lto n , Id a h o ; B e v e r l y M a s s e e , B u rle y , U se o f la b o r a to r y a n d l i b r a r y f a c i l i t i e s : D r s . an d H e n ry F . To th e s e n a m e d , a g in g , c ritic a l, M ay l a n d , A R S - U SD A , a n d to o t h e r s , and c o n c e rn e d , I .. v Id ah o . M a r v in E . K im b e rly , Jensen Id ah o „ w h o h a v e be,e n p a t i e n t , e n c o u r­ th e a u t h o r w i l l a l w a y s b e in d e b te d . TA B LE O F CONTENTS Page I IN T R O D U C T IO N . L i t e r a t u r e R e v ie w . H y p o th e s is . . ............................... . . . . . . . . . . . . I . . . E X P E R I M E N T A L M E T H O D S A N D M A T E R IA L S T h e o r e t i c a l D e v e lo p m e n t . 23 . . . . . 25 .... . . . . . . . . . . . 25 S o ils U s e d a n d G e n e r a l C h e m i c a l a n d P h y s ic a l A n a ly s is ..................... 29 C h e m i c a l D e t e r m i n a t i o n o f S o lu ti o n a n d S o r b e d C o n c e n tr a tio n and C a p a c ity F a c t o r s f o r P h o s ­ p h o r u s a n d P o t a s s i u m ........................................... 33 D e t e r m i n a t i o n o f S o lu tio n a n d S o r b e d C o n c e n ­ t r a t i o n , B u f f e r C a p a c i t y a n d I m p e d a n c e V a lu e s , b y D i f f u s i o n .......................... 34 D e t e r m i n a t i o n o f P l a n t U p ta k e f r o m S o ils 38 ,R E S U L T S A N D I N T E R P R E T A T IO N S ...... . . . . . . . . . . . 39 I m p e d a n c e V a lu e s f r o m C h l o r i d e D if f u s io n . . . . 39 D if f u s io n a n d C h e m i c a l l y D e t e r m i n e d S o il P o t a s s i u m . „ . •............................... - • 41 P l a n t P o t a s s i u m U p ta k e C o m p a r e d to C h e m i c a l a n d D if f u s io n T e s t s . . . . . . . . . . . . . . . . .4 5 . D if f u s io n a n d C h e m i c a l l y D e t e r m i n e d S o il P h o sp h o ru s . . . . . . . . . . . . . . . . . . . . 50 P l a n t P h o s p h o r u s U p ta k e C o m p a r e d to C h e m ­ i c a l a n d D if f u s io n T e s t s . . . . . . . . . . . . . . . 55 SUM M ARY i/ . . . . . . . * . . . @. , . . / • vi . 59 Page R E F E R E N C E S C IT E D A P P E N D IX E S . . . 62 .......................... 69 A p p e n d ix A - R e s u l t s o f c h e m i c a l d e t e r m i n ­ a t io n s o f s o i l p o t a s s i u m - ( s o i l b u lk d e n s i t y i s in c lu d e d f o r c o n v e r t i n g v o lu m e d a t a to a w e ig h t b a s i s i f d e s i r e d ) .......................... 6.9 A p p e n d ix B - R e s u l t s o f c h e m i c a l d e t e r m i n a ­ tio n s o f s o i l p h o s p h o r u s - ( s o i l b u lk d e n s i t y i s in c lu d e d f o r c o n v e r t i n g v o lu m e d a t a to a w e ig h t b a s i s i f d e s i r e d ) . . . . . . . . . . . . . 70 A p p e n d ix C - C a l c u l a t e d im p e d a n c e v a l u e s (I) a n d q u a n tity o f p o t a s s i u m d i f f u s i n g to r e s i n s i n k s u r f a c e (7 . 92 c m 8 ) p e r 2 4 - h o u r p e r i o d (JS4^_) . . . . . . . . . . . o e . . . * . . . . . . . 71 Appendix D - Calculated impedance values (I) a n d q u a n t ity o f p h o s p h o r u s d if f u s in g to r e s i n s i n k s u r f a c e (7 . 92 c m 8 ) p e r 2 4 - h o u r p e r i o d (M j.) . . . . . . . . . . . . . . . . . . . . v ii • / ' ■ ! ' ;' 72 LIST O F T A B L E S Page R e s u lts o f s o il p h y s ic a l an d c h e m ic a l d e te r m in a tio n s on s o ils u s e d in e x p e r i- I. I Yl B n t S 2. 3o 4. / ' 5. I 6. 7. o e e o o e e o e ' e e e e e e e e o 30 C o m p a ris o n s b e tw e e n c h e m ic a l d e te r m in ­ a t i o n s a n d d if f u s io n d e t e r m i n a t i o n s o f l a b i l e K , (C + C ), a n d s o l u t i o n K , (C ) . 42 C o m p u te d q u a n t i t i e s o f K s p ik in g n e e d e d to o b ta in ( a c c u m u l a t i v e f lu x p e r d ay ) v e r s u s q u a n tity o f K a c t u a l l y s u p p lie d t o o b ta in ........................................ 46 R e s u lts of s im p le lin e a r c o r r e l a t i o n ' r e l a t i n g p l a n t u p ta k e o f p o t a s s i u m to ■ c h e m i c a l a n d d if f u s io n t e s t s . . . « ....................... 48 C o m p a ris o n s b e tw e e n c h e m ic a l d e te r m in ' a t io n s a n d d if f u s io n d e t e r m i n a t i o n s o f l a b i l e P , (C + C ), s o l u t i o n P , (C ) , a n d (R + l) „ S. . . ° . 52 S lo p e o f p h o s p h o r u s a d s o r p t i o n i s o t h e r m fro m c h e m ic a l d e te rm in a tio n s a s d e ­ p ic te d in te x t . . . . . . . . . . . . . . . . . 54 C o m p u te d q u a n t i t i e s o f p h o s p h o r u s s p ik in g n e e d e d to o b t a i n ( a c c u m u l a t i v e flu x p e r d a y ) v e r s u s q u a n t ity .o f s p ik in g a c t u a l l y s u p p l i e d to o b ta in 58 v iii. I L I S T O F F IG U R E S F ig u re 1. D if f u s io n c e l l s h o w in g : A - D i m e n s i o n s B - C e l l i n o p e r a t i o n C - M e th o d o f e x ­ t r a c t i n g r e s i n . . . . . ...................... . . . . . . 2. . 3. 4. 5» Page 35 C o m p u te d s o l u t i o n c o n c e n t r a t i o n o f c h l o r i d e a s r e l a t e d to d i s t a n c e f r o m s i n k , a f t e r d if f u s in g o n e d a y . . . . . . . . . .40 A d s o r b e d p o t a s s i u m c o n c e n t r a t i o n (C ) f o r s o i l s . C o m p a r i s o n i s m a d e b e tw e e n tw o s p ik in g r a t e s to c a l c u l a t e C s 44 R e la tio n s h ip s b e tw e e n p la n t p o ta s s iu m . u p t a k e a n d o n e - d a y a c c u m u l a t i v e d if f u s iv e f lu x 49 . Relationships between plant phosphorus c o n t e n t a n d s o i l q u a n t ity a s m e a s u r e d b y t h r e e m e th o d s . . . . . . . . . . . . . . . . ■ Z/ / I I ix . 56 . / ' INTRODUCTION L ite r a tu r e Review A lthough th e d if f u s io n p r o c e ss was e x p la in e d on a s c i e n t i f i c b a s is by F ic k more than a cen tu ry a g o , i t was o n ly s in c e 1950 th a t i t was r e c o g n iz e d a s an im p ortan t phenomenon r e g u la t in g th e tr a n s p o r t o f many . n u t r ie n t io n s to p la n t r o o t s . In a d d itio n to th e academ ic in t r ig u e a s s o c ia t e d w ith t h i s r e l a t io n s h i p , v a lu a b le a p p lic a t io n s may be im p le­ m ented. These in c lu d e th e measurement and r e g u la tio n o f s o i l f e r t i l i t y , and p rob ab ly p la n t management and g e n e t ic s e le c t io n ., In 1855 F ic k , a m ed ica l p h y s i o lo g is t a t th e U n iv e r s ity o f Z u rich, was ' th e f i r s t to show how th e h e a t flo w eq u a tio n s d ev elo p ed by F o u rier co u ld be a p p lie d to d i f f u s i o n . Thus, . even though o n ly a co m p a ra tiv ely few a n a l y t i c a l s o lu t io n s ( o f d i f f u s i o n - l i k e phenomena) were known th en , th e fundam ental p r i n c i p l e ( s ) were e s t a b lis h e d . "It ^is n o t s u r p r is in g th a t i t took such a lo n g tim e fo r a g ro n o m ists to r e c o g n iz e th e s i g n i f i ­ can ce o f t h i s . • F i r s t , th e q u a n tity o f s o lu t io n flo w (som etim es termed .. ' t r a n s p ir a t io n , v is c o u s , or mass flo w ) co u ld a ls o c o n c e iv a b ly accou n t fo r la r g e q u a n t it ie s o f Io n s b e in g tr a n s fe r r e d to p la n t r o o t s - w h ich , I • was a v a lid assum ption fo r c e r t a in n u t r ie n t s . - T his tr a n s f e r p ro cess was b e lie v e d to be accom panied by a ren ew al o f s o lu t io n io n s from, m in era l r e s e r v e s , an oth er p la u s ib le p r o c e s s i These two f a c e t s were fir m ly lin k e d to g e th e r by Cameron (1911) in one o f th e f i r s t d e t a ile d works d e a lin g w ith th e s o i l s o l u t i o n . , 2 S in ce th en , a g r e a t d e a l o f s p e c u la t io n has e x is t e d on how to m easure th e a c t i v i t y o f s o i l s o lu t io n s so th a t d ir e c t in t e r p r e t a t io n s co u ld be made. For exam ple, H oagland, in h is f i r s t le c t u r e g iv e n a t Harvard U n iv e r s ity under th e P ra th er L ectu resh ip (1 9 4 4 ), to ld o f the background o f th e ! i n i t i a l work in C a lif o r n ia p r io r to 1920. He s a id "much had been w r it t e n about th e s o i l s o lu t io n and c o n tr o v e r sy had n o t ceased . I t was ap p aren t t h a t ex p erim en ta l ev id e n c e was most inadequate^ G e n e r a lly , ch em ica l a n a ly s is had been made on f i e l d sam ples o f s o i l under no adequate c o n t r o l." To o b ta in b e t t e r c o n t r o l, he to ld how 13 s o i l s from th e S ta te w ere s e le c t e d and tw o-ton sam ples o f each were sent to Berkeley for s o i l solution analysis while being cropped. had been done fo r 27 y e a r s a t th e tim e o f th e L e c tu r e sh ip . c lu d in g remarks about th e s e s t u d ie s were ". . . i t T his Some con­ has become apparent th a t s o i l s o lu t io n s can o f t e n be more d i l u t e than th o se o f our o r i g in a l s e t o f s o i l s , and s t i l l p la n t s w i l l n o t n e c e s s a r ily f a i l to absorb adequate amounts o f n u t r ie n t v io n s . Thus th e co n cep t o f esu p p ly in g power8 and th e i n t e r r e l a t i o n o f th e s o l i d to th e liq u id ph ase o f the s o i l became c o n s id e r a t io n s o f paramount s ig n if ic a n c e and th ey are so to d a y ." A n u t r ie n t o f p a r t ic u la r c o n s id e r a tio n in th e s e remarks was p h osphorus. I t had been found to be below one ppm in many s o lu t io n sa m p les, even a t th e b eg in n in g o f th e cro p p in g p e r io d . A ls o , p otassiu m was low - u s u a lly l e s s than 20 ppm. Byers e t . a l (1938) ex p ressed s im ila r th ou gh ts in 1938 in w r it in g ab ou t th e s o i l s o lu t io n , and s p e c u la te d on methods o f e x t r a c t in g 88. , »: 3 none o f w hich i s w h o lly s a t i s f a c t o r y . When such s o i l e x t r a c t s are o b ta in e d , i t i s g e n e r a lly found th a t th e c o n c e n tr a tio n o f th e s o lu b le s a l t s in th e s o lu t io n i s l e s s than i s req u ir ed in a r t i f i c i a l n u t r ie n t s o lu t io n s to produce co rresp o n d in g r e s u l t s . . . . I t seems th a t p a rt . . ' o f th e s e r e l a t io n s a re to be a sc r ib e d to th e p resen ce o f c o l l o i d s in th e s o i l s . In g e n e r a l, th e c o n c e n tr a tio n o f any s o lu t io n i s u s u a lly g r e a t e s t in th e f il m a d ja c e n t to any s o l i d s u r fa c e „ . . Thus, th e y , a s d id H oagland, q u e stio n e d why th e e x tr a c te d s o i l s o lu t io n i s to o low to a cco u n t fo r proper p la n t grow th, and p rop ose th a t e x t r a c t io n methods do n o t d u p lic a t e what a p la n t r o o t may e n c o u n t e r .• More recent d a ta by Barber (1962), and Barber (1 9 6 8 ), s t i l l ,in d icate, la r g e d if f e r e n c e s in measured a c t i v i t i e s o f s o i l s o lu t io n s fo r v a r io u s p r o d u c tiv e s o i l s . T his f a c t s u b s t a n t ia t e s th e im p r a c t ic a lit y o f u sin g a v era g es fo r draw ing c o n c l u s i o n s F o r p h osphorus, Olsen^ e t a l (1962) con clud ed (w ith a p p lic a b le l i t e r a t u r e q u o ta tio n s n o t shown h e r e in ) ’’F e r t i l e s o i l s u s u a lly c o n ta in 0 .2 to 0 .3 ppm P in th e s o i l s o lu t io n , and a corn p la n t ta k es up 250 to 350 g o f w ater p er g o f d ry m a tter. , I Thus, v is c o u s flo w o f w ater used by th e p la n t would su p p ly 2 to 4% o f th e t o t a l P taken up by th e p la n t ; ” Barber e t a l (1 9 6 2 ), a f t e r study-r in g 145 p red om in an tly m idw est s o i l s and by u sin g th e same rea so n in g a s O lsen e t a l (1 9 6 2 ), concluded t h a t o n ly one p e r c e n t o f th e phosphorus and 10 p e r c e n t o f th e p o ta ssiu m co u ld be tr a n s fe r r e d to th e r o o t by mass flo w a lo n e . R esearch on o th er n u t r ie n t s , summarized in th e more r e c e n t r ev iew by O lsen and Kemper (1968) in d ic a te d th a t u s u a lly th e tr a n sp o r t I 1 • V / ^ ' . I • 1 . . ' . . X 4 .^r o n J m anganese, boron , cop p er, z i n c , molybdenum and som etim es n i t r o ­ gen and s u lf u r must be supplem ented by m echanism (s) in a d d itio n to mass flo w . E arly a ttem p ts to d e s c r ib e th e means ( in a d d itio n to mass flo w ) by w hich io n s were tr a n s fe r r e d to r o o t s have c r e a te d an array o f i n t e r e s t ­ in g c o n c e p ts . One w hich provoked much thought and c o n tr o v e r sy was th a t o f " c o n ta c t exchange" w hich was developed by Jenny and O v e r str e e t (1939) in 1939, They proposed th a t exch a n g ea b le s o i l c a t io n s , and a l s o c a t io n s on th e p la n t r o o t s u r f a c e , moved about in an o s c i l l a t i n g volum e. These volum es o v erla p p ed , and whenever a neighbor pair o f io n s sim u lta n e o u sly happened to be c l o s e s to each o t h e r - s origin al a ttra ctiv e s i t e than , I t h e ir own, th ey traded ,s i t e s . In t h i s manner io n s exchanged between p la n t r o o t s and charged s o i l p a r t i c l e s - and by a s im ila r a c t io n , betw een s i t e s on s o i l p a r t i c l e s a t w i l l . From t h is co n cep t i t was co n - , elu d ed th a t th e s o i l s o lu t io n was n o t n e c e s s a r y to a cco u n t fo r th e t r a n s f e r o f io n s . Bray (1 9 5 4 ), how ever, argued "A s i n g l e r o o t , to be f u n c t io n a l, must se c u r e many tim es th e amounts o f n u t r ie n t s th a t are to be found on th e im m ediate s u r fa c e o f a c la y m in eral p a r t i c l e w ith which i t may be in c o n t a c t . R eg a rd less o f w hether th e r o o t and c la y s u r fa c e s a re so c l o s e t h a t c o n ta c t exch an ge, a s p o s tu la te d by Jenny and O v e r str e e t (1939) can ta k e p la c e , th e amount o b ta in ed from th e im m ediate c o n ta c t would be sm a ll and i n s u f f i c i e n t to make th e r o o t f u n c t io n a l. The s i g n i f i c a n t so u rce o f n u t r ie n t s to th e r o o t su r fa c e comes from movement or d if f u s i o n i n t o th e f ilm o f w ater betw een th e r o o t s u r fa c e 5 and th e s o i l s u r fa c e ," B ra y 's c o n c lu s io n d id n o t s p e c if y a llo w a n ce s fo r th e ren ew al o f io n s on th e c la y exchange s i t e by c o n ta c t exchange w ith o th e r c la y m a t e r ia l, even i f he d id c o n s id e r t h i s in h i s comput­ a t io n s ; However, Brown (1953) had j u s t com pleted an exp erim en t th a t showed th a t io n tr a n sfe r , w ith o u t li q u i d f ilm media was n o n - e x is t e n t , under th e c o n d itio n s he im posed. He had con verted p a r t o f a s o i l sam ple to H -cla y and e n c lo se d i t in a perm eable membrane. T his was th en b u ried in th e n a tu r a l p o r tio n o f s o i l so th a t ion. exchange cou ld ta k e p la c e betw een th e two sa m p les. With s o i l w ater c o n te n ts s im ila r . to th o se where p la n t r o o t s t h r iv e , io n exchange was r a p id . H o w ev er,. . when the water content.was reduced to near w iltin g point, the quantity .. th a t exchanged a ls o d e c r e a se d toward z e r o . s o lu t io n was n e c e s s a r y fo r t r a n s f e r . f e r t o "m igration" and " d iffu s io n " . T his in d ic a te d th a t th e Brown (1953) a s c r ib e d th e tr a n s­ Thus, Brown's s ta te m e n ts , l i k e B r a y 's , fa v o red d if f u s io n over c o n ta c t exch an ge, At about t h i s same tim e , Husted and Low (1954) p u b lish ed r e s u l t s which a l s o in d ic a te d th a t io n movement was dependent b n .th e s o lu t io n p h a se, and d eriv ed a s o lu t io n fo r s o i l io n t r a n s f e r w hich fo llo w e d P ic k 's d if f u s io n la w s. Perhaps th e m ost c o n v in c in g d a ta to d i s p e l . t h e c o n ta c t exchange th eory was p rovid ed by O lsen and Peech (1960) who measured p la n t uptake a t Rb+ . and Cat+ from b o th th e su sp e n sio n and:e q u ilib r iu m d ia ly z a t e . A lthough th ey v a r ie d th e r e la t iv e : c o n c e n t r a t io n s in th e p h ases to ex trem es; th e ^ r a t e o f Rbt and Ca"*"*" uptake from b oth p h a ses was th e same, A d i f f e r e n t p r o c e s s th a t has b een e n v is io n e d a s a l s o c o n tr ib u tin g & 6 v. to io n uptake i s i n i t i a t e d b y . th e a c i d i f y in g a c t io n o f p la n t r o o t s . It \ was p o s tu la t e d th a t th e s o lu t io n a c t i v i t y n ear th e r o o t was enhanced above th a t measured in s o i l , e x t r a c t s . CO2 , H^CO^ may be form ed, For exam ple, a s th e r o o ts e x c r e te Or i f H+ io n s a re e x c r e te d to p r e s e r v e e l e c t ­ r i c a l n e u t r a li t y ( in c a se more c a t io n s a re absorbed than a n io n s ) , the , s o i l s o lu t io n pH would d e c r e a se . q u e n t ia l a c t i v i t y d if f e r e n c e s , A pH d e c r e a se would p ro v id e co n se­ From Donnan e q u i l i b r i a i t can be c a lc u la t e d th a t a pH d e c r e a se o f o n e .u n it would in c r e a s e th e s o lu t io n p o ta ssiu m by a f a c t o r / 1 0 , w h ile th e ca lciu m would in c r e a s e by a f a c t o r <. o f 3Z 10. Nye (1968) has argued th a t perhaps j u s t th e r e v e r s e s i t u a t io n , may exist? He sta te s "It i s widely ,believed that roots make nutrients more a v a ila b le by ren d erin g t h e ir environm ent more a c id ." By u sin g th e d a ta o f Cunningham (1 9 6 4 ), where 62 common p la n t s p e c ie s were s tu d ie d , he reason ed t h a t , on th e a v e r a g e , more a n io n s than c a t io n s were taken up from th e s o i l - when c o u n tin g n itr o g e n uptake a s NO" r a th e r than NH^. Nye sp e c u la te d from th e s e d a ta th a t r o o t s e x c r e t e HCOg (n o t H+) , which a ten d s to r a i s e th e p H .• As an in d ic a t io n o f t h i s , he p o in te d out th a t i t \ . i s normal fo r p la n t s grow ing in n u t r ie n t m edia to in c r e a s e th e pH v a lu e when th e n itr o g e n i s a p p lie d a s NO » v B ecause o f th e d i f f i c u l t i e s ' / 3 r I . en cou n tered in m easuring a c t u a l pH changes near r o o t , s p e c u la t io n o n ly (. ’ . ■ has. dom inated. . T h erefo r e, i t must be, con clud ed th a t t h i s typ e o f 1 ■ e x p lo r a tio n i s in c o n c lu s iv e and more s p e c i f i c e v id e n c e . i s need ed . Coupled w ith t h i s need i s a l s o a need fo r d eterm in in g more about th e e x a c t n a tu re o f th e s e v e r a l com plexing a g e n ts th a t a p la n t may •1 ' 7 e x c r e te . To stu d y th e e f f e c t s , E lgaw hary:e t a l (1970b) used a simu­ la t e d r o o t made o f porous c er a m ic: tu b in g which th ey embedded in the s o il. Complexing m a te r ia ls were mixed w ith w a ter and p a ssed through t h i s "root" w hich a c te d a s a s in k fo r i o n s . . EDTA9 a t IO- 3 M concen­ t r a t io n , in c r e a se d z in c uptake by a f a c t o r o f 17 o v e r .w a te r a lo n e . Other m a te r ia ls in c r e a se d z in c uptake l e s s , b u t were s t i l l h ig h ly e ffe c tiv e . As to th e a c t u a l m a te r ia ls e x c r e te d by p la n t r o o t s , R ovira (1962) was a b le t o i s o l a t e o n ly sm a ll amounts o f c h e la t in g a n io n s as c i t r a t e and l a c t a t e from w heat r o o t s . Thus i t was concluded by Hale e t a l (1 9 7 1 ), b eca u se o f la c k o f c o n c lu s iv e evidence^ th a t th e impI i car-' tio n s in m in era l n u t r it io n o f p la n t s a re unknown,■ From th e p r e v io u s l i t e r a t u r e c i t e d h e r e in i t has been p o in ted ou t th a t mechanisms such a s c o n ta c t exch an ge, a c i d i f y in g a c t io n o f r o o t s , or t h e ir com plexing ex u d a tes have f a i l e d to e x p la in th e la r g e d i f f e r ­ e n c e s betw een s o i l s o lu t io n " co n cen tration and p la n t uptake by mass flo w . E vid en ce p o in t in g toward d if f u s io n i s more c o n c lu s iv e , a s w i l l be shown. ■ The f i r s t work in s o i l io n d if f u s io n d id n o t r e l a t e to th e p la n t r o o t r o l e in th e p r o c e s s . Emphasis was p la c e d .o n d if f u s i o n o f f e r t i l i z e r m a te r ia ls once th ey had been added to th e s o i l , or to th e t h e o r e t i c a l b a s is o f s o i l d if f u s io n i t s e l f . I n i t i a l w orkers in th e s e s t u d ie s in c lu d e d Chernov (1 9 3 9 ), Brown (1 9 5 4 ), Husted and Low (1 9 5 4 ), K lute and L etey (1958) and M arsh all (1 9 5 8 ), However, in th e e a r ly 1960*s B o u ld in . (1961) and O lsen e t a i'( 1 9 6 2 ) i n i t i a l l y proposed th e im portance o f d i f f u s i o n fo r tr a n s p o r tin g io n s to p la n t r o o t s . ' In t h e ir p u b lic a t io n s - - I ' ' ' , I, , . / . . : ■ Z ' , l ' \ \ I 1 -• - i I . 1 .1 * - I ‘ " . . . 8 i t was p o in ted o u t th a t th e r o o t must red u ce th e s o lu t io n c o n c e n tr a tio n o f io n s a t th e r o o t - s o i l boundary an d . th ey so lv e d m ath em atical m odels in d ic a t in g th e e x t e n t . A q u it e c o n v in c in g p o r tr a y a l o f th e r o o t s in k - d i f f u s i v e flo w mechanism was p ro v id ed about t h is same tim e by Barber (1962) w ith a u to ra d io g ra p h s. He used a tech n iq u e o f growing p la n ts in s o i l s la b e le d w ith a r a d io a c t iv e is o t o p e . X -ray f ilm was p la ce d c l o s e I to th e a c t i v e r o o t s so th a t th e d ev elo p ed f ilm would d e p ic t th e is o t o p e d is t r ib u t io n about them. U sing t h i s m ethod, Barber la b e le d a s o i l w ith a sm a ll amount o f Rb- 8 6 . The r e s u lt i n g a u to ra d io g ra p h s showed th a t th e r e was d e p le t io n o f t h i s m a te r ia l in th e r o o t v i c i n i t y a s s o c ia t e d with plant uptake. As time of uptake progressed, the s o i l zone of d e p le t io n w idened. To tr y to en su re th a t th e d e p le t io n was n o t a s s o c i­ a te d w ith a s o i l w ater g r a d ie n t in th e r o o t a r e a , th e p la n t s were w atered d a i l y . In an oth er p o r tio n o f t h i s g e n e r a l stu d y he a p p lie d e x c e s s ( t o p la n t uptake) S r-9 0 to an agar r o o t m edia, grew p la n t s , and added H oagland1s s o lu t io n afe a so u rce o f n u t r ie n t s . In t h i s system the is o t o p e i n i t i a l l y c o l le c t e d around th e r o o ts by mass f lo w . 1 A fte r the r o o t s were c a r e f u l ly p u lle d ou t o f th e agar th e S r-90 d if f u s e d away from th e p r e v io u s area o f c o n c e n tr a tio n . T h erefo r e, i t was ev id en ced th a t a r o o t was ca p a b le o f in d u cin g a c o n c e n tr a tio n g r a d ie n t, e it h e r by red u cin g or by in c r e a s in g th e n e a r -r o o t io n c o n c e n tr a tio n . From th e n , d if f u s io n became a cce p te d a s an im p ortan t mechanism fo r .. ' V p la n t n u t r it io n ,- and th e i n i t i a l s o i l d if f u s io n s t u d ie s took on new ,f 1 r ' im portance as- th ey ./h elp ed 1t o .d e p ic t th e b a s ic p r o c e s s . / -O Vl . 9 As y e t , t h i s d is c u s s io n has been d ev o ted to th e way th a t s o i l d i f f u s i o n became e s t a b lis h e d r a th e r than to t h e . t h e o r e t i c a l developm ent o f th e p r o c e s s i t s e l f . As d if f u s io n o f io n s in s o i l encom passes a broad f i e l d , th e r e w i l l be em phasis p la ced on th e sco p e o f th e h y p o th e sis and ex p erim en ta l work to be g iv e n h e r e in . Where io n or m atter tr a n s p o r t r e s u l t s from Brownian m otion i t i s termed d if f u s i o n . Brownian m otion i s random, so i f a c o n c e n tr a tio n g r a d ie n t i n i t i a l l y e x i s t s th e m otion r e s u l t s in red u cin g th e g r a d ie n t w hich in turn r e s u l t s in a n e t t r a n s f e r o f m atter to th e r e g io n o f i n i t i a l l y low er c o n c e n tr a tio n . To some, th e a c t u a l n e t tr a n s fe r sh ou ld e x i s t b e fo r e th e term d if f u s io n may be im p lie d . Even s o , many s o i l s exp erim en ts have invoked th e i n i t i a l c o n d itio n th a t one zone o f a s o i l c o n ta in e d la b e le d m a te r ia l added w h ile th e a d ja cen t zone had an eq u a l amount o f n o n la b eled m a t e r ia l. The t r a n s f e r o f la b e le d and n o n la b eled m a te r ia l in t o each o t h e r ’ s zone has been stu d ie d and i s termed d if f u s io n , alth ou gh th e r e was no n e t tr a n sfe r , o f th e g e n e r a l io n , P ic k ’ s f i r s t . l a w d e s c r ib e s th e d if f u s io n p r o c e ss fo r a ste a d y s t a t e c o n d it io n , and a s amended fo r a s o i l an ion i s - J =' -D I6(dC /dx) (I) where J = th e f lu x o f su b sta n c e c r o s s in g a s o i l u n it a rea p e r p e n d ic u la r to flo w d ir e c t io n p er tim e, ■ (meq, grams. , , , ) (cm- ^) (sec"7"*-) 0 = th e v o lu m e tr ic s o i l w ater c o n te n t (d im e n s io n le s s ) i., . ■ - ' . ■ . . " . , : .' i .. C =• s o i l s o lu t io n c o n c e n tr a tio n (meg, grams . •. ) (cm"3) x = sp a ce v a r ia b le (cm) D = d if f u s io n c o e f f i c i e n t (cm^) ( s e c I = im pedence. f a c t o r , d u e .to s o i l p a r t i c l e s in t e r f e r in g w ith : aqueous d if f u s io n (d im e n s io n le s s ) There i s some am b igu ity r eg a r d in g term s in th e l i t e r a t u r e . Concen­ t r a t io n has som etim es been used to d en o te th e am ount.per volume o f s o i l , in e f f e c t com bitiing C and 6; s o lu t io n c o n te n t. As j u s t shown, C w i l l alw ays r e f e r to By u se o f th e denoted terms combined w ith D in e q u a tio n ( I ) , J w i l l r e f e r to a u n it area o f s o i l . "I" in c lu d e s a com b in ation o f im pedence f a c t o r s w hich a re t o r t u o s i t y , reduced f l u i d i t y and e l e c t r o s t a t i c r e p u ls io n fo r a n io n s (o r , in th e c a s e o f c a t io n s , n e g a tiv e a d s o r p tio n ). These th ree f a c t o r s th a t p ro v id e th e o v e r a ll im pedence term a r e i ( in th eo ry ) m u lt ip lie d by each o th er to d eterm ine ' r ' th e impedence v a l i / e . - However, in p r a c t ic e i t has been n e c e s s a r y to measure t o t a l im pedence, then se p a r a te v a lu e s o f th e c o n tr ib u tin g f a c t o r s - u s u a lly by assum ing v a lu e s o f a t l e a s t one o f th e f a c t o r s . ' The v a lu e s o f ”1" (e x c e p t p o s s ib ly fo r H+ ) w i l l b e v le s s than I (which i s th e v a lu e o f an aqueous s o lu t io n a lo n e where 0 = I ) . D are l i t e r a t u r e v a lu e s fo r d i l u t e aqueous s o lu t io n s . The v a lu e s o f I t may be n oted th a t some p u b lic a t io n s have r e fe r r e d to a d if f u s io n c o e f f i c i e n t . f o r s o ils (o r D a s an e f f e c t i v e d if f u s io n c o e f f i c i e n t ) w hich was a co m b in -' e , a t i o n o f ( D )(I ) or (D )(I)(O ) in com parison to eq u a tio n ( I ) . The u s e .o f a t o r t u o s it y f a c t o r , , acknowledged from th e o i l in d u str y 11 l i t e r a t u r e by P o rte r e t a l (1 9 6 0 ), in c o r p o r a te s th e in c r e a se d path le n g th an io n must t r a v e l to reach i t s f i n a l d e s t in a t io n w ith the reduced p ath area in w hich to t r a v e l . p ro p o se, th e s e two f a c t o r s a re r e l a t e d . As can be shown by th e model they T h e r e fo r e , th e t o r t u o s it y f a c to r th ey d e s c r ib e i s (L/L )^ . L sta n d s fo r th e e f f e c t i v e d is ta n c e an 1 6 io n t r a v e ls w h ile d en o tes th e t o t a l d is t a n c e i t t r a v e ls in i t s ■ to r tu o u s p a th . ' T his f a c t o r i s dependent on w ater c o n te n t, s o lu t io n f i s c o s i t y and i o n i c - c l a y i n t e r a c t io n s . are n o t in d ep en d en t o f each o th e r . F u rth er, th e s e o th e r f a c t o r s ' For exam ple, red u cin g th e w ater c o n te n t in c r e a s e s th e a v era g e s o lu t io n v i s c o s i t y (a s th e s o lu t io n i s more viscous near surfaces) and causes diffusion to take place in r e g io n s c l o s e r to c la y p a r t i c l e s where th ey become s u b j e c t to e l e c t r i c a l fo rce s. S in c e an an ion i s r e p e lle d away, from th e c la y ch a rg e, i t does . n o t e x p e r ie n c e as much in f lu e n c e from in c r e a se d v i s c o s i t y as a c a t io n , b u t i t does e x p e r ie n c e th e e f f e c t i v e pathway red u c tio n to a g r e a te r e x te n t. With c h lo r id e , w hich i s n o t a p p r e c ia b ly ad sorb ed , P o r te r e t a l . (1960) found t h a t th e p rod u ct o f th e t o r t u o s it y tim es reduced f l u i d i t y , tim es e l e c t r o s t a t i c r e p u ls io n was l i n e a r l y r e la t e d to v o lu m e tr ic w ater ■ c o n te n t. The p rod u ct term had v a lu e s e x t r a p o la t in g to 0 when 0. was reduced to near 15 atm osp h eres. R o w ell e t a l (1967) o b ta in ed very s im ila r r e s u l t s to th o se o f .P o r t e r e t a l and denoted th e s i m i l a r i t y in 1 . 1 . t h e i r w r it in g s by p l o t t i n g b o th s e t s o f d a ta on one graph.' ■ ' A f u n c t io n a l r e la t io n s h ip th a t was d eriv ed by Kemper and van Sch aik (1966) i s . Die = Daeb0 (2) A • . ■• T I J• . • > , I1 t ii* 1X ' i .i i " I . ' . i n - ' ! i. 'i . - x: . i-i i i ' , v ; ■! 11; ' I . , 11 • ' ' • ii ' . : i ; . ' x ___ ; i 12 where "a" and "b” a r e e m p ir ic a l c o n s ta n ts w ith "a" b e in g r e la t e d to the s u r fa c e a rea o f th e s o i l s t u d ie d . O lsen and Kemper (1968) l a t e r con­ clu d ed t h a t , fo r th e o v e r a l l work done, th e r e was r e a so n a b le agreem ent, when "b" was e q u a l to 10 and "a" ranged from 0 .0 0 5 to 0 .0 0 1 f o r sandy loam to c la y s o i l s . When phosphorus d if f u s io n was measured under s e v e r a l w a ter con­ t e n t s , Mahtab e t a l (1971) found a f a i r l y lin e a r r e l a t io n s h ip betw een w ater c o n te n t and impedance v a lu e s as o th e r s had w ith c h lo r id e . However, O lsen e t a l (1965) and a l s o R ow ell e t a l (1967) found more cu rv a tu re in th e form o f a h y p e r b o lic f u n c t io n , O lsen e t a l a t t r ib u ­ ted th e d if f e r e n c e betw een phosphate and c h lo r id e to a d so r p tio n o f th e 1 p h o sp h a te. That i s , a s th e s o lu t io n phosphate i s adsorbed a t low ered w ater c o n t e n t s , i t s t o t a l s o lu t io n c o n c e n tr a tio n per volume o f s o i l becomes l e s s . In .co m p a riso n , th e t o t a l c h lo r id e c o n c e n tr a tio n per volume rem ained th e same. Low (1962) has rep o rte d th a t w a ter ta k e s on " q u a s i- c r y s t a llin e " p r o p e r tie s a t c l o s e p r o x im it ie s to c la y s u r f a c e s . These reduced m o b ility e f f e c t s were measured by Kemper e t a l (1964) and th e f lu id i t y , found to be 0 .0 5 (a s compared to I fo r norm al w ater) in th e f i r s t la y e r o f a C a -cla y and 0 .0 3 on a N a-c la y . The m o b ility in c r e a se d r a p id ly by th e th ir d w ater la y e r b u t w a s. s t i l l a f f e c t e d at.40& from th e c la y . For c a tio n s ,' Bear (1964) d e p ic t s th a t th e d is t r ib u t io n o f io n s ■ r from a c la y s u r fa c e f o llo w s th e p r o p o sa l o f S te m in 1923 fo r a d ou b le la y e r . The d is t r ib u t io n i s r e l a t i v e to th e io n ic dim ension o f th e io n , 13 in a d d itio n to th e f o llo w in g th e e a r l i e r p r o p o sa ls o f Gouy and Chapman, and H elm h o ltz. A djacen t to th e c la y a la y e r o f c a tio n s (S te r n la y e r ) i s c o n cen tra ted and th e r e th ey r a r e ly exchange p o s i t i o n s . N ext to th e S tern la y e r a l e s s t i g h t l y h e ld and co n c e n tr a te d la y e r e x i s t s where th e c a tio n s a re termed ex ch a n g ea b le . s o lu t io n . Away from t h is la y e r i s th e b ulk In com parison to th e s te a d y s t a t e eq u a tio n g iv e n f o r a n ion s (e q u a tio n I ) „ O lsen and Kemper (1968) show th a t w ith c a t io n s th e r e i s a ' c o n tr ib u tio n from s o l u t i o n , and ■ jCfrom, solution) ^ ‘ (™C/RT) dS/dx CS) where E s the gas constant T = a b s o lu te tem perature dp/dx = th e d r iv in g f o r c e , where p = pq + RT In a + zFi|), and a • is a c t i v i t y , z i s v a la n c e , F i s Faraday, and i s th e phase e le c t r ic p o te n tia l. Other n o t a t io n i s th e same as used f o r eq u a tio n ( I ) . The s o i l s u sp e n sio n d r iv in g f o r c e , d y /d x , has been c o n t r o v e r s ia l. W hile i t has been argued th a t th e g r a d ie n t in th e ch em ica l p o t e n t ia l ( c a ll e d the, d a/d x th e o r y ) d e p ic t s th e d r iv in g f o r c e , Khasawneh (1 9 7 1 ), in r e v ie w , s t a t e s th a t th e more r e c e n t body o f e v id e n c e su p p o rts th e d y/d x (e le c tr o c h e m ic a l p o t e n t ia l) th eo ry as argued by F rere and A xley I (1964) ,* L agerw erff (1960) and O lsen (1 9 6 8 ). With c a t io n s , R ow ell e t a l (1967) and P a t e l e t a l (1963) found n e a r ly th e same h y p e r b o lic curve r e l a t i n g impedance f a c t o r s to v o lu m e tr ic w ater c o n te n t a s .was found by most w orkers w ith phosphorus. The r e l a t i v e c o n tr ib u tio n to d if f u s io n w ith in th e adsorbed phase has been co n sid ered to be minor fo r stro n tiu m and sodium by R ow ell e t a l (1967) minor fo r sodium b y.M ott and Nye (1968) and minor fo r calciu m by van S ch aik e t a l ■(1 9 6 6 ). . These l a t t e r a u th o rs found th a t sodium was '• la r g e ly r e g u la te d by d if f u s io n in th e adsorbed ph ase on a N a -c la y , E l l i s e t a l (1 9 6 9 ), from u sin g e q u a tio n s th ey d ev elo p ed , con clud ed th a t Mott, and N ye’ s (1968) f in d in g s c o in c id e d w ith t h e ir developm en t. Con­ v e r s e l y , Elgawhary e t a l (1972) and B ole and Barber (1 9 7 1 ), w ith p la n t uptake s t u d ie s w ith ca lciu m and. s tr o n tiu m , con clud ed th a t w ith d if f u s io n o f th e s e i o n s , th ey w ere th e p o r tio n b a la n ced by n e g a tiv e c la y ch a rg es. By u sin g th e e x p r e s s io n d ev elo p ed by E l l i s , e t a l (1 9 6 9 ), P h i l l i p s e t a l (1972) p roposed th a t when o n ly a sm a ll f r a c t i o n o f th e s o i l c a tio n exchange, c a p a c ity i s f i l l e d w ith an io n in q u e s tio n ,1 i t w i l l tend to d iffu se primarily in the adsorbed phase. Thus they calculated th a t copper and presum ably manganese and z in c w i l l d if f u s e in th e adsorbed p h a se , . . 1 As t r a n s ie n t c o n d itio n s are more common in s o i l s - than s te a d y s t a t e , ' e q u a tio n s fo r th e s e w i l l be g iv e n . Some s im p lif i c a t io n w i l l be made to cop e w ith problem s found in l e s s than i d e a l s i t u a t i o n s , as in . s o i l s , b u t \ no more than i s u s u a lly found in th e l i t e r a t u r e . For exam ple. Low (1962) • . . has d is c u s s e d th a t b oth c o - d if f u s io n ( a ls o term ed. s a l t d if f u s io n ) and c o u n t e r - d if f u s io n a re assumed to be o p e r a tiv e in s o i l - p l a n t sy ste m s. C o -d iffu s io n i s th e p r o c e s s w hereby, in o rd er to m a in ta in e l e c t r i c a l / / 15 n e u t r a l i t y , an a n ion and c a t io n move in th e same d ir e c t io n . For coun­ t e r - d i f f u s i o n , e l e c t r i c a l n e u t r a li t y i s m ain tain ed by io n s o f l i k e . ch arge t r a v e lin g in o p p o s ite d i r e c t i o n s . The g e n e r a l eq u a tio n fo r t r a n s ie n t c o n d itio n d i f f u s i o n ( P ic k 's secon d law) can be d eriv ed by u se o f P ic k 's f i r s t law fo r an an ion and th e eq u a tio n fo r c o n t in u it y 9C /9 t = DK32C/9 x 2) (4) A nother way o f e x p r e s s in g t h is i s by m u ltip ly in g by 0 , and 9M /9t;= D 0I(92C/9 x 2) (5) where M i s th e q u a n tity d if f u s in g per u n it volume o f s o i l . Gardner (1965) has g iv e n a u s e f u l a n a ly t ic a l s o lu t io n fo r eq u a tio n (5) fo r p lan ar d if f u s io n in a s e m i - i n f i n i t e sy stem . They were d e r iv e d by assum ing th a t th e i n i t i a l c o n c e n tr a tio n in th e s o i l i s u n iform , b u t a f t e r tim e zero th e boundary i s m a in ta in ed a t a new c o n c e n tr a tio n , or C = Cq , t = 0 , x> 0 (6) C = Cr , t >0, x = 0 (7) where C i s th e o r i g i n a l s o i l s o lu t io n c o n c e n tr a tio n , and C i s th e o ■ ■■ . r■ boundary (a s r o o t .or o th e r s in k ) c o n c e n tr a tio n . c o n d itio n s , Then, s u b j e c t to th e s e X . (C-Cr )/C 0-Cr ) = . e r f [X Z (Z )(D It)1 / 2 ] ■ . ( 8 ) w hich d e p ic t s th e s o lu t io n c o n c e n tr a tio n w ith v a ry in g t and x . The r a t e : o f d if f u s i o n in t o th e s in k i s D I( d C /d x )^ o= (C0-Cr ) D I/(irD It) i i ' 1 /2 (9) 16 I n te g r a t io n to show th e q u a n tity o f m a te r ia l d if f u s e d per u n it a rea ■' u n t i l tim e p •t shows 1 /2 1 /2 M f t= 2 ( Co“ c r ) (DIGt) ' /H (10) where M = th e q u a n tity p er -u n it s u r fa c e a rea o f s o i l p er tim e. E quation (10) has been used by N y e 'and co-w orkers- (1966b) fo r d if f u s io n ■. o f b o th c a t io n s and a n io n s , and a v e r s io n o f i t was used by Warnche and Barber (1972)„ In th e s e e q u a tio n s th e d if f u s io n c o e f f i c i e n t , D, was taken to be c o n s ta n t. I t i s known to vary w ith c o n c e n tr a tio n , b u t n o t a p p recia b ly u n t i l c o n c e n tr a tio n s become la r g e r than a re.n o rm a lly found in s o i l so lu tio n s. For example, Kemper and van Sehalk sta te that a constant d if f u s i o n c o e f f i c i e n t " w i ll be s u f f i c i e n t l y a ccu ra te f o r m ost p r a c t ic a l, a p p lic a t io n s " . I f o n ly two io n s were in v o lv e d in a d if f u s io n .p r o c e s s in s o i l ( f o r c o - d if f u s io n or c o u n t e r - d if f u s io n ) a w e ig h tin g method to o b ta in a m utual d i f f u s i o n c o e f f i c i e n t co u ld be used a s shown by Low (1 9 6 2 ). A lthough t h i s method cannot be a p p lie d to more com plex system s where th e e x a c t a c t io n s o f th e many io n s a re unknown, i t d oes p ro v id e i n s i g h t in t o th e g e n e r a l n a tu re o f th e d if f u s io n p r o c e s s . is : . The eq u a tio n , D12 = D1D2 (Z1C1 t Z2C2) / (D1Z1C1 + D^z2C2) (11) when D1 2 i s th e m utual d if f u s io n c o e f f i c i e n t , C i s th e io n c o n c e n tr a tio n , / z i s th e v a le n c e o f th e io n , and th e s u b s c r ip t s I and 2 r e f e r to the two r e s p e c t iv e io n s . From t h i s eq u a tio n i t may be seen th a t th e v a lu e o f D ^ i s betw een D1 and Dg, and th a t th e io n p r e s e n t in low c o n c e n tr a tio n . . ' . . ■ r ■ 17 w i l l la r g e ly c o n t r o l.D ^ . . Nye (1966a) has proposed th a t in d if f u s io n to a zero s in k , th e a p p ro p ria te average d if f u s i o n c o e f f i c i e n t i s the s e l f - d i f f u s i o n c o e f f i c i e n t , such as would be o b ta in ed from m easuring th e r a t e th a t a la b e le d io n d if f u s e s co u n ter to an i d e n t i c a l u n la b eled • io n . F u r th e r , he b e lie v e d th a t io n s p r e s e n t in sm a ll c o n c e n tr a tio n s . may be assumed to be moving in d ep en d en tly w ith t h e ir own d if f u s io n c o e f f i c i e n t s , b e in g l i t t l e a f f e c t e d by o th er macrocomponents in th e system . , A method o f d eterm in in g th e c o n t r ib u t io n from adsorbed io n s to ' d i f f u s i v e f l u x , where they entey in t o a simultaneous r e v e r s ib le r e a c t io n . with the solu tion phase, was f ir s t proposed by Olsen et a l (1962) in 1962. The s o l i d p lu s s o lu t io n phase c o n tr ib u tio n fo r t h i s r e a c t io n comes from th e d i f f e r e n t i a l eq u a tio n (9 C /d t)0 + ( 3 S /9 t ) = DIG(9 2C/3 x 2) (12) where S i s th e q u a n tity o f io n per u n it volume o f s o i l e n te r in g in t o th e d if f u s i o n p r o c e s s . I f th e iso th erm betw een adsorbed and s o lu t io n phase i s l i n e a r S = RGC + c o n s ta n t (13) i . , ' where R i s th e r a t i o o f io n s in th e adsorbed phase to th o s e in the j s o lu t io n p h a se , per u n it volume o f s o i l . A new eq u a tio n may be w r itte n . ' by com bining e q u a tio n s (12) and (13) . 9C /3.t'= .[ D l/ ( R + l) ] ( 9 2C /3x2) , (14) The (R fl) term d e p ic t s th e s lo p e o f th e iso th erm fo r th e r a t i o o f the (adsorbed + s o lu t io n p h ase) t o th e s o l u t i o n , o n ly , p h a se. I t i s what 18 O lsen e t a l (1962) term ed a " c a p a c ity f a c t o r " . D / (Rl-I) i s a n a lo g o u s to th e rm a l d i f f u s i v i t y . In h e a t flo w e q u a t io n s , When in c lu d in g th e c a p a c i t y f a c t o r ( R + l) , e q u a tio n s (8) (9) and (10) becom e, r e s p e c t i v e l y C" Cr /C o~Cr = e r f { tx ( R + l) 1 / 2 ] / 2 ( D I t ) 1Z2 } (15) D I(d C /d x )x=0 = (Co-C r ) B I / [ ( r D I t ) / ( R + l ) ] 1 /2 (16) Mt = '2 (C0-C r ) [D I0 t (R +l) J1 Z2Zrr1 / 2 (17) I t may be n o te d t h a t , f r 0 m th e a d s o rb e d p o o l, th e c o n t r i b u t i o n to th e d i f f u s i o n p r o c e s s i s enhanced by th e c a p a c ity f a c t o r o v er t h a t o f n o t h a v in g th e a d so rb e d m a t e r i a l - b u t o n ly when r e l a t i n g C a s th e • s o lu tio n c o n c e n tr a ti o n a s done h e r e . In th e l i t e r a t u r e o f Nye and co­ w o rk e rs (1966b) and o t h e r s who ta k e th e c o n c e n tr a ti o n term to e q u a l th e t o t a l d i f f u s i b l e c o n c e n tr a ti o n p e r u n i t volum e o f s o i l , th e y use term s t h a t d e p i c t t h a t th e d i f f u s i o n p r o c e s s i s red u ce d by th e a d s o r p ti o n o f io n s . G ard n er (1972) h as d e r iv e d th e e q u a tio n s o f Nye e t a l i n term s u sed h e r e i n and- shown them to be i d e n t i c a l , and v a r y in g o n ly i n how i n d i v i d u a l s p r e f e r to w ork w ith them. When th e a d s o r p ti o n is o th e r m i s n o t l i n e a r , a s shown i n e q u a tio n (1 3 ) , f i n i t e d i f f e r e n c e m ethods a r e n e c e s s a r y to s o lv e th e c o n t r i b u t i o n o f b o th so rb e d and s o l u t i o n p h a s e s . ■ im p o rtan t c o n s i d e r a t i o n . T h is a s p e c t , th e n , becom es an O lsen e t a l (1962) found th e am ount o f P t h a t u n d erw en t i s o t o p i c d i l u t i o n w ith P-32 i n a 2 4 -h o u r r e a c t i o n was l i n e a r th ro u g h o u t th e im p o r ta n t ra n g e o f c o n c e n tr a ti o n . c a p a c it y f a c t o r ( s lo p e o f R +l) was a c o n s t a n t . T h e r e f o r e , th e As more f e r t i l i z e r P was added th e s lo p e o f (R+l) d e c re a s e d ta k in g th e form o f a F r e u n d lic h 19 iso th e r m . A ls o , i t was thought th a t th e s lo p e o f th e iso th erm would be more v a r ia b le fo r a c id s o i l s w ith t h e ir g r e a te r an ion a d so r p tio n capa­ c ity , Nye (1966) has in d ic a t e d th a t th e a p p ro p ria te m easure o f t h e • c a p a c ity f a c t o r i s a s t r a ig h t l i n e p a s s in g from th e p o in t (x=C0 , y = . t o t a l d i f f u s i b l e c o n c e n t r a t i o n ) , t o th e o r ig in in th e c a s e th a t th e / ^ iso th erm d is p la y s some cu r v a tu r e . With boron, a s w ith p h osp h oru s, th e iso th erm has been found to be lin e a r ov er low c o n c e n tr a tio n s by B igger ' and Fireman (1 9 6 0 ), K in gston (1 9 6 4 ), Okazaki and Chao (1 9 6 8 , and Sulaiman and Kay (1 9 7 2 ), b u t f o llo w in g a F re u n d lich or Langmuir iso th erm a t h ig h - ■ er c o n c e n t r a t io n s . These a u th o rs have n o t agreed on a d so r p tio n and. d e so r p tio n c h a r a c t e r i s t i c s . But t h i s m ight be ex p ected when c o n s id e r in g th a t boron may; in a d d itio n to b ein g sorbed or. form ing co m p lex es, e n te r in t o th e c la y l a t t i c e or p r e c i p it a t e w ith s e s q u io x id e s , a s was found b y; Sims and Bingham (1^ 67, 1 9 6 8 ). With c a t io n s , V aidyanathan e t a l (1968) found c e r t a in s o i l s had f a i r l y lin e a r s o r p tio n iso th erm s fo r K. B rew ster and T inker (1970) found th a t most o f th e K iso th erm was l i n e a r , -b u t s im ila r to B e c k e t t 's fin d ­ in g s (1 9 6 4 ), th e r e were m in era l s o r p tio n s i t e s p a r t ic u la r to K o n ly w hich were o p e r a tiv e a t a very low K s t a t u s ,' Thus, a la r g e r r a t io o f K i s sorbed a t low c o n c e n tr a tio n s as compared to th e r a t i o found a t in t e r ­ m ed iate or h ig h er t o t a l c o n c e n tr a tio n s . From Brew ster and T in k e r 's ex­ perim ent (1970) Na and Mg had lin e a r is o th e r m s . They s t a t e , though, „ th a t a s Ca i s th e major s o i l io n , th e a s p e c t .o f in c r e a s in g th e Ca . .sorb ed phase w ith, in c r e a se d s o lu t io n ph ase c o n c e n tr a tio n would n o t be 20 . / . / I f I p o s s i b l e , e x c e p t w ith v ery lim it e d s o lu t io n ch an ges. have a lin e a r iso th erm by Elgawhary e t a l (1 9 7 0 a ). Z inc was found to With ir o n , O’Connor e t a l (1971) found th a t th e s lo p e o f th e iso th erm in c r e a s e d w ith one month’s tim e (from 1000 to 5 0 0 0 ), and th e r e fo r e in s te a d o f term ing the s lo p e a ." c a p a c ity f a c to r " , s t a t e d th a t i t sh ou ld be used a s a " co rrec­ t io n fa c t o r " . The in c r e a s e in th e s lo p e was a s s o c ia t e d w ith grad u al p r e c i p it a t io n o f added ir o n a s amorphous ir o n o x id e s , Nye (1966) p o in te d ou t t h a t , to a v o id h y s t e r e s is p rob lem s, the iso th erm s sh o u ld be determ ined under th e same c o n d itio n s a s d if f u s io n i s •to o c c u r , in d ic a t in g th a t i f d i f f u s i o n to a s in k were to be s tu d ie d , a d e s o r p tio n i s Ofhermiwould be p r e fe r r e d to an, a d so r p tio n is o t h e r m ,■ The p roced u res used in d e so r b in g s o i l m a te r ia ls have u s u a lly c o n s is te d o f s e q u e n t ia lly e x t r a c t in g p o r tio n s o f th e io n s and m easuring them to ­ g e th e r w ith new ly o b ta in ed e q u ilib r iu m s o i l s o lu t io n c o n c e n tr a tio n . C o n v e rsely , B ar-Y osef e t a l (1972) p o in ted out th a t th e h y s t e r e s is , phenomena in th e a d s o r p tio n -d e s o r p tio n p r o c e s s w ith phosphorus a r i s e s d u rin g d e s o r p tio n from d r a s t i c a l l y red u cin g the P c o n c e n tr a tio n . /^ B ecause o f t h i s , th e r e i s d i s s o l u t i o n o f s i l i c a and an a l t e r i n g o f th e 1 a v a il a b l e P a d so r p tio n s i t e s on th e c l a y . Thus, w ith th e s e opposing v iew s and q u e s tio n a b le u n d ersta n d in g o f h y s t e r e s i s , i t ap p ears th a t c o n c lu s io n s a t p r e s e n t would be prem ature. As an o v e r a l l c o n s id e r a tio n ab ou t th e b u ffe r c a p a c ity term , when i t i s o b ta in ed from 'an iso th erm , i t i s an approxim ation^ v a r y in g in e x a c t­ n e s s o f a p p lic a t io n among s o i l s , ,.and w ith io n ty p e .and c o n c e n tr a tio n 21 w ith in a s o i l . Even w it h th e s e draw backs, how ever, t h i s f a c to r quant­ i t y has p ro v id ed c o n s id e r a b le needed r e s o lu t io n o f q u a n t it a t iv e , d i f f ­ u sio n p r o c e s s . In /r e g a r d to o th er f a c t o r s c o n tr ib u tin g to d if f u s io n r e g u la t io n , O lsen and Kemper (1968) have s t a t e d "While th e osm otic movement and e l e c t r i c a l p o t e n t ia l in c r e a se d by s a l t g r a d ie n ts are in t r i g u i n g , they I change th e s a l t d i f f u s i o n c o e f f i c i e n t s o n ly s l i g h t l y th e s e item s w i l l n o t .b e d e t a il e d h e r e . T h erefo re, I o n -p a ir fo rm a tio n i s s t i l l an oth er f a c t o r th a t d e s e r v e s m en tion , b u t f a l l s in t o t h i s same c a te g o r y . Ion exchange r e s in s have been used in d if f u s io n s t u d ie s b ecau se o f their a b ility to reduce a s o i l ion concentration a t a s o i l - r e s i n ■I n te r ­ fa c e . V aidyanathan and Nye ( 1 9 6 6 ) ,: used b oth c a t io n and an ion exchange r e s in s in paper s t r i p s a s s in k s fo r p la n a r d if f u s i o n s t u d ie s and o u t lin e methods o f d eterm in in g a ccu m u la tiv e f l u x . ' They d id n o t compute a c a p a c ity f a c t o r , b u t o b ta in ed o v e r a l l . p o t e n t i a l s fo r s o i l s to c o n tr ib u te to d i f f u s i v e f lu x . T his tech n iq u e was a ls o used by Warncke and Barber (1972) in z i n c - s o i l in t e r a c t io n s t u d ie s w ith eq u a l s u c c e s s . V aidyanathan and Nye (1 9 7 0 ), in . l a t e r s t u d i e s , r e j e c t e d th e u se o f an an ion exchange r e s in paper fo r m easuring P d if f u s io n a s th ey assumed th a t d if f u s io n through th e paper was r a t e li m it in g . T h eir n e x t approach (1971) to m easuring P d if f u s io n was by e v a lu a tin g impedance f a c t o r s to g e th e r w ith th e c a p a c ity f a c t o r a s had been proposed by O ls e n .e t a l (1962) p r e v io u s ly . ' . . . / • ■ In conclusion/,^-much work has gone in t o d eterm in in g how to measure 22 s o i l d if f u s io n and in t e r p r e t in g th e b a s ic p r o c e s s , b oth from s o i l and from p l a n t - s o i l a s p e c t s , As i s n orm ally en cou n tered in p la n t and s o i l r e s e a r c h , system s have n o t been i d e a l and a ls o much measurement has had to be done by in d ir e c t m e th o d s,, As y e t , a p p lic a t io n o f d i f f u s i v e mechanisms fo r d eterm in in g s o i l f e r t i l i t y s t a t u s and p la n t c o n tr ib u tio n have been r e l a t i v e l y u n u t iliz e d e x c e p t in i s o l a t e d in s t a n c e s . i f■ V■/ ' 23 H y p o th e s e s ' I t w a s h y p o t h e s i z e d t h a t b y m e a s u r i n g p l a n a r d i f f u s i v e f lu x f r o m a s o i l to a n e x c h a n g e r e s i n s in k th e r e s u l t s c o u ld b e u s e d to d e p i c t th e s o i l 's f e r t i l i t y s t a t u s , e s p e c i a l l y in r e g a r d to t h o s e n u t r i e n t s t h a t a r e t r a n s p o r t e d to a p l a n t r o o t b y t h i s m e th o d . S p e c ific a lly , th o s e a s p e c ts t h a t c o u ld b e e s t i m a t e d b y t h i s m e th o d i n c l u d e th e f o llo w in g : 1. T h e o r i g i n a l ( b e f o r e r e d u c t i o n b y s in k u p ta k e ) s o i l s o lu ti o n c o n c e n tra tio n . A l s o , th e c o n c e n t r a t i o n a f t e r t i m e = t a n d d i s t a n c e = x f r o m th e a d s o r b i n g s in k . 2. T h e s o i l a d s o r b e d ( a n d o t h e r s t a t e ) io n c o n c e n t r a t i o n th a t c o n t r i b u t e d to d if f u s iv e f lu x b y e q u i l i b r i a , c a l c u l a t e d f r o m th e m o d e l f o r a n i n s t a n t a n e o u s r e v e r s i b l e r e a c t i o n h a v in g a lin e a r a d s o rp tio n is o th e r m . 3. T h e e s t i m a t i o n o f t h e s lo p e o f a l i n e a r a d s o r p t i o n i s o t h e r m ( b u f f e r c a p a c i t y ) c a l c u l a t e d to go to th e o r i g i n f r o m I . a n d . 2. , a b o v e . 4. T h e im p e d e n c e v a l u e f o r a n i n d i f f e r e n t io n ( C l) f o r a n y s o i l u n d e r c o n s id e ra tio n . 5. . F r o m t h e s e f i r s t f o u r (a b o v e ) q u a n t i t i e s , th e c a l c u l a t e d q u a n t i t i e s o f a f e r t i l i z e r t h a t n e e d to b e a d d e d to a s o i l to h a v e i t p r o v i d e a. f lu x r a t e e q u a l t o p l a n t n e e d s . I t w i l l b e s h o w n i n th e " T h e o r e t i c a l C o n s i d e r a t i o n s " s e c ti o n .h o w th e d e v e l o p m e n t o f e q u a t io n s (1 5 ), (16) a n d (17) ( s h o w n i n th e l i t e r a t u r e i y-l . I . . ' • • I • I • 'I ' 1 vi , . - - - - " i t " I i I » i I < v I I y ‘ ' ■ ** I . " ' i ^ I • i V . • ^ • i . . i" 24 r e v i e w p o r t i o n o f th e " I n t r o d u c t i o n " s e c t i o n ) c a n b e d e v e lo p e d to d e t e r m in e th e s e v a r io u s a s p e c t s . W h ile i t m a y .b e n o te d th a t'^ th e i n t e g r a t e d ( o v e r t i m e ) p l a n a r f lu x h a s b e e n p r e v i o u s l y m e a s u r e d b y V a id y a n a f h a n a n d N y e (1966^ a n d o t h e r s , th e s e p a r a t i o n o f a n y o f th e c o m p o n e n ts s h o w n a b o v e h a s n o t b e e n p r e v i o u s l y a c c o m p l i s h e d u s i n g d if f u s io n : th e o ry . :' i ‘ . : i .< I 11■ ’ 25 '' E X P E R I M E N T A L M E T H O D S A N D M A T E R IA L S T h e o r e t i c a l D e v e lo p m e n t A m a j o r p o r t i o n o f th e b a s i c s t u d i e s in s o i l d if f u s io n h a v e b e e n to r e s o l v e h o w f u n d a m e n t a l p r i n c i p a l s o f d if f u s io n a p p ly to ' r a s o il s y s te m . / T h e r e f o r e , th e l i t e r a t u r e r e v i e w s e c t i o n c o n t a in s th e g e n e r a l e s t a b l i s h e d t h e o r y r e l a t i n g to t h i s s tu d y . fro m th is g e n e r a l e s ta b lis h e d th e o ry , P ro c e e d in g a d e v e l o p m e n t w i l l b e g iv e n to s h o w h o w th e c o m p o n e n ts t h a t c o n t r i b u t e to d if f u s iv e m o v e m e n t ( s o i l s o lu ti o n c o n c e n t r a t i o n , fa c to r, s o i l a d s o r b e d c o n c e n tr a ti o n * c a p a c ity e t c . ) c a n b e s e p a r a t e d to c h a r a c t e r i z e a s o i l . T h e q u a n t ity o f s o i l io n f lo w by d if f u s io n in a u n i d i r e c t i o n a l s y s t e m to a c o n s t a n t s i n k o v e r a t i m e p e r i o d h a s b e e n g iv e n p r e . v io u s ly M t = 2 (C o - C r ) [ D i e t (R + l ) ] l / 2 /l7 1 /2 ’ i s th e . s lo p e o f a n a d s o r p t i o n . In e q u a t i o n (1 7 ), is o th e rm , th e (17) (R + I ) t e r m a n d i s a s s u m e d to b e l i n e a r . I t d e s c r i b e s th e a m o u n t o f c h a n g e in t o t a l d i f f u s i b l e io n c o n c e n t r a t i o n ( s o lu ti o n p lu s a d ­ s o r b e d p h a s e ) p e r a m o u n t o f c h a n g e i n s o lu ti o n c o n c e n t r a t i o n w h e n a c o n d i tio n i s i m p o s e d to c a u s e t h i s c h a n g e . M a th e m a tic a lly . (R + I ) = (A C q + A C s ) / A C o w h e re C i s th e s o r b e d (18) 1 ( a n d / o r o t h e r - u n s p e c if ie d ) p h a s e . . If..,/ a f e r t i l i z e r o r o t h e r m a t e r i a l i s a d d e d to a s o i l , m a t e r i a l r e m a in s in d iffu s ib le f o r m , «... , , , ‘‘x . . ‘ I 1 . . I,•I. .I v., r’ < . / I v. , .1 J i l V - W - I i \ ! i x v\ I .. ^ , I < I I ; X - « I . t. . W I I I . I * ' . ‘ ’ 1. x . I I / I a ’ V. / I I I I / X I , j - . - i * ‘ w I i W‘ I I ' I )t I I I V • th e n t h i s q u a n t i t y b e c o m e s -' " v I I .1 I 1 "x < i ' • I I l x i. I v X, / j • : . 11 t U I*. i t i Vy <I a n d if th e : h - _ J . .« , - > . I k ' . -I ' • , " ' . : .. . . ,1 i . . " a / I. I e - U V^ I I■. X » I I . "x • ■ ■ ' / .• (x . . 26 (A C q + A C g). T h e q u a n t ity o f d if f u s iv e m o v e m e n t o v e r a t i m e p e r i o d m a y b e r e w r i t t e n f o r a n u n f e r t i l i z e d s o i l a n d a l s o f o r a f e r t i l i z e d s o il u s i n g th e t e r m s i n t h e r i g h t s i d e o f e q u a t io n (1 8 ), a n d e q u a t io n (17) becom es M t u " 2 (C 0 ~ C r ) ( D l6 t) 1 / 2 [(A C o+ A C s ) / A C o ] 1 / 2 /7T w h ere r e p r e s e n t s th e u n f e r t i l i z e d c o n d i tio n . 1 /2 (19) W h e re f e r ti liz e r h a s b e e n a d d e d , th e n ew s o lu tio n c o n c e n tr a tio n b e c o m e s C q + ACq , an d M fcf = 2 (c 0 + A C o * C r )(D I9 t)1 / 2 [(A C o + A C s ) / A C o ] 1 z 2 Ztt1 / 2 u s in g (20) to r e p r e s e n t th e f e r t i l i z e d c o n d i tio n . T he te rm A C q c a n b e s o lv e d i n t e r m s o f C q b y d iv id in g e q u a tio n (19) b y e q u a t io n (20) M t u ZMt f = (G 0 - C r ) / ( C 0 + A G o - G r ) A ls o , (21) s i m p l i f i c a t i o n m a y b e m a d e b y h a v in g C ^ g o t o >0 ’ ■( a s w a s fo u n d to b e t h e . c a s e i n e x p e r i m e n t s d o n e ) a n d M t u /M tf = V t c O + A C o> <2 2 > . P e r h a p s i t w i l l a d d c l a r i t y , b e f o r e s o lv in g f o r (C q + A C q ) i n t e r m s of C q , to in tr o d u c e a f a c to r " z " . z Cq ; = Cq + ACq. . L e t z b e a q u a n t ity s u c h t h a t T h e n e q u a t io n (22) m a y b e w r i t t e n a s + A c o) = 1 / z = W . . <2 3 > or I .■I < // ■ ■■ W I. 27 * = . (2 4 ) I a n d r e v e r t i n g b a c k to t e r m s u s e d b e f o r e i n t r o d u c i n g z , A C 0 = [ (M t i ZMt u ) - I 3 C o (2 5 ) If th e q u a n t ity o f f e r t i l i z e r a d d e d to a d if f u s io n s y s t e m i s te rm e d " K " , a n d w h ic h e q u a l s A C m a y c o n t r i b u t e to d if f u s io n ) , + AC o ( w h e r e th e t o t a l ' a d d e d " s a n d u s i n g t e r m s j u s t d e f in e d M t u = 2 C o ( D i e t ) l / 2 (K M t u ) l / 2 / [ C o (M t r M t u h ] l / 2 . (26) B y s q u a r i n g b o th s i d e s o f e q u a t io n (2 6 ) a n d s o lv in g C o = (M t u )(M t f - M t u H77) M D ie tK A ls o , fro m . (2 7 ) e q u a t i o n s (2 5 ) a n d (27) A C o = [ ( M t f ZMt u ) - I j ( M t u )(M t f - M t u )(T r)M D ietK . (28) 2 ' A C o = (M t f _ M t u r ( T r ) /4 D I 6 tK . (29.) or F o llo w in g t h i s d e v e l o p m e n t , fro m AC (R + I ) m a y b e e a s i l y d e n o te d r e a l i z i n g i t i s e q u a l to K / A C q . fro m S u b s tit u tin g th e v a lu e o f e q u a t i o n (2 9 ) in to t h i s e x p r e s s i o n 2 2 (R + I ) = 4 K D ie tZ (M t f - M fcu)^TT T q s o lv e f o r C g , th e m in in g la b ile s a m e a n a lo g y w ill be u s e d a s i s w h en d e t e r ­ s o i l io n s A 6 0 /A C S * C0 /C S o r, (30) on re a rra n g in g - ' ... ■ ^ ' C g = (C o ) ( A C g )Z A C o ' (32) an d a ls o I I , . : 4 « . - I l". . I 11 I xl , *' i I j I I v I I I. > \ *. "• X . I I* . i ■I . I - ________ I i J <. i W / I i) ' I I I I I I I ( . ' I < • I <• «I . » I , / , ' ' . " z‘ . ' I I \ I k J• '-I I. ' v ■. . ■ , - . » * ' « ■ ______x _ L i ___________________ . . . -• ■ __________________ J 28 ACs = K - ACo (33) and c S = (C o ) ( K - A C o ) / A C o (34) T h e t e r m s i n t h e r i g h t h a n d s i d e o f e q u a t io n (34) h a v e b e e n fo u n d p r e v ­ io u s ly so th a t . C s = M fcu C(K)/( M t f - M t u ) _ (M t f _ M t u )(7T )/4D I6tK ] (35) T h e u s e o f th e a n a l o g y i n e q u a t io n (31) d e p i c t s t h a t a s t h e s o r b e d p h a s e o f a n i o n a p p r o a c h e s z e r o , th e s o l u t i o n p h a s e m u s t a l s o , a n d w ith a lin e a r re la tio n s h ip . m e re ly T h e re fo re , (R + I ) f r o m t h i s r e l a t i o n s h i p i s (C q + C g) / ^ . F r o m t h e s e e q u a t i o n s , th e v a l u e s i n e q u a t io n (17) m a y b e s o lv e d , providing t h a t t o t a l ions transferred to a sink from a fertilized and u n ­ f e r tiliz e d s o il a r e m e a s u r e d . , a n d tim e m u s t b e m e a s u r e d . I n a d d i tio n , v o l u m e t r i c w a t e r c o n te n t (6), D if f u s io n c o e f f i c i e n t s f r o m d il u te a q u e o u s ^ s o lu tio n e x p e r im e n ts m a y b e u s e d . F o r C l " , K"**, a n d o r t h o p h o s p h a t e i o n s t h e r e h a s b e e n r e p e a t e d a g r e e m e n t i n s o i l s l i t e r a t u r e , w ith I b e in g , ’ D ■ r e s p e c t i v e l y ; I . 8 2 , I . 98 , a n d 0 . 5 X10” ^ c m 3 / s e c . T h e im p e d ­ a n c e v a l u e m a y b e s o lv e d b y a d d in g a n io n a s c h l o r i d e , w h ic h i s n o t a d ­ s o r b e d b y th e c l a y a n d b e c o m e s ACq. I = (M fcf- M t u )3 F r o m e q u a t io n (29) (T T )H D Q tK a (36) T h e t e r m " l a b i l e " u s u a l l y a s s o c i a t e d w ith th e a m o u n t o f s o i l io n e x c h a n g in g w ith i t s i s o t o p e , h a s b e e n u s e d h e r e to a l s o i n d i c a t e th e . t o t a l d i f f u s i b l e a m o u n t. I 29 S o ils U s e d a n d G e n e r a l C h e m i c a l a n d P h y s i c a l A n a l y s i s T w e n ty o n e S ta te s , s o i l s a m p l e s w e r e g a t h e r e d f r o m th e . U n ite d a n d r e p r e s e n t e d a w id e r a n g e o f c h a r a c t e r i s t i c s . T hey w e r e d r i e d f o r 3 d a y s i n a f o r c e d a i r d r i e r a t 60° C a n d s t o r e d f o r f u t u r e p l a n t u p ta k e , c h e m ic a l an d p h y s ic a l a n a ly s is , a n d io n d iffu s io n t e s t s . To d e te rm in e th e ir g e n e ra l c h a r a c te r i s t ic s , w e re d o n e i n i t i a l l y b y u s u a l r o u t i n e m e t h o d s a s fo u n d in m a n y te x tb o o k s . m e th o d , T h e s e i n c l u d e d t e x t u r a l a n a l y s i s b y th e h y d r o m e t e r o r g a n i c m a t t e r c o n t e n t b y th e W a l ld e y - B la c k ( w ith o u t e x t e r n a l h e a t ) m e th o d , w ith ro u tin e ' te s t s IN N H ^ O A c ), e x c h a n g e a b le C a, M g, c a tio n e x c h a n g e c a p a c ity , K a n d N a (e x tra c te d an d a v a ila b le p h o s­ p h o r u s b y O l s e n 's N aH C O g t e s t (w ith c o l o r d e v e l o p m e n t i n a s c o r ­ b i c a c i d ) (1 9 6 5 ). S o il pH m e a s u r e m e n t w a s d o n e b y m i x in g 0 . 01 N C a C lg a n d s o i l i n a 2 :1 r a t i o , a n d p l a c i n g th e pH m e t e r g l a s s I . e l e c t r o d e in th e s o i l s u s p e n s i o n a n d th e c a l o m e l e l e c t r o d e in th e s u p e r n a ta n t liq u id . te rm in e .A ls o , a IN N a O A c e x t r a c t w a s m a d e to d e ­ e x c h a n g e a b le C a a n d M g o n th e c a l c a r e o u s s o i l s , e v i d e n c e d b y t h e i r '.pH v a lu e a n d a l s o b y th e K + Na fro m c a p a c ity . as s u m o f C a + M g +. th e N H ^ O A c e x t r a c t e x c e e d i n g th e c a t i o n e x c h a n g e The IN N aO A c e x tr a c tio n p r o c e d u r e w a s id e n tic a l, c e p t fo r e x tra c ta n t, to th e IN ex­ N H ^O A c e x tra c tin g p r o c e d u r e . T he r e s u lt s o f th e s e d e te r m in a tio n s a r e g iv e n i n T a b le I. T a b l e I - R e s u l t s o f s o i l p h y s i c a l and" c h e m i c a l d e t e r m i n a t i o n s o n s o i l s u s e d in e x p e r i m e n t s . E x c h a n g e a b le c a t i o n s S o il/O rig in C la y . p H CEC % 26 A m s te rd a m si I - M T 26 7 . 5 5 6 A s t o r i a c l - OR 4 . I .3 3 12 5. 8 ^ o / C a m a s C r e e k s i I - ID 18 36 • 5 .4 ’■ 25 D a y to n s i c I - O R . D oO r I - IL 23 5 . 1 18 D r u m m e r s i c I - IN 35 6. 6 29 35 • F r a n k f o r t - B r y c e c -. IN 45 7 . 2 '2 6 J o r y s i I ,- OR ■ 23 5 . 6 17 L lo y d c - A L ' 45 5. I x M i n i d o k a s i - ID •7 7 7. 5 25 d x P o rtn e u f s i I - ID 24 7 . 6 ^ X P o rtn e u f s u b s o i l s i I - ID 16 7. 7 18 12 7. 7 . 13 S agem oor s i - WA 14 S t a n t o n 's C r o s s i n g s i - ID 7 7 . 5 " 21 ^ x T e to n ia s i I - ID 20 7 . 6 12 18 4 . I T ra c y s i - IL t ' 12 W a h lu k e 1 - W A 9 7 .4 21 6. 7 21 W h itn e y 1 - C A 28 6. 3 24 W illia m s I - M T 30 4 . 6 ' W illa m e tte s i c I - OR 28 4 7. 5 8 W in c h e s te r I s - WA Ca Mg ------ m e q /lO O g 16 0.2 9 . 9 ■ 4 12 .14 5 I. 5 5 16 14 13 . 12 1.5 0. 8 8 13 8 5 4.2 . . K Na — 3. 0 1 .5 0. 5 . 0 .4 0 .4 1 .4 1 .4 0 .9 ■ 0 .2 2 .4 6. 0 1 .1 7. 2 I. 0 0. 8 I. 3 0. 7 0 .1 1 .6 1 .0 6. 3 I. I 5. 2 0 .7 2 .2 0 .6 2 .0 0. I 1 .6 2 .5 0. 2 . 0. I 2 .0 0. 3 3. 6 0. 8 5 .4 . I . 0 2 .0 0. 3 0.7 I. 9 P ppm T 0 .3 0. I. T T . T . T . T T T 0. 2 0. 3 0. 3 0. I 0. I T 0 .2 0. 3 T T 0. I OM % ■ 2 .1 20 1 1 .2 9 15. ' 2. I . HO 3 .4 14 3 .2 54 '. 4 . 7 102 3 .7 16 3 .4 4 . 0 .4 - 13 I. 3 43' I. 3 17 0 .9 11 . 0. 6 . 8 I. 9 11 1 .4 ; 24 . 2 .4 34 0 .7 54 3 .4 22 2.0 7 • 2.8 3 0. 3 31 / i / / / • I T o e s t i m a t e l a b i l e P , th e m e th o d i n i t i a l l y p r o p o s e d b y A m e r e t - a l (1 9 5 5 ) a n d w h ic h w a s a l s o c o m p a r e d b y O ls e n (1 9 7 0 ) w a s u s e d . F o r t h i s t e s t I g o f th e t h r e e r a t e s o f t h e s p ik e d s o i l t h a t w e r e u s e d to e s tim a te la b ile K w e re p la c e d in a 12 5 -m l E r le n m e y e r fla s k . T o th is I g o f llA m b e r l i t e 1 R A - 4 1 0 M a n io n r e s i n , w h ic h h a d b e e n p r e v i o u s l y p u r i f i e d i n a c o l u m n r e g e n e r a t i o n p r o c e s s w ith I N r e ta in e d on a 3 2 -m e s h s ie v e , w a s a d d e d . HG I , a i r d r i e d a n d T h e s a m p l e s w e r e th e n p l a c e d u n d e r p a r t i a l v a c u u m to d e g a s th e r e s i n , s t o p p e r e d a n d p l a c e d o n a h a n d s h a k e r f o r 24 h o u r s . A f t e r t h i s s h a k in g p e r i o d , th e r e s i n - s o i l - w a t e r s a m p l e w a s p o u r e d in t o a 6 0 - m e s h s i e v e . T o o b ta in c o m ­ p l e t e t r a n s f e r o f s o i l a n d r e s i n , th e E r l e n m e y e r w a s p a r t i a l l y r e f i l l e d w ith a d d i t i o n a l d i s t i l l e d w a t e r a n d a g a i n p o u r e d in t o t h e s i e v e . The s o i l w a s w a s h e d t h r o u g h th e s i e v e w ith a j e t o f d i s t i l l e d w a t e r , w h ic h l e f t o n ly th e r e s i n . T o c o l l e c t th e r e s i n f o r e x t r a c t i o n , a p i e c e o f f in e . m e s h n y lo n f a b r i c w a s f a s t e n e d v e r y l o o s e l y o v e r th e to p o f a g r a d u a t e c y l i n d e r w ith a r u b b e r b a n d s o t h a t th e r e s i n c o u ld b e r i n s e d o u t o f th e s i e v e w ith d i s t i l l e d w a t e r i n t o t h e h o llo w f o r m e d b y th e n y lo n f a b r i c . ' r A f t e r t r a n s f e r , th 4 n y lo n f a b r i c h o ld in g th e r e s i n w a s t i e d in t o a b a g . T o p r e p a r e to e x t r a c t , t h e b a g g e d r e s i n w a s p o s i t i o n e d a t t h e b o tt o m o f a 3 0 - m l s e p a r a t o r y f u n n e l (w h ic h h a d t h e to p p r e v i o u s l y c u t o ff), a n d w a s h e l d t i g h t l y i n p l a c e b y a t e f l o n - c o a t e d s t i r r i n g r o d w h ic h i n t u r n w a s a t t a c h e d to a s t r e t c h e d r u b b e r b a n d . d o n e w ith 50 m l o f I N v o lu m e tr ic fla s k . , » . I . x > X i I' I ■ - V I . . : -I . ■ xi • . .-i . I ' I I • ■ .X . . r I ' r H ^ S a t th e r a t e o f I d r o p p e r s e c o n d in t o a P h o s p h o r u s c o n t e n t w a s d e t e r m i n e d b y a m m o n iu m i . . „ I [ . . *! W .. C iY I ' ‘ * « < I • • I . V i I I ;: I . / • 1 ! ■x J i ■ ■ ‘ : I . I ' ■ ■. ■ • X. I I < t . »xI « . I IV) ‘ V . I* » ‘ x- ..X ^ • '■ : ■ I ii, •' I1 E x tr a c tio n of th e r e s i n w as j ' X/ I , I I ' t ' ■ I » • -I . ‘ • ' > • 32 m o ly b d a te c o lo r d e v e lo p m e n t in a s c o r b ic a c id . T h e s o il s o lu tio n c o n c e n tr a tio n o f K and P ( a s s o c i a t e d w ith th e l a b i l e c o n c e n t r a t i o n j u s t d e s c r i b e d ) w a s d e t e r m i n e d a t t h e s a m e s p ik in g r a t e s f r o m e x t r a c t s of n e a r s a t u r a t e d p a s t e o n s o i l s a m p l e s u n d e r g o i n g d if f u s io n t e s t s . T h e m e th o d o f p r e p a r i n g th e p a s t e s i s i n ­ c l u d e d i n th e s e c t i o n d e s c r i b i n g d if f u s io n t e s t s . C o n c e n tra tio n of K -i i n th e e x t r a c t s w a s d e t e r m i n e d w ith a f l a m e p h o t o m e t e r . P h o sp h o ru s w a s d e t e r m i n e d , o n t h e e x t r a c t s b y a m m o n i u m m o l y b d a te c o l o r d e v e lo p ­ m e n t in a s c o r b ic a c id w h e r e th e r e w a s s u ffic ie n t c o n c e n tr a tio n f o r th is te s t. A n e x t r a c t i o n o f a m m o n i u m p h o s p h o m o ly b d a te in t o i s o b u t y l a l c o ­ hol was made on eictraets having ins.uffieient concentration for the a s c o r b i c a c i d m e th o d . ' ' V ■ 33 C h e m i c a l D e t e r m i n a t i o n o f S o lu ti o n a n d S o r b e d C o n c e n t r a t i o n a n d C a p a c ity F a c t o r s f o r P h o s p h o ru s a n d P o ta s s iu m ■ •/" T h e d r i e d s o i l s a m p l e s w e r e i n i t i a l l y m o i s t e n e d w ith w a t e r to h a v e 15 p e r c e n t w a t e r b y w e ig h t. T h e y w e r e th e n s t o r e d in p l a s t i c lin e d c o n ta in e r s a t fo u r d e g r e e s c e n tig r a d e f o r s ix w e e k s . To d e te r­ m i n e i f w a t e r l o s s h a d o c c u r r e d a f t e r t h e r e f r i g e r a t i o n p e r i o d , th e s a m p l e s h a d w a t e r c o n t e n t d e t e r m i n e d a n d a llo w e d f o r s p ik in g w ith f e r t i l i z e r to b e d o n e o n a d r y w e ig h t b a s i s . A n e u t r a l s o l u t i o n c o n t a in ­ in g 4 . 32 g K C 1, I . 4 5 g K H 2 P O 4 a n d 2. 89 g K 2 H P O 4 ' SH 2 O p e r l i t e r w a s a d d e d a t r a t e s o f 0, 1 0 , a n d 20 m l p e r 100 g s o i l ( w h ic h h a d p r e v ­ io u s ly p a s s e d th r o u g h a 100 m e s h s ie v e ). T h e s o il w a te r c o n te n t w as t h e n i n c r e a s e d to p r o d u c e a s a t u r a t e d p a s t e a n d th e s o i l w a s m ix e d , a n d a i r d r i e d a t o t a l o f f o u r t i m e s d u r i n g a tw o - d a y p e r i o d . Tb e s ti­ m a te la b ile K , th e m e th o d of G ra h a m a n d K a m p b e ll ( I 9 6 8 ) w a s u s e d , w h e r e 1 . 0 g o f s o i l a n d 24 m l o f 0. 01 M C a C l 2 w e r e a d d e d to a c e n t r i ­ f u g e tu b e . T h e m i x t u r e w a s s t o p p e r e d a n d p l a c e d o n a s h a k e r h a v in g 120 e x c u r s i o n s p e r m i n u t e f o r o n e - h a l f h o u r . T h e n th e s a m p le w as c e n t r i f u g e d a n d t h e s u p e r n a t a n t l i q u i d c o l l e c t e d in a 2 5 0 m l p l a s t i c b o ttle . S e v e n m o r e p o r t i o n s o f C a C l 2 .w e r e s e q u e n t i a l l y a d d e d , s h a k e n a n d c e n t r i f u g e d a s b e f o r e a n d th e r e s u l t i n g e x t r a c t a d d e d to th e p l a s t i c b o ttle . T h e c o l l e c t e d v o l u m e w a s b r o u g h t, to 200 m l b y a d d in g a d d i t i o n a l C a C l 2 s o lu ti o n . P o t a s s i u m c o n t e n t o f th e e x t r a c t w a s d e t e r m i n e d b y fla m e s p e c tro s c o p y , , 34 D e t e r m i n a t i o n o f S o lu tio n a n d S o r b e d C o n c e n t r a t i o n , B u f f e r C a p a c ity A n d I m p e d a n c e V a lu e s b y D if f u s io n F o r th e s e d e te r m in a tio n s , s o i l w a s u s e d f r o m th e s a m e b u lk c o n ta in e r s h a v in g th e s o il w a te r a n d r e f r i g e r a t i o n p r e tr e a tm e n t a s f o r th e c h e m i c a l d e t e r m i n a t i o n o f p h o s p h o r u s , c a p a c ity f a c t o r s . A ls o , th e sam e p o ta s s iu m and s p ik in g s o lu ti o n a n d r a t e w a s a p p l i e d to a 4 0 0 g ( d r y w e ig h t b a s i s ) s a m p l e . T hese s a m p le s w e r e th e n m i x e d w ith d i s t i l l e d w a t e r to p r o d u c e a p a s t e t h a t w a s s lig h tly l e s s w e t th a n a s a tu r a te d p a s te . (T h e r e a s o n f o r t h i s d e v i a t i o n f r o m a n o r m a l s a t u r a t e d p a s t e w a s to e n s u r e t h a t th e solid portion of the samples would not shrink away from the resin s i n k d u r i n g th e d i f f u s i o n p e r i o d , w h ic h w o u ld h a v e p r o d u c e d p o o r • T h e w e tt e d s o i l w a s t h e n p l a c e d in a i I s o il- r e s in s in k c o n ta c t. ) s e a le d p la s tic b a g , ' ' ■ ■ th e b a g w a s p l a c e d i n a r o u n d c a p p e d j a r , and th e j a r p l a c e d o n a s lo w ly r e v o l v i n g r o c k t u m b l e r f o r 2 4 h o u r s . I n t h i s m a n n e r th e b a g r o l l e d i n th e j a r a n d th e s o i l w a s m ix e d w ith n o s e p a r a t i o n o f li q u id f r o m s o lid p h a s e , p r o b l e m w ith o t h e r m i x in g m e t h o d s a t t e m p t e d . w h ic h h a d b e e n a A f t e r t h i s m ix in g a p o r t i o n o f th e s o i l s o l u t i o n w a s e x t r a c t e d u n d e r s u c t i o n in a B u c h n e r f u n n e l a n d th e e x t r a c t s tio n c o n c e n tra tio n - - s a v e d f o r d e te rm in in g s o i l s o lu ­ a s m e n tio n e d in th e s e c t i o n o n " C h e m i c a l D e t e r m i n a t i o n o f S o lu tio n a n d S o r b e d C o n c e n t r a t i o n a n d C a p a c ity F a c to rs fo r P h o sp h o ru s and P o ta s s iu m " . w a s u s e d to f i l l th e d i f f u s i o n c e l l , T he o th e r p o r tio n o f s o il sh o w n in F ig u r e I. In a d d i t i o n t o m e a s u r i n g th e q u a n t i t y o f w a t e r a d d e d to th e s o i l f o r th e d if f u s io n . . . ' - ■ 1 i V V V ' • ’ ' ■ * < 1 . ■ ' 1 - . \ - • * ■ I A C B *-0.30cm wall Brace ■Fine Nylon Mesh E xtracting Solution 4.45cm-> Top View O -ring 0 .3 0 cm wall A djustable Clamp — YZZZA F ig u re I . D if f u s io n c e l l s h o w in g : A - D i m e n s io n s ( m o d e l s h o w n c o u ld h a v e s o i l c o lu m n h e i g h t r e d u c e d to o n e - h a l f ) ; B - C e l l in o p e r a t i o n ; C - M e th o d o f e x t r a c t i n g re s in . A w o o d e n m a tc h c a n b e i n s e r t e d th r o u g h c a p h o l d e r to p u s h o u t r e s in a f te r e x tra c tio n . 36 I • t e s t , th e , s o i l f i l l e d c e l l (o f k n o w n v o lu m e a n d t a r e w e ig h t) w a s w e ig h e d . j F r o m th is , ( p e r c e n t b y v o lu m e ) w a s c a l c u l a t e d f r o m e s t i m a t i n g t h a t th e s p e c i f i c g r a v i t y o f th e m i n e r a l p o r t i o n w a s 2. 65 a n d I P y = [ m l s o i l - ( m l s o i l - g w e t s o i l ) / I . 6 5 ] (m l s o i l / 1 0 0 ) U s in g t h i s s a m e i n f o r m a t i o n to c a l c u l a t e P w (37) ( p e r c e n t b y w e ig h t) P w = 100 [ 2 . 65 ( m l s o i l - w e t s o i l ) ] / 2 . 65 (g w e t s o i l - m l s o il) (3 8 ) a n d b u lk d e n s i t y w a s c o m p u te d f r o m B D = P v ZPw (39) T w o r e p l i c a t i o n s w ith th e t h r e e s p ik in g r a t e s f o r e a c h s o i l w e r e 'd o n e . . W h e n f i l l i n g th e c e l l s , a v i b r a t i n g h a i r c l i p p e r w a s to u c h e d to th e s i d e o f t h e c e l l w h ic h f a c i l i t a t e d g e t tin g th e s o i l p a c k e d w ith o u t a i r b u b b le s . T h e e x p o s e d s o i l a t th e to p o f t h e c e l l w a s s t r u c k o ff w ith a s p a t u l a to p r o d u c e a s m o o t h g l i s t e n i n g s u r f a c e , a n d th e r e s i n s in k (d e ­ g a s s e d a n d p r e v io u s ly s to r e d in w a te r ) w a s p la c e d in c o n ta c t an d w as c a p p e d a s s h o w n i n p a r t B o f F i g u r e I . ' A f t e r d if f u s io n o f i o n s w a s a l lo w e d to t a k e p l a c e f o r 24 h o u r s , th e c a p w ith r e s i n s in k w a s r e m o v e d , a n d th e s o i l a d h e r i n g to t h e n y lo n m e s h w a s r i n s e d a w a y w ith a j e t o f ■ d is tille d w a te r. show n in p a r t E x t r a c t i o n w a s d o n e w ith 100 m l o f IjN C IHL^SO^. a s of F ig u re I . T h e r e s i n u s e d i n t h e s in k w a s a n e u t r a l m i x t u r e o f A m b e r l i t e L< I R - 120 H ( m e d i u m y p o r o s ity ) , a s t r o n g l y a c i d i c r e s in * a n d A m b e r l i t e / IR A -4 1 0 OH (m e d iu m p o r o s ity ) , a s tr o n g ly b a s ic r e s in . th e r 6 s i n s w e r e s i z e d . B e fo re u se , T h e I R - 120 H r e s i n w a s p u r i f i e d w ith I N H ^S O ^ w h ile th e b a s i c 1 R - 4 1 0 r e s i n w a s c o n v e r t e d f r o m th e C l”"to O H " ty p e b y Cv . : -V v* ... .1' 37. IN N aO H in s ta n d a r d r e s i n c o lu m n te c h n iq u e . T o d e t e r m i n e th e p r o p o r ­ t i o n o f e a c h r e s i n to a d d to th e m i x t u r e , e n o u g h o f e a c h w e r e a d d e d to p r o d u c e a n e u t r a l p H w h e n a s a m p l e , w a s p l a c e d in a t e n p e r c e n t N a C l s o lu ti o n . P o t a s s i u m c o n t e n t o f th e e x t r a c t w a s d e t e r m i n e d b y f l a m e e m i s s i o n , ■/ ^ / ■ p h o s p h o r u s b y a m m o n i u m m o l y b d a te c o l o r d e v e l o p m e n t i n a s c o r b i c / ■ acid, a n d c h l o r i n e b y a p o t e n t i o m e t r i c m e th o d . T h i s m e t h o d in v o lv e d t i t r a t i n g a s t a n d a r d 0 . 0 0 2 _N K C l s o l u t i o n i n I N H ^ S O ^ ( r e s i n e x t r a c ­ t i o n s o lu tio n ) w ith 0. 005 N A g N O ^ a n d d e t e r m i n i n g th e r e l a t i v e m i l l i ­ v o l t r e a d i n g ( s e t a t z e r o b e f o r e t i t r a t i n g ) w i t h e a c h i n c r e m e n t a d d i tio n o f th e A g N O 3 . A Ag r e f e r e n c e an d A g -A g -C l e le c tro d e w e re u se d . J T h e i n f l e c t i o n p o in t o f t h e r e s u l t i n g g r a p h a g r e e d w ith th e c a l c u l a t e d e n d p o in t a n d t h e u n k n o w n s w e r e t i t r a t e d to t h i s m i l l i v o l t e n d p o in t w ith th e A g N O 3 s o l u t i o n . | • / 38 I D e t e r m i n a t i o n o f P l a n t U p ta k e f r o m S o ils T h e N e u b a u e r s e e d l i n g m e th o d a s d e s c r i b e d b y V a n d e c a v e y e (1 9 4 8) w a s f o llo w e d c l o s e l y , u s i n g t h r e e r e p l i c a t i o n s o f e a c h s o i l a n d s a n d ch eck s. B a r l e y (H o r d e u m d i s t i c h o n v a r P i r o l i n e ) w a s g r o w n f o r 17 d a y s i n a g r o w th c h a m b e r w ith f u ll l i g h t ( 5 0 0 -6 0 0 m i c r o e i n s t e i n s / m 3/ ■ s e c w ith i n th e 4 0 0 - 7 0 0 n m w a v e le n g th r a n g e ) f o r 16 h o u r s a t 2 4 ° C a n d w ith a n e i g h t - h o u r n i g h t t i m e o f 1 8 ° C . T h e n th e e n t i r e p l a n t w a s h a r ­ v e s t e d , w e ig h e d a n d g r o u n d i n a U d y c y c lo n e m i l l . T he TC A e x tra c ­ t i o n p r o c e d u r e f o r p h o s p h o r u s a n d p o t a s s i u m , a s o u tl in e d b y L e g g e t t , a n d W e s t e r m a n n (1 9 7 3 ), w a s u s e d . P o t a s s i u m c o n t e n t o f th e e x t r a c t w a s d e t e r m i n e d b y f l a m e p h o t o m e t e r , w h ile p h o s p h o r u s w a s d e t e r m i n e d b y a m m o n iu m m o l y b d a te c o l o r d e v e l o p m e n t i n a s c o r b i c a c i d . I I A ls o , th e s h o r t t e r m m e th o d o f D e M e n t, S t a n f o r d a n d B r a d f o r d (1 9 5 9 ) w a s u s e d w ith 4 0 b a r l e y s e e d l i n g s g r o w n . T w o r e p l i c a t i o n s of " m i n u s K " a n d a l s o tw o r e p l i c a t i o n s o f " m i n u s P " t r e a t m e n t s w e r e g r o w n p e r s o i l arid a l s o t h r e e s a n d c h e c k s . T h e r o o t s a n d to p s w e r e g r o u n d , e x t r a c t e d , a n d K a n d P c o n t e n t m e a s u r e d i n th e s a m e m e th o d a s th e N e u b a u e r t e s t s . 39 R E S U L T S A N D I N T E R P R E T A T IO N S I m p e d a n c e V a l u e s f r o m C h l o r i d e D if f u s io n T h e q u a n t ity o f C l t h a t d if f u s e d to th e r e s i n , u s i n g t h e c e l l s h o w n in F ig u re I , w as m e a s u re d . I m p e d a n c e v a l u e s (w h ic h d e n o te th e r e l ­ a t i v e q u a n t ity o f d if f u s iv e f lo w i n s o i l s o l u t i o n a s c o m p a r e d to a n a q u e o u s s o lu tio n of s i m i l a r c o n c e n tra tio n ) w e r e c a lc u la te d f r o m e q u a ­ t i o n (36) to a v e r a g e 0. 28 f o r th e v a r i o u s s o i l s u s e d . T h e s ta n d a rd d e v i a t i o n w a s 0. 1 1 , a n d t h e r a n g e w a s f r o m 0. 10 t o . 0 . 4 6 . T hese v a l u e s fo u n d w e r e i n g e n e r a l a g r e e m e n t w ith th o s e t h a t P o r t e r e t a l (I9 6 0 ) o b ta in e d f r o m C l d if f u s io n . P r e c i s i o n o f t h i s m e a s u r e m e n t w a s s u c h t h a t th e a v e r a g e d e v i­ a t i o n o f a s i n g l e s o i l s a m p l e v a l u e f r o m th e m e a n of r e p l i c a t e s (fo r t h e s a m e s o il) w a s 3. 8 p e r c e n t . F r o m c o m p a r i n g t h e im p e d a n c e v a l u e s o f t h e v a r i o u s s o i l s to t h e i r b u lk d e n s i t y ( w ith in t h e d if f u s io n c e l l ) , t e x t u r e , a n d o r g a n i c m a t t e r c o n t e n t, t h e r e w e r e n o a p p a r e n t re la tio n s h ip s . T h e s o i l w ith th e l o w e s t im p e d a n c e v a l u e (0. 10) w a s A s to r ia c la y lo a m . I t w a s a n e x t r e m e l y " f lu f f y " s o i l a n d h a d a b u lk d e n s i t y o f o n ly 0. 76 w h ile u n d e r g o in g d if f u s io n . T o c o m p u te th e t h e o r e t i c a l C l d i s t r i b u t i o n w ith i n a s o i l u n d e r ­ g o in g d if f u s io n , e q u a t io n (8) m a y b e u s e d . F o r illu s tra tiv e p u rp o se s, th e r e s u l t s a r e s h o w n i n F i g u r e 2 f o r th e D a y to n s o i l a f t e r 24 h o u r s . T h i s s o i l h a d a n a v e r a g e im p e d a n c e v a l u e . A s m a y b e n o te d f r o m F i g ­ u r e 2, d if f u s io n r e d u c e d th e i n i t i a l C l c o n c e n t r a t i o n (C q ) f o r a 2 - c m s o i l d i s t a n c e f r o m th e r e s i n s in k d u r in g th e p e r i o d . T he a v e ra g e quan­ t i t y o f C l a d s o r b e d i n 24 h o u r s b y t h e r e s i n s in k w a s 4 . 3 p e r c e n t o f th e SOLN CONC - /xeq CIZcm^ x - cm (DISTANCE FROM RESIN SINK) F ig u re 2. C o m p u te d s o lu tio n c o n c e n t r a t i o n o f c h l o r i d e a s r e l a t e d to d is ta n c e f r o m s in k , a f t e r d if f u s in g o n e d a y . A z e r o s in k i s a s s u m e d h e r e . C q w a s c a l c u l a t e d f r o m th e C l s p ik in g d o n e . 41 i a m o u n t a d d e d to th e s o i l i n th e s p ik in g s o lu ti o n . It m a y a ls o be v is u ­ a l l y n o te d t h a t th e a r e a o f r e d u c e d c o n c e n t r a t i o n in F i g u r e 2 , a s c o m ­ p a r e d to th e t o t a l a r e a f o r a 1 5 - c m h ig h c e l l , a g r e e s w ith th e 4 . 3 p e r* cen t of Cl a d so rb e d . D if f u s io n a n d C h e m i c a l l y D e t e r m i n e d S o il. P o t a s s i u m T h e r e p e a t e d 0 .0 1 C a C lg e x t r a c t i o n o f s o i l K , a s p r o p o s e d b y G r a h a m a n d K a m p b e l l (1 9 6 8 ) w a s u s e d a s a n e s t i m a t e o f l a b i l e K . I t h a d b e e n s h o w n b y th e a u t h o r s to v e r y c l o s e l y p r e d i c t K - 42 is o to p e m e a s u r e d la b ile K . F r o m c o m p a r i n g th e r e s u l t s o f th e C a C lg e x t r a c t to th e IN N H ^ O A c e x t r a c t f o r e x c h a n g e a b le K ( T a b le I ) , i t w a s n o te d t h a t th e C a C lg e x t r a c t p r o v i d e d s o m e w h a t l a r g e r v a l u e s . T hese a v e r ­ a g e d 0 . 8 4 m e q K / l 0 0 g f r o m th e C a C lg e x t r a c t a n d 0 . 71 m e q K /lO O g s o i l f r o m th e N H ^ O A c e x t r a c t . S im ila r d iffe re n c e s w e re re p o rte d by G r a h a m a n d K a m p b e l l (1 9 6 8 ), a n d th u s th e u s e o f t h e i r p r o c e d u r e se e m e d ju s tifie d . T h e r e s u l t s o f t h i s t e s t a r e s h o w n in T a b le m a y b e c o m p a r e d to d i f f u s i o n - b a s e d e s t i m a t e s o f l a b i l e K . 2 , and T h e d if f ­ u s i o n d a t a d e p i c t i n g l a b i l e K w e r e o b ta in e d f r o m m e a s u r i n g f lu x o f K a n d C l to th e r e s i n s in k d u r i n g a m e a s u r e d t i m e t o g e t h e r w ith th e v a l u e s n e e d e d to s o lv e e q u a t i o n s (27) a n d (3 5 ) f o r C q a n d C g , r e s p e c ­ t i v e l y - a s m e n tio n e d i n th e " M e th o d s a n d M a t e r i a l s " s e c t i o n . \ A lth o u g h t h r e e r a t e s o f s p ik in g (0 , 1 0 , a n d 20 m i s s p ik in g so l* u ti o n p e r 1 0 0 ,g s o il) w e r e u s e d , o n ly th e r e s u l t s f r o m th e 0 a n d 10 m l 'I r a t e w e r e u s e d f o r i n c l u s i o n in T a b le 2 . A l s o , v a l u e s o f M ^ a n d M ^ t h e s e s p ik in g r a t e s a r e i n c lu d e d w ith o t h e r d a t a i n .'T ab le 3 . It w as 42 T a b l e 2 - C o m p a r i s o n s b e t w e e n c h e m i c a l d e t e r m i n a t i o n s a n d d if f u s io n . d e t e r m i n a t i o n s , o f l a b i l e . K , .(C + C ), a n d s o l u t i o n K , (C ). . ' s o o S o il ' C h e m i c a l M e th o d s D if f u s io n M e th o d s L a b ile K * L a b ile K $ f ie q /c m 3 c Ot C o* JLleq/c m 3 J ie q /cm 3 J ie q /cm 3 1.7. 5 0 .4 1 2 3 .7 0 . 33. A s to ria 1 .4 . 06 4 .8 . C am as C re e k 8. 5 . 12 8. 7 . 14 D a y to n 7. 8 .4 7 .' 1 2 . 4 . 67 D oor I, 3 .1 0 '4 / 8 -. 13 1 0 .2 . .5 4 1 2 .0 . 56 • F ra n k fo rt- B ry c e 1 3. T . 46 2 0 .4 . 46 Jo ry 1 0 .2 .. 34 7 ,6 . , 63 7 .4 . 11 1 .8 .1 4 M in id o k a 2 5 .5 I . 82 12. 3 3. 60 P o rtn e u f 16. 9 . 28 1 2 .7 . 17 P o rtn e u f s u b s o il 10. I .1 9 11. 8 .2 5 Sagem oor 1 2 .9 . 17 7 .4 . 23 5. 7 . 04 1 2 .6 ■ .0 7 22. 8 . 39 . . 24. I .4 3 T ra c y 3. 8 . 54 W a h lu k e 5 .7 . 12 W h itn e y 1 5 .2 . ,7 6 W illia m s 18. 6 . 34 1 4 .4 W illa m e tte 2 .6 . 06 4 .5 W in c h e s te r 21. 8 A m s te rd a m • D ru m m e r L lo y d , / S t a n t o n 's C r o s s i n g T e t o n ia . . 33.'.; ' ; ■ 2. 0 5. 8 ■ 1 5 .0 1 1 .6 * F r o m G r a h a m - .E a m p b e ll m e th o d t F r o m s o il s a tu r a tio n e x tr a c t $ C o m p u te d a f t e r m e a s u r i n g K f lu x to r e s i n s in k . . . 03 . 36 • . .0 5 ',.7 5 ■ . 33 .0 5 . .4 1 43 th o u g h t t h a t th e c a p a c i t y f a c t o r (R + l) m i g h t b e r e d u c e d a t h i g h e r s p i k ­ i n g r a t e s b e c a u s e , w ith a l i m i t e d q u a n t i t y o f e x c h a n g e s i t e s o n th e . c l a y s , th e n e w e q u i l i b r i u m b e tw e e n ' s o r b e d a n d s o lu tio n p h a s e w o u ld t e n d to m a i n t a i n a. g r e a t e r s h a r e o f K in s o lu ti o n . F r o m 'r e c o m p u tin g ! f r o m th e h i g h e r t o g e t h e r w ith th e z e r o s p ik in g r a t e ( a s tw o r a t e s a r e n e e d e d f o r o n e d e t e r m i n a t i o n ) , i t w a s fo u n d t h a t th e n e w a v e r a g e C g v a l u e s w e r e r e d u c e d to 83 p e r c e n t o f t h e o ld v a l u e s . L ik e w is e , th e re w a s a n i d e n t i c a l i n c r e a s e i n th e n e w a v e r a g e G q v a l u e s ( a s m a t h e m a t , i c a l l y w o u ld b e e x p e c te d ) . F ig u re 3 i l l u s t r a t e s th e C v a lu e s , as s d e t e r m i n e d f r o m th e z e r o p l u s th e 10 m l s p ik in g r a t e v e r s u s t h o s e d e ­ t e r m i n e d f r o m th e z e r o p l u s t h e 20' m l s p ik in g r a t e . B e c k e t t (1 96 4 ) h a s e s t a b l i s h e d t h a t (R + l) v a l u e s d e c r e a s e w ith h i g h e r c o n c e n t r a t i o n s of . K a d d e d , a n d s o th e r e s u l t h e r e m i g h t b e e x p e c te d . T h e v a r i a t i o n a b o u t th e t r e a t m e n t m e a n f o r K d e t e r m i n a t i o n s .4 o f th e r e s i n s in k e x t r a c t ( M ^ , . M ^ ) a v e r a g e d o n ly 2. 9 p e r c e n t . T h u s t h e p r o c e d u r e a p p e a r e d to b e s u f f i c i e n t l y s i m p l e a n d w ith o u t i n h e r e n t s o u r c e s o f e x p e r i m e n t a l e r r o r f o r a c c e p t a b l e p r e c i s i o n w h e n u s e d to d e te rm in e K d if f u s io n . T h e s i m i l a r i t y o f v a l u e s s h o w n i n T a b le 2 o b t a i n e d f r o m c h e m i c a l e x t r a c t i o n o f s o i l i t s e l f v e r s u s d if f u s io n u p ta k e w a s a n e x c i t i n g s u r p r i s e , i n s p i t e o f th e o r i g i n a l h y p o t h e s i s s u g g e s tin g t h a t a d if f u s io n m e c h a n i s m c o u ld b e u s e d to m e a s u r e s o l u t i o n a n d a d ­ s o r b e d i o n c o n c e n t r a t i o n (C q a n d C g). T h e u s e o f e q u a t io n (30) m a y b e a r r a n g e d s o t h a t ■ ' K = (M t f - M t u ) TT 1 / 2 y ( R + l ) 1 / 2 / (4 D I6 t)1 / 2 /■ 1z "f . (40) Z.Or O 1----------------------------------1------------------------------------- 1— 0 10 20 Cs -/z.eq/cm3 - ESTIMATED FROM O AND IOmI SPIKING/100 g SOIL F i g u r e 3. A d s o r b e d p o t a s s i u m c o n c e n t r a t i o n ( C g ) f o r s o i l s . b e tw e e n tw o s p ik in g r a t e s to c a l c u l a t e C g . C o m p a r is o n i s m a d e 45 and K p r e d i c t s th e q u a n t ity o f s p ik in g n e e d e d to i n c r e a s e th e a c c u m u ­ l a t i v e f lu x o f a n o n s p ik e d s o i l (M^y ) to a n e w v a l u e ( M ^ ) .. I n o r d e r to m a in ta in n o ta tio n , w i l l d e n o te s p ik in g w ith p o t a s s i u m a n d d e n o te p h o s p h o r u s s p ik in g . w ill ■ I n th e c a s e w h e r e f e r t i l i z e r r e c o m m e n d a - . t i o n s a r e n e e d e d K^. w o u ld e q u a l th e q u a n t ity n e e d e d . A p re lim in a ry ' c h e c k w a s m a d e to d e t e r m i n e th e v a l i d i t y o f th e u s e o f th e d if f u s io n e x p e r i m e n t s to d e t e r m i n e n e e d e d ' K^. n e e d e d to o b t a i n t h e v a lu e s . T h i s in v o lv e d c o m p u tin g f o u n d f r o m t h e lo w s p ik in g r a t e (10 m l s p ik in g s o l u t i o n a d d e d p e r 100 g s o il) , o r w h e r e w as a lre a d y know n. T o d o t h i s , th e v a l u e s o f (R + l) a n d I w e r e u s e d f r o m th e r e s u l t s o f th e diffusion cells having the high spiking rate together with the nonspiked s o il. T h e s e r e s u l t s a r e s h o w n i n T a b l e 3. c o m p u te d K w a s 90 p e r c e n t o f a c t u a l K I n t h i s T a b l e , th e a v e r a g e u s e d to o b ta in I t is r e c o g n i z e d t h a t t h e s e v a l u e s w e r e o b ta in e d e n t i r e l y f r o m th e d if f u s io n e x p e rim e n ts. T h e r e f o r e , w h ile i t d o e s n o t s u p p ly p r o o f o f t h e u tility , o f th e m e th o d , i t d o e s m a k e a c o m p a r i s o n f r o m th e d a t a t h a t c o u ld h a v e d is p ro v e n its u tility . T h e r e la tiv e e ffic ie n c y of to w a rd in c re a s in g f lu x c a n b e c o m p a r e d f o r v a r i o u s s o i l s b y u s e o f t h i s m e th o d , w h ic h v a r i e s l a r g e l y f r o m th e p o r t i o n o f K^. g o in g in to s o lu ti o n v e r s u s b e in g a d so rb e d . P l a n t P o t a s s i u m U p ta k e C o m p a r e d t o C h e m i c a l a n d D if f u s io n T e s t s T h e r e s u l t s f r o m th e D e M e n t - S t a n f o r d s h o r t - t e r m t e s t (1959) w e r e s o m e w h a t d i f f e r e n t t h a n th e N e u b a u e r t e s t . S e v e r a l s im p le lin e a r c o r r e l a t i o n s w e r e m a d e b e t w e e n p l a n t u p ta k e q u a n t i t i e s b y t h e s e tw o t , » , \ ' I ' I " ; i,'\ . 1 1! i » ■1 •■ , ! / / I- . I ■ . Z/ / 46 ' I' T a b l e 3 - C o m p u te d q u a n t i t i e s o f s p ik in g n e e d e d to o b ta in ( a c c u m u l a t i v e f lu x p e r d a y ) v e r s u s q u a n t ity o f ,, , a c tu a lly s u p p lie d to o b ta in , S o il M fcu* —----- / ^ e q /c m 3/ d a y -------- C o m p u te d K, t A c tu a l S u p p lie d ----------/ i e q / c m 3 ----------- 2 .8 8 ■ 1 .9 3 11. 6 . 0. 66 0 .2 7 7 .1 4 .6 C am as C re e k I . 84 0 .7 5 12. 8 6 .2 D a y to n 3. 21 I . 68 11. 3 1 0 .0 D oor 2.06 0 . 54 „ 1 3 .3 1 0 .0 D ru m m er 3. 68 2. 05 9 .6 ■ ‘ 1 2 .9 F ra n k fo rt- B ry e e 2 .3 6 1 .5 5 1 0 .6 9 :4 Jo ry .2 .0 3 . 0 . BI 1 1 .6 13. 6 A m s te rd a m . A s to ria ■ ■ , . 9 .7 L lo y d 1 .5 4 0 .1 9 . 1 3 .0 1 0 .9 M in id o k a 7 .4 3 3 .4 8 1 3 .9 1 4 .0 P o rtn e u f I . 88 0 .9 6 12. 2 1 2 .4 P o rtn e u f s u b s o il 2. 37 1 . 14 12. 9 10. 6 . Sagem oor 2. 35 0 . 80 1 4 .5 1 8 ,6 S t a n t o n 's C r o s s i n g 0. 96 0 .4 5 1 4 .1 6. 5 3. 21 2 . 08 •13. 0 1 0 .4 . 2 .4 8 0 .3 3 13. 0 13. 0 I . 05 0 .3 3 12. 8 W h itn e y . 3 .7 0 ■ 2 . 07 11. 8 1 0 .2 W illia m s 2 . 12 1 .1 1 13. I ' 1 3 .4 W illa m e tte I . 01 0 .2 8 12. 0 13. 2 W in c h e s te r 2 .2 9 I . 00 1 5 .0 10. I T e to n ia .f r . •/ ^ T ra c y W a h lu k e ■ * M e a s u re d v a lu e s . ■- • 1 2 .6 f r o m 0 a n d 10 m l s p ik in g r a t e / 1Od g s o il, t, V a lu e c o m p u te d f r o m r e s u l t s o f 0 a n d 20 m l s p ik in g r a t e / 100 g s o il. ■. 47 m e t h o d s v e r s u s c h e m i c a l a n d d if f u s io n t e s t s . The sq u a re d c o rre la tio n ' c o e f f i c i e n t v a l u e s (r3 ) a r e g iv e n i n T a b l e 4 .. 'I n th e D e M e n t - S ta n f o r d m e th o d , p l a n t s a r e f i r s t p a r t i a l l y g r o w n i n a s a n d - n u t r i e n t s o lu tio n K. la c k in g T h e n th e K- d e p l e t e d p l a n t s a r e t r a n s f e r r e d so t h e i r r o o t s g r o w i n s o i l f o r o n ly 6 d a y s . I n c o m p a r i s o n , th e N e u b a u e r m e th o d a l lo w s s e e d l i n g p l a n t s to g ro w i n l i m i t e d s o i l f o r 18 d a y s a n d c o m p l e t e l y K s u p p ly . e x h a u s t th e T h e r e f o r e , th e D e M e n t- S ta n f o r d m e th o d m e a s ­ u r e s a n i m m e d i a t e l y a v a i l a b l e s u p p ly w h ile t h e N e u b a u e r m e th o d t e n d s ■r to c o m b in e t h i s w ith th e r e s e r v e a m o u n t s . A s s e e n , th e N e u b a u e r m e t h o d v a l u e s a n d t h e s o i l e x c h a n g e a b le c o r r e l a t e d ( r a - . 8 1 ), K c o n t e n t w e r e f a i r l y w e ll T h e g r e a t e r s o il e x tra c tio n done b y Graham-* Kampbell1S method, as c o m p a r e d to e x c h a n g e a b le K, r e s u l t e d in m u c h r e d u c e d v a l u e s (r3 = . 3 9 ). C o r r e l a t i o n b e t w e e n th e d if f u s io n m e th o d a n d N e u b a u e r ’ s v a l u e s (r3 = . 54) w e r e i n t e r m e d i a t e to t h e c o r r e l a t i o n s j u s t d e s c rib e d . B y t h e o r y , t h e d if f u s io n m e th o d s h o u ld r e f l e c t i o n m o v e ­ m e n t f r o m a n in fin ite s o u r c e . I n c o n t r a s t , t h e b a r l e y p l a n t s i n th e . N e u b a u e r p o t s a r e e x p e c t e d to a l m o s t c o m p l e t e l y e x p l o it th e a v a i l a b l e K so u rc e . T h u s , th e p o o r c o r r e l a t i o n b e t w e e n th e d if f u s io n m e th o d a n d N e u b a u e r 's m e th o d m i g h t b e a n t i c i p a t e d . R e s u l t s f r o m th e d if f u s io n m e th o d h a d b e t t e r c o r r e l a t i o n w ith th e . D e M e n t - S t a n f o r d c r o p p i n g e x p e r i m e n t ( r 3 = . 88) th a n a n y o f th e c h e m i c a l e v a lu a tio n m a d e . T h u s th e d if f u s io n m e t h o d a p p e a r e d to b e v a l u a b le f o r d e p i c tin g s h o r t - t e r m u p ta k e b y p l a n t s . B y d if f u s io n t h e o r y , io n d if f u s io n to a s in k f r o m s o l u t i o n s h o u ld I I . .... . : , ■ ■ . . • I 11 1 i , i . Ii> . I . I i ^ *v i I » I • I i, < I » ■ ■ / I 48 T a b l e 4 - R e s u l t s o f s i m p l e l i n e a r c o r r e l a t i o n r e l a t i n g p l a n t u p ta k e ....................... o f p o t a s s i u m to c h e m i c a l a n d d if f u s io n . t e s t s . In d e p e n d e n t v a r ia b le E x c h a n g e a b le K G ra h a m -K a m p b e ll " la b ile K " D ep en d en t v a ria b le N e u b a u e r to ta l H It D if f u s io n E x c h a n g e a b le Il G ra h a m -K a m p b e ll " la b ile K " D if f u s io n K S o il s o lu ti o n e x t r a c t K X (c a p a c ity f a c t o r ^ * S o il s o l u t i o n e x t r a c t K X ( c a p a c i t y f a d 'o r ) 1*8 1 .* Il C a p a c i t y f a c t o r c o m p u te d a s : SI Il 39 ’ Il 54 D e M e n t - S t a n f o r d p l a n t K (%) K M, tu S o il s o lu ti o n e x t r a c t K u p ta k e r 3X 100 ' 1 62 M M Il 41 U it it 88 . H Il . 11 54 Il M Il 63 Il Ii M 43 . G r a h a m - K a m p b e ll " l a b i l e K " / s o il s o lu tio n e x t r a c t K t C a p a c i t y f a c t o r c o m p u te d a s : (e x c h a n g e a b le e x t r a c t K ) / s o i l s o lu ti o n e x t r a c t K K + s o i l s o lu ti o n ■' "I Mtu -^.eq/cm2/ 2 4 hrs F ig u re 4 . R e l a t i o n s h i p b e tw e e n p la n t p o t a s s i u m c o n te n t a n d o n e - d a y a c c u m u la tiv e d if f u s iv e f lu x . 50 b e e n h a n c e d b y th e s q u a r e r o o t o f th e c a p a c i t y f a c t o r . T h e re fo re , c a p a c i t y f a c t o r s w e r e e s t i m a t e d f r o m c h e m i c a l d a ta , m u l t i p l i e d b y th e s o l u t i o n c o n c e n t r a t i o n , a n d ’ th e r e s u l t i n g p r o d u c t v a l u e s c o r r e l a t e d . I w ith D e M e n t- S t a n f o r d v a l u e s . T h e r e s u l t i n g c o r r e l a t i o n c o e f f ic ie n ts ( T a b l e 4) w e r e a b o u t th e s a m e a s th e c o r r e l a t i o n c o e f f i c i e n t o b ta in e d ' rZ"" b y c o m p a r i n g s o l u t i o n c o n c e n t r a t i o n a l o n e to th e D e M e n t - S t a n f o r d r e ­ s u lts . T h e r e f o r e , n o b e n e f i t w a s fo u n d b y u t i l i z i n g t h i s c o n c e p t w h e n th e c a p a c i t y f a c t o r w a s t a k e n f r o m th e c h e m i c a l m e th o d s o u tlin e d a t th e b o t t o m o f T a b l e 4 . T h e r e d u c t i o n i n s o lu ti o n K c o n t e n t n e x t to a n e w r o o t i n a s o i l c a n b e d e t e r m i n e d f r o m e q u a t io n (15). I t w a s fo u n d t h a t m o s t o f th e s o i l s w o u ld h a v e th e s o l u t i o n c o n c e n t r a t i o n r e d u c e d to a d e g r e e to a b o u t 0 . 4 c m a t t h e e n d o f a d a y a n d a b o u t d o u b le t h i s in t h r e e d a y s . In th is c a lc u la tio n i t w a s a s s u m e d th a t th e p la n t r o o t g e o m e tr y w a s th a t of a n in fin ite c y lin d e r . E q u a t i o n (15) i s th e f i r s t t e r m o f a s e r i e s s o lu ti o n f o r a c y l i n d e r , a n d th u s a n a p p r o x i m a t i o n . red u ce d , T o k n o w th e p e r c e n t o f C q w o u ld a l s o n e e d to b e k n o w n - - th e f i g u r e o f 0 . 4 c m d e n o t e s t h e e f f e c t i v e s o i l s o l u t i o n v o lu m e a b o u t th e r o o t in r e g a r d to p o t a s s i u m . D i f f u s i o n a n d C h e m i c a l l y D e t e r m i n e d S o il P h o s p h o r u s R e s u l t s o f a v a i l a b l e p h o s p h o r u s d e t e r m i n a t i o n s b y O l s e n 's NaHCOg m e t h o d w e r e g iv e n i n T a b l e I . v a r i a t i o n i n th e s o i l 's T h e s e d a ta p o in t to th e la r g e P 0 E x t r e m e - v a l u e s w e r e 3 a n d H O p p m -P 0 T h e t e s t o f A m e r e t a l (1 9 5 5 ). w ith a n i o n e x c h a n g e r e s i n to e s t i m a t e la b ile P w a s n o t e d t o b e r e l a t e d to O l s e n 's t e s t ( r = O0 9 7 , w h e n e l i m ­ 51 i n a t i n g o n e o b v io u s ly b a d p o in t) w h e r e th e r e s i n e x t r a c t e d a b o u t tw o tim e s a s m u c h s o il p h o s p h o ru s a s N aH C O g. S o il s o l u t i o n e x t r a c t s o f u n s p i k e d A s t o r i a , D o o r , L lo y d a n d S t a n t o n 's C r o s s i n g s o i l s c o u ld n o t b e d e t e r m i n e d w ith s u i t a b l e r e l i a b i l i t y a s t h e y c o n t a in e d l e s s t h a n . 02 ppm P , a s d id L lo y d e v e n a t th e lo w s p ik in g r a t e . s o l u t i o n e x t r a c t s c o n t a in in g a s m u c h a s 2 . 8 p p m O th e r s o ils h a d P. I B y h a v in g th e e s t i m a t e o f l a b i l e P , w h ic h h a s b e e n d e n o t e d a s ( C g + C q ), a n d b y k n o w in g th e s o lu ti o n c o n c e n t r a t i o n , (C q ), f u r t h e r e s t i m a t e s o f th e c a p a c i t y f a c t o r , ( R + l) , w e r e c o m p u te d . . I n th e f i r s t c o m p u t a t i o n ( R + l) w a s l e t e q u a l (C q + C g) / C ^ - w h ic h w a s a l s o u s e d a s a f i r s t a p p r o x i m a t i o n i n th e d if f u s io n e x p e r i m e n t w ith P. F i v e s o i l s i n t h e d if f u s io n e x p e r i m e n t d id n o t s h o w d e f in i te i n - ■ c r e a s e d ( o r s o m e t i m e s e v e n p o s i t i v e ) d if f u s iv e f lu x f r o m i n c r e a s e d r a te s of P s p ik in g . T h e a v e r a g e v a r i a t i o n f r o m th e t r e a t m e n t m e a n v a l u e a v e r a g e d 8. 6 p e r c e n t f o r a l l s o i l s . B e c a u se of th is v a r ia tio n a n d e r r a t i c d i f f u s i v e r e s p o n s e f o r t h e f iv e s o i l s i n p a r t i c u l a r , t h e i r v a l u e s o f C q , C ^ a n d ( R + l) a r e n o t i n c l u d e d i n th e d if f u s io n d a t a . th e o t h e r s o i l s , c o m p a r i s o n a r e s h o w n i n T a b l e 5. For T h e v a lu e s in th is t a b l e w e r e t a k e n f r o m th e n o n - s p i k e d s o i l s a n d th e lo w s p ik in g r a t e . U s in g t h e s e , th e r3 v a l u e r e l a t i n g c h e m i c a l l y d e t e r m i n e d C q to d if f u s io n C q w a s 0. 6 6 . T h e r e v a l u e s r e l a t i n g c h e m i c a l l y d e t e r m i n e d (C g + C q ) a n d (R + l) to d if f u s io n m e t h d s w e r e 0. 33 a n d 0. 2 5 , r e s p e c t i v e l y . O t h e r m e th o d s o f a p p r o x i m a t i n g (R + l) f r o m d if f u s io n w e r e t r i e d , b u t c o r r e l a t i o n s W e re n o t a s g o o d a s t h o s e j u s t s h o w n . 52 T a b l e 5 - C o m p a r i s o n s b e t w e e n c h e m i c a l d e t e r m i n a t i o n s a n d d if f u s io n d e te rm in a tio n s of la b ile P, (C + C ), s o lu ti o n s o P , (C ), a n d ! o (RfI). . C h e m i c a l m e th o d s . S o il L a b ile P * C t O (R + l) ----- /T e q /c m 3 ----- D if f u s io n m e th o d s . L a b ile P $ C o* (R + l)* ---- /T e q /c m 3 ----- A m s te rd a m 39 . 06 650 218 C am as C re e k 62 . 10 620 478 .38 13 D oor '67 .0 3 2140 . 389 . 15 2590 830 415 1 .2 4 330 2 .2 240 D ru m m e r 134- •I& . F ra n k fo rt-B ry c e 219 . 528 2. 6 36 Minidoka Portneuf.subsoil 61 Sagem oor 39 S ta n t o n ’ s C r o s s i n g 20 . 04 460 316 . T ra c y 62 . 08 760 W a h lu k e . 68 .4 0 W h itn e y 150 39 . t4 O ' CO Jo ry 730 . 30 . Q6 . 620 230 ,27 , 21 190 „ 13 ■308 ' 117 . 13 84 900 - 54 7, 6 '7 . 98 1 .4 70 1 .7 4 72 10 3160 203 . 04 5120 170 62 .96 . 65 HO 223 125 W illia m s 58 ,2 0 280 . 273 W in c h e s te r 60 .1 2 . 510 57 * F r o m m e th o d o f A m e r e t a l (1 9 5 5 ) t F ro m s a tu ra tio n e x tra c t $ C o m p u te d a f t e r m e a s u r i n g P f lu x to r e s i n s in k 1 0 .4 I. 58 2 ,8 .21 170 20 53 I A r e a s o n b e l i e v e d p a r t l y r e s p o n s i b l e f o r th e d e v i a t i o n i n d if f u s ­ io n r e s u l t s f r o m c h e m i c a l r e s u l t s (if a s s u m i n g th e c h e m i c a l d e t e r m i n ­ a t i o n s to b e m o r e c o r r e c t ) w a s th e l a c k o f l i n e a r i t y i n th e a d s o r p t i o n is o th e rm s . F r o m c h e m i c a l d a t a th e c a l c u l a t e d s l o p e s f o r s o lu ti o n c o n c e n t r a t i o n s b e tw e e n : (I) 0 to C , o’ (3) c Io w s p ik in g r a t e to (2) x ' C o to C n ^ and lo w s p ik in g r a t e , C h ig h s p ik in g r a t e a r e s h o w n i n T a b l e 6 ‘ m e t h o d o f c o m p u tin g ( I ) w a s th e s a m e a s w a s u s e d in T a b l e 5. c o m p u tin g (2) a n d (3 ), ( A C s o r f e e d + w ere u sed . solation) / The For s o l a t i o n H g u re s It is r e a d ily a p p a re n t th a t F r e u n d lic h - I ik e a d s o rp tio n is o ­ t h e r m s a r e b e in g a d h e r e d to . T h i s ty p e o f i s o t h e r m h a s b e e n a s s o c ­ iated with acid s o i l s b y O ls e n a n d Kemper (1 9 6 8 ). Fox and Kamprath (1 9 7 0 ), f r o m a c i d s o i l s , h a v e p l o t t e d t h e s o l u t i o n c o n c e n t r a t i o n o n a lo g s c a l e v e r s u s t h e a d s o r b e d c o n c e n t r a t i o n o n a l i n e a r s c a l e a n d o b ta in e d s tra ig h t lin e s . T h e c o n s t a n t v a l u e s O l s e n a n d W a ta n a b e (1 9 7 0 ) fo u n d w e re fro m c a lc a re o u s s o ils . A ls o , a d d in g to o m u c h p h o s p h o r u s s p ik in g s o l u t i o n c o u ld b e e x p e c te d to m a k e th e i s o t h e r m f l a t t e n i n t h a t a r e a o f th e c u r v e . H o w e v e r , i f f e r t i l i z e r a p p l i c a t i o n r a t e f i g u r e s a r e to b e d e t e r m i n e d f r o m d i f f u s i o n d a t a , i t s e e m s l o g i c a l t h a t t h e d if f u s io n e x ­ p e r i m e n t s s h o u ld b e d o n e a t , a t l e a s t , t h e s e r a t e s . . T h e p r o b l e m o f c o r r e c t l y s o lv in g C Q, C g , a n d (R + l) v a l u e s , w h e r e c u r v a t u r e e x i s t s , c o u ld b e r e s o l v e d i f t h e r e w e r e a n a l y t i c a l s o lu ti o n s - - o r e v e n a p p r o x ­ im a tio n s . W ith o u t t h e s e , f i n i t e d i f f e r e n c e m e th o d s n e e d to b e u s e d in c o n j u n c tio n w ith a c o m p u t e r . \ '/ 54 T a b l e 6 - S lo p e o f p h o s p h o r u s a d s o r p t i o n i s o t h e r m f r o m c h e m i c a l d e te r m in a tio n s a s d e p ic te d in te x t. S lo p e ( R + l) B e tw e e n S o lu tio n C o n c e n t r a t i o n s S o il O to C O C to C lo w s p ik in g Q H o w . s p ik in g to h ig h s p ik in g A m s te rd a m 560 23 - 470 C am as C re e k 620 168 18 2140 520 194 D ru m m er 830 188 199 F ra n k fo rt-B ry c e 730 22 18 M in id o k a 230 H 37 P o r tn e u f s u b s o il 190 302 . 47 Sagem oor 308 60 142 S t a n t o n 's C r o s s i n g 460 942 T ra c y , 760 ; 547 W a h lu k e 170 16 W h itn e y HO 14 . W illia m s 200 35 W in c h e s te r 510 25 D oor i... u I '! C, : i- • 75 -2. 7 29 5 5 P l a n t P h o s p h o r u s U p ta k e C o m p a r e d to C h e m i c a l a n d D if f u s io n T e s t s T h e N e u b a u e r t e s t f o r p h o s p h o r u s , a l th o u g h fo u n d to g iv e r e p e a t a b l e r e s u l t s , w a s n o t s i g n i f i c a n t l y r e l a t e d to o t h e r s o il o r p l a n t d e t e r m ­ i n a t i o n s . . J n f a c t , th e c o r r e l a t i o n c o e f f i c i e n t r e l a t i n g i t to th e D e M e n tS t a n f o r d s h o r t - t e r m u p ta k e t e s t w a s n o t in c lu d e d h e r e in . O. T h e re fo re , its ’ r e s u lts a re T h e D e M e n t - S t a n f o r d t e s t i t s e l f w a s b e l i e v e d to c o n t a i n s o m e i n h e r e n t e r r o r a s i t a d j u s t e d d i f f e r e n t s o i l s to v a r y i n g m o i s t u r e t e n s i o n s d u r in g t h e t i m e th e s o i l a n d p l a n t s w e r e t o g e t h e r . A s e c o n d D e M e n t - S t a n f o r d t e s t w a s d o n e a n d a t t e m p t s w e r e m d d e to c o m ­ p e n s a te f o r th is . ■T h e s h a p e o f th e c u r v e s r e l a t i n g p e r c e n t P i n th p y p la n ts to s o il q u a n t i t i e s ( O ls e n P , " l a b i l e " P , a n d d if f u s io n P ) w e r e l o g a r i t h m i c . T h e r e f o r e , a l o g a r i t h m i c t r a n s f o r m w a s m a d e o n th e in d e p e n d e n t v a lu e of s o il P. i n F i g u r e 5. R e s u l t s o f th e t h r e e r e g r e s s i o n s a n d c o r r e l a t i o n s a r e 's h o w n T h e b e s t c o r r e l a t i o n s w ith p l a n t u p ta k e w e r e f r o m O l s e n 's N a H C O ^ t e s t (r3 = . 70} w ith th e " l a b i l e " P t e s t (r3 = . 58) b e i n g i n t e r m e d ­ ia te . T h e p o i n t s f r o m tw o s o i l s f o r d i f f u s i o n - m e a s u r e d P w e re not in c lu d e d in F ig u r e 5 a s t h e i r r e p lic a tio n d e v ia tio n w as la r g e . th e y b e e n i n c l u d e d , t h e r H ad v a l u e v /o u ld h a v e r e m a i n e d a b o u t t h e s a m e ■as th e v a l u e o f . 5 2 , s h o w n . T h e c u r v i l i n e a r a p p r o a c h ( F i g u r e 5) w a s th o u g h t j u s t i f i e d i n t h e s e p h o s p h o r u s u p ta k e s t u d i e s , a s i t i s c o m m o n ly a c c e p t e d t h a t t h e r e i s d e c r e a s e d u p ta k e o f i n c r e m e n t s of a d d i t i o n a l ab o v e th re s h o ld le v e ls . P F r o m a d if f u s io n a s p e c t , t h i s c o u ld b e b r o u g h t a b o u t b y p l a n t r e g u l a t i o n o f th e P c o n c e n t r a t i o n a t th e r o o t - s o i l i n t e r f a c e . PLANT P- 56 9- .0 4 3 9 + .0153 (log X) PLANT P-% Mfu - P - /ig Zcm2ZDAY 9- .0 2 6 + .0 2 0 3 (log X) PLANT P-% OLSEN P - ppm Y - . 0 2 8 + .0154 ( I ogX) r2 - . 5 8 50 IOO 150 RESIN "LABILE" P - ppm F ig u r e 5. R e l a t i o n s h i p s b e tw e e n p la n t p h o s p h o r u s c o n te n t a n d s o il q u a n tity a s m e a s u r e d by th r e e m e th o d s . . V > 57 If, f o r e x a m p le , a p la n t th a t i s a b u n d a n tly s u p p lie d w ith s o il le t th e C r P w e r e to in c r e a s e ', th e n th e d iffu s iv e flo w w o u ld d e c r e a s e - - a s it is • r. t h o u g h t to b e p r o p o r t i o n a l to (C Q - C ^ ) . J u d g i n g f r o m t h e r 3 v a l u e s i n F i g u r e 5, t h e d i f f u s i o n t e s t w o u ld not be th e b e s t c h o ic e fo r d e te rm in in g th e so il P s ta tu s . ‘ H o w e v e r, th e u s e o f t h e d i f f u s i o n t e c h n i q u e d o e s a l l o w f o r e s t i m a t i n g t h e a m o u n t of . s p ik in g n e e d e d to b r i n g a b o u t a d e s i r e d f lu x i n c r e a s e p e r t i m e (e q u a tio n 40). U sin g th e s a m e a p p r o a c h a s w a s u s e d f o r p o ta s s iu m , th e q u a n tity • o f s p ik in g w a s e s t i m a t e d th a t w o u ld b e n e e d e d to p r o v id e a d iffu s iv e r a t e e q u a l to (lo w r a t e s p i k i n g ) . T h e e s t i m a t e s w e r e f a i,r ly a c c u r a t e i n a b o u t o n e h a l f o f t h e c a s e s , t h e i r d e v i a t i n g l e s s t h a n 10 p e r c e n t f r o m t h e k n o w n a m o u n t ( T a b l e 7). In th e e x t r e m e c a s e h o w e v e r, th e e s ti m a t e w a s o n l y 21 p e r c e n t of t h e t r u e v a l u e . C h a n g e s i n f l u x r a t e p e r q u a n t i t y of P sid e ra b ly . sp ik in g a d d e d v a r i e d c o n - . F o r e x a m p le , f r o m T a b le 5 it m a y b e c a lc u la te d th a t A s to r ia n e e d e d 4 5 t i m e s a s m u c h p h o s p h o r u s a d d e d a s t h e W h i t n e y s o i l to c h a n g e t h e d i f f u s i v e f lo w I jig P / c m ^ d a y . T h e r e f o r e , th e d e v ia tio n s in c a l c u ­ l a t e d p h o s p h o r u s a s c o m p a r e d to th e v a l u e s a c tu a lly u s e d a p p e a r l e s s s i g n i f i c a n t - - w h e n c o n t r a s t e d w i t h t h e r a n g e of r e l a t i v e e f f i c i e n c y t h a t n e e d s to b e e s t i m a t e d . F r o m e q u a t i o n (15), a n d b y u s i n g t h e s a m e r e a s o n i n g a s w a s u s e d for K, it c a n b e e s t i m a t e d th a t fo r a so il w ith a n o r m a l b u ffe r c a p a c ity o f 5 0 0 , t h e r o o t w i l l r e d u c e t h e s o l u t i o n p h o s p h o r u s c o n c e n t r a t i o n to d i s t a n c e s of o n l y 0. 04 c m i n a d a y . T h is is th e s a m e d is ta n c e as r e ­ p o r t e d b y O l s e n a n d W a t a n a b e (1970) w i t h c o r n ... 5 8 T a b l e 7 - C o m p u t e d q u a n t i t i e s of p h o s p h o r u s ' s p i k i n g n e e d e d to o b t a i n • (a c c u m u la tiv e flu x p e r day) v e r s u s q u a n tity o f sp ik in g a c t u a l l y s u p p l i e d to o b t a i n S o il . C o m p u ted M t£* ■M t u * — At e q / c m 3 / d a y A m ste rd a m A sto ria / I I C am as C reek ■ ■ Peq/ cm 8. 27 . 43 I . 03 0.95 51 5. 31 4 . 35 22 • 3.26 2.58 13. 17 1 1 .1 9 9.92 i l . 62 A c t u a l K. S u p p lie d 3 -------89. ■ 55 105 169 102 74 74 8.59 105 ' 82 1 5 .6 0 5 .7 0 97 ' 106 P o rtn e u f su b so il 7. 71 3.86 Sagem oor 8. 37 4. 46 ■ 151 S ta n to n 's C r o s s i n g I . 83 I . 36 . 46 108 • T racy 2.29 I . 54 98 100 W ah lu k e 6. 12 2.3? 99 98 W h itn e y 21.19 15. 25 89 91 D oor D ru m m er F ra n k fo rt-B ry c e M in id o k a ' . ' 106 . • 99 111 W illia m s 7. 33 5.38 73 100 W in c h e ste r 8.73 3. 57 73 115 * M e a su re d v a lu e s. . M ^ f r o m 0 a n d 10 m l s p i k i n g r a t e / l OOg so il t V a l u e c o m p u t e d f r o m r e s u l t s o f 0 a n d 2 0 m l s p i k i n g r a t e / IOOg ' so il SUMMARY T w o m e t h o d s w e r e u s e d to d e t e r m i n e s o i l s o l u t i o n p o t a s s i u m c o n ­ c e n t r a t i o n s ; (a) t h e q u a n t i t y f r o m a s a t u r a t i o n e x t r a c t a n d (b) th e q u a n t i t y a s e s t i m a t e d f r o m m e a s u r i n g d i f f u s i v e flo w i n t o a r e s i n s i n k . T h e s e a m o u n ts w e r e n e a r l y e q u a l in m o s t s o i l s . F r o m th e d iffu siv e flo w m e a s u r e m e n t s , i t w a s c a l c u l a t e d t h a t t h e e q u i l i b r u m b e t w e e n s o l u t i o n a n d a d s o r b e d p h a s e c l o s e l y a d h e r e d to t h a t of a n i n s t a n t a n e o u s re v e rs ib le re a c tio n . T h is r e s u l t im p lie d th a t th e " c a p a c ity f a c t o r " ' v a l u e (to d e n o t e th e r e l e a s e of s o r b e d i o n s to d i f f u s i v e flo w ) c o u l d be u tilis e d . I n t e r m s of q u a n t i t y of m a t e r i a l t r a n s p o r t e d , th e c a p a c ity f a c t o r c o n c e p t d e n o t e s t h a t d i f f u s i o n i s e n h a n c e d p r o p e r ti o n a d ly to th e s q u a r e r o o t of t h e a d s o r b e d p o o l - - a s c o m p a r e d to if o n ly t h e s o l u t i o n c o n c e n tra tio n w ere, p r e s e n t. T he to ta l q u an tity , ( s o lu tio n p lu s a d s o r b e d ) of p o t a s s i u m e n t e r i n g in t o d i f f u s i v e flo w w a s t h a t w h i c h h a s b e e n n o rm a lly m e a s u r e d as " la b ile " p o ta ss iu m . T he d iffu s io n c e ll, b u ilt for th is e x p e r i m e n t , w o rk e d w e ll w hen p o ta s s iu rn an d c h lo rid e w e r e b ein g d e te r m in e d . By c o m p a rin g d iffu sio n f r o m a s o i l w h i c h h a d t h e s e m a t e r i a l s a d d e d , th e s o i l s o l u t i o n a n d a d s o rb e d q u a n titie s and im p e d a n c e te r m s w e re c a lc u la te d . A lso , c a l c u l a t i o n s d o n e to e s t i m a t e t h e q u a n t i t y of a d d i t i o n a l p o t a s s i u m t h a t w o u ld b e n e e d e d to b r i n g a b o u t a p r e d e t e r m i n e d f l u x r a t e g a v e f a i r e s tim a te s of th e a c tu a l q u a n tity n eed ed . 60 S h o r t - t e r m p la n t u p ta k e o f p o ta s s iu m w a s m o r e c lo s e ly c o r ­ r e l a t e d w ith th e a c c u m u la tiv e d iffu s iv e flu x (as m e a s u r e d f r o m th e u s e o f t h e d i f f u s i o n c e l l ) t h a n w i t h d i r e c t s o i l e x t r a c t s m a d e to d e ­ te r m in e so lu tio n , e x c h a n g e a b le , o r la b ile p o ta s s iu m . Q u a n titie s of la b ile an d so lu tio n p h o s p h o ru s , d e te r m in e d f r o m c h e m i c a l e x t r a c t i o n , in d ic a te d th a t th e a d s o r p t i o n i s o t h e r m w a s n o t lin e a r. T h e r e f o r e , t h e m a t h e m a t i c s d e r i v e d to c a l c u l a t e s o l u t i o n a n d a d s o rb e d c o n c e n tra tio n of p h o sp h o ru s f ro m m e a s u re d acc u m u la tiv e d i f f u s i v e f l u x c a n b e c o n s i d e r e d o n ly a f i r s t a p p r o x i m a t i o n . S h o rt- . t e r m p la n t u p ta k e of p h o s p h o ru s w a s b e t t e r c o r r e l a t e d w ith m o s t c h e m ­ i c a l e x t r a c t s th a n d iffu s iv e flu x . H o w e v e r , th e d iffu s io n m e a s u r e m e n t (as w ith p o ta s s iu m ) p ro v id e d f o r e s tim a tin g t h e , q u a n tity of p h o s p h o ru s ' a s o i l n e e d e d to b r i n g a b o u t a p r e d e t e r m i n e d f l u x r a t e . A s th e q u a n ­ t i t y o f p h o s p h o r u s n e e d e d to i n c r e a s e a u n i t f l u x r a t e v a r i e d m a n y , fo ld b e tw e e n s o i l s , . th e e r r o r a s s o c i a t e d w ith th e e s t i m a t e d p h o s p h o r u s • n e 'e d w a s b e l i e v e d to b e m o r e a c c e p t a b l e . M u c h a d d i t i o n a l r e s e a r c h i s n e e d e d to m o r e c l e a r l y r e s o l v e p r o b le m s a s s o c ia t e d w ith th e th e o ry a n d .e x p e rim e n ta l m e th o d s' u se d , a n d to r e s o l v e p r o b l e m s i n t r o d u c e d b y t h e e x p e r i m e n t i t s e l f . In­ c lu d e d i s th a t o f o b ta in in g a b e t t e r k n o w led g e of th e f a c t o r s in v o lv ed in th e ti m e la p s e b e t w e e n a d d in g a s p ik in g " m a te r ia l a n d s t a r t i n g th e . d iffu s io n p r o c e s s . A b e t t e r a t t a c k i s n e e d e d to d e t e r m i n e t h e c a ­ p a c ity f a c to r fo r p h o s p h o ru s , and in te r p r e tin g it m a th e m a tic a lly . T h e v a r i a t i o n b e t w e e n r e p l i c a t i o n s i n p h o s p h o r u s f l u x to a r e s i n s i n k ■ . " . ■ .61 n eed s m o re c o n tro l.. needs T h e t i m e i n v o l v e d i n d o i n g th e d i f f u s i o n t e s t s h o r t e n i n g i f t h e m e t h o d w e r e to b e u s e d i n r o u t i n e a n a l y s i s . C o r r e l a t i o n b e tw e e n r e s u l t s of fie ld f e r t i l i t y s tu d ie s an d d iffu sio n t e s t s a r e n e e d e d i f t h e d i f f u s i o n t e s t i s to b e a p p l i e d i n t h a t m a n ­ n er. O th er p la n t n u tr i e n ts , b e sid e p h o sp h o ru s and p o ta s s iu m , th a t a r e t r a n s p o r t e d to th e r o o t m a in ly by d iffu s io n m ig h t be e v a lu a te d s i m u l t a n e o u s l y by. t h e d i f f u s i o n m e t h o d a n d t h u s m a k e t h e t e s t m o re in c lu siv e . 62 R E F E R E N C E S C IT E D • A m er, F . , D . R . B o u l d i n , ■ C . A . B l a c k , a n d F . R . D uke.. 1955. C h a r a c te r iz a ti o n of s o il p h o s p h o ru s by a n io n ex c h a n g e r e s i n a b so rp tio n and P -3 2 - E q u ilib ra tio n . P l a n t a n d S o il VI, N o . 4 :3 9 1 -4 0 8 . x B a r b e r , S ta n le y A . 1962. A d iffu s io n a n d m a s s - f lo w c o n c e p t of „ s o il n u trie ry h a v a ila b ility . S o il S c i . 9 3 : 3 9 - 4 9 . B a r b e r , S. A . 1968. On th e m e c h a n i s m g o v e rn in g n u t r i e n t . su p ­ p ly to p l a n t s g r o w i n g i n s o i l . 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R . O l s e n . 1965. T e s t of a n a s c o r b ic a c i d m e th o d f o r d e t e r m i n i n g p h o s p h o r u s in w a t e r a n d N aH C O g - e x t r a c ts f r o m s o il. S o il S c i . S o c . A m e r . P r o c . 2 9 : 6 7 7 - 6 7 8 . .68 W a t a n a b e , F 1. S . , a n d S. R . O l s e n . 1962. C o lo m e tric d e te rm in a tio n of p h o s p h o r u s in w a t e r e x t r a c t s of s o il. S o il S c i . 9 3 : 183-188. ■ A p p e n d i x A - R e s u l t s o f c h e m i c a l d e t e r m i n a t i o n s of s o i l p o t a s s i u m - ( s o i l b u l k d e n s i t y i s i n c l u d e d f o r c o n v e r t i n g v o l u m e d a t a to a w e i g h t b a s i s i f d e s i r e d ) . 0 sp ik in g BDt S o il S o ln K t L a b i l e K ** 10 m i s s p i k i n g p e r 100 g s o i l * S o ln K t * t $ ** 1 .2 4 0. 76 1 .4 6 1 .2 0 1 .4 2 I . 02 I . 13 1 .2 3 I . 38 1 .4 8 I . 30 1 .3 7 . I . 54 I . 50 I . 39 1 .3 9 I . 36 1 .2 6 1 .3 9 1 .2 8 1.60 S o ln K t L a b ile _ ^ cm 3 g /cm A m ste rd a m ■' — A sto ria C am as C reek D a y to n Door D ru m m er F ra n k fo rt- B ry ce Jo ry L lo y d M in id o k a P o rtn e u f P o rtn e u f su b so il Sagem oor S ta n to n 's C r o s s i n g T e to n ia T racy . W ah lu k e " W h itn e y W illia m s W illa m e tte W in c h e ste r L a b i l e K ** 20 m i s s p i k i n g p e r 100 g s o i l * .4 1 . . 06 : .1 2 .4 7 . 10 .5 4 .4 6 . 34 .1 1 I . 82 . 28 . 19 .1 7 .0 4 . 39 .1 6 . 12 . 76 . 34. .66 .3 3 17. 5 1 .4 8.5 7. 8 I. 3 8. 5 13. I 10. 2 7 .4 2 5. 5 16. 9 10. I 12. 9 5 .7 22.8 3. 8 5 .7 . 1 5 .2 18. 6 2.6 . 21. 8 I . 04 .4 1 .8 1 1 .4 9 .9 0 1 .2 1 .0 7 I . 12 .7 3 2 .7 4 .7 4 .7 1 .7 3 . 61 .99 I . 30 .5 5 I . 78 1 .1 1 . 50 I . 13 22. 8 5 .0 1 3 .1 1 1 .9 5 .1 13. 3: 18. 9 1 5 .4 13. I 32. 3 22. 5 16. 6 20. 0 11. 8 —1 0. 3 11. 9 2 0. 0 2 5. 2 8 .4 2 9. 0 I . 84 .9 9 2. 56 2. 63 2. 33 2. I I . 88 2. 21 2. 03 6. 10 1 .2 1 I . 56 I . 58 I . 26 I . 64 3. 27 I . 34 2.96 2. 06 I . 26 2.38 2 7 .0 7 .2 1 6 .2 1 6 .4 1 1 .2 . -17.-5 2 2 .4 • 21. 2 18. 5 3 5 .7 26.3 . 2 2 .5 24. 5 1 6 .0 27. 6 1 5 .6 1 6 .4 24.3 3 0 .8 1 3 .4 33.9 T h e 10 a n d 20 m l s p i k i n g r a t e s h a d e q u i l i v a l e n t to 0. 9 4 a n d I . 82 m e q K a d d e d / 1 0 0 g so il, r e s p e c tiv e ly . B u l k d e n s i t y f i g u r e s t a k e n f r o m d i f f u s i o n c e l l d a t a , u s i n g e q u a t i o n (39). S o lu tio n K v a lu e s w e r e f r o m so il s a tu r a tio n e x t r a c ts . L a b ile K e s ti m a t e d f r o m C a C l^ e x t r a c t d e n o te d in te x t a s G r a h a m - K a m p b e ll m e th o d . A p p e n d i x ' B - R e s u l t s of c h e m i c a l d e t e r m i n a t i o n s o f s o i l p h o s p h o r u s - ( s o i l b u l k d e n s i t y i s i n c l u d e d f o r c o n v e r t i n g v o l u m e d a t a t o a w e i g h t b a s i s if d e s i r e d ) . 10 m i s s p i k i n g p e r 100 g s o il* 0 sp ik in g S o il BDt S o ln P t . L a b i l e P * * * t $ . 07 I. 2 4 -T ,0 4 . 76' 1 .4 6 . 10 1 .2 0 .1 2 1 .4 2 ' . 03 I . 02 . 16 I . 13 . 30 I . 23 . .06 0 I . 38 .2 7 ■ 1 .4 8 .4 5 I . 30 I . 37 . 20 .1 3 1 .5 4 .04 I . 50 . 26 I . 39 . 08 I . 39 I . 36 . .40 I . 26 1 .3 9 . . 20 • I . 39 ; 04 I . 28 . 12 I . 60 S o ln P t L a b ile P** u Si/ c m 3 g /c m A m ste rd a m A sto ria C am as C reek D a y to n D oor D ru m m er F ra n k fo rt- B ry ce Jo ry L lo y d M in id o k a P o rtn e u f P o rtn e u f su b so il Sagem oor S ta n to n ’s C ro s s in g T e to n ia T racy W ah lu k e ' W h itn e y Willia m s W illa m e tte W in c h e ste r L a b ile P * * S o ln P t 20 m i s s p i k i n g p e r 100 g s o i l * ■ 39 •24 . 62 133 67 134 21 9 36 40 61 100 39 39 20 59 63 68 150 58 73 60 .. I . 00 . .03 .34 .1 7 .1 2 .36 .8 7 . 04 0 3. 57 I . 92 .29 .89 .. 08 .4 6 .1 7 2 . 00 2 . 85 .8 2 ,06 4 .0 5 T h e 10 a n d 20 m l s p i k i n g r a t e s h a d e q u i v a l e n t re sp e c tiv e ly . B u lk d e n s ity f i g u r e s ta k e n f r o m d iffu s io n c e l l S o lu tio n P v a lu e s w e r e f r o m so il s a tu r a t io n L a b ile P e s tim a te d f r o m r e s in e x tra c tio n a s • . 60 33 103 178 112 171 2-31 51 57 100 137 63 86 58 105 HO 94 171 80 101 114 .93 .0 3 I . 76 .4 0 .2 1 .4 9 1 . 13 . 05 . 03 ■ 4 .2 9 2 .4 5 1.25 . 1 .0 9 .52 1 .2 9 —— I . 69 4.21 2. 58 . 11 3.38 95 44 129 2 13 130 198 236 62 69 127 169 HO 114 . 92 135 124 129 175 130 119 145 ' to 72. 3 a n d 144. 5 /i e q P / g s o i l a d d e d , d a t a , u s i n g e q u a t i o n (39). e x tra c ts. d e n o te d in te x t. 71 A p p e n d i x G - C a l c u l a t e d i m p e d a n c e v a l u e s (I) a n d q u a n t i t y o f p o t a s s i u m d i f f u s i n g to r e s i n s i n k , s u r f a c e (7. 9 2 c m ) p e r 2 4 - H o u r p e r i o d (M t ) 1 • S o il I* 0 sp ik in g 10 m l s p i k i n g p e r 100 g s o i l t /4»g JX/ I o' O CH J L / <-^*x XlT D .A m ste rd a m . .42 '15. 3 • 22. 8 A sto ria $ . 11 2 .1 5 .2 C am as C reek .28 5. 9 D a y to n .29 1 3 .3 Door .46 4 .3 D ru m m er $ .2 6 F ra n k fo rt-B ry c e ' . 20 m l s p i k i n g p e r 100 g s o i l t 33. 2 , 1 4 .4 . 5 0 .5 1 4 .6 ' . 2 5 .4 40. I 1 6 .3 35. 6 16.2 29.1 41. 5 .2 1 1 2. 3 1 8 .7 Jo ry .1 2 ' 6 .4 1 6 .1 2 2 .5 L lo y d .1 4 ' 1 .5 12. 2 26.8 M in id o k a .2 8 27. 6 58.8 90.0 P o rtn e u f .38 7. 6 1 4. 9 2 1 .8 P o rtn e u f su b so il .4 3 ■ 9.0 1 8 .8 32.2 Sagem oor . 39 ■ 6. 3 1 8 .6 S t a n t o n ' s C r o s s i n g . . 23 3. 6 ' 7 .6 . ■ 2 6 .7 , " ' .25.5 20.8 T e to n ia .4 0 1 6 .5 2 5 .4 T racy $ .,36 .2.6 19. 6 47. 6 W ah lu k e . 35 2. 6 8.3 1 4 .2 W h itn e y . 33 1 6 ,4 .29.3 45.9 W illia m s . 15 8.8 16.8 2 9 . 2 W illa m e tte . 32 2.2 8. 0 W in c h e ste r .2 4 7. 9 18. I . ' . .38.9 ' 17. 3 38. I '* I m p e d a n c e v a l u e s c a l c u l a t e d f r o n d e q u a t i o n (36), a f t e r m e a s u r i n g C l" d i f f u s i o n . t T h e 10 a n d 20 m l s p i k i n g r a t e s c o n t a i n e d e q u i v a l e n t t o 0 .'9 4 .and I . 82 m e q . K a d d e d / 1 0 0 g s o i l , r e s p e c t i v e l y . $ S a m p l e s d if f u s e d f o r 40 h o u r s , r a t h e r th a n 24. 72 A p p e n d i x D - C a l c u l a t e d i m p e d a n c e v a l u e s (I) a n d q u a n t i t y o f p h o s p h o r u s d i f f u s i n g to r e s i n s i n k s u r f a c e (7. 92 c m ) p e r 2 4 -h o u r p e r i o d (Mfc) S o il 0 sp ik in g I* 10 m l s p i k i n g p e r 100 g s o i l ! ■ r* H n -O I l & ■*■ / 1• 0/ 9“ A m ste rd a m . 66 .42 ' 7 .5 / 9 A. ^ t ~ 20 m l s p i k i n g p e r 100 g s o i l ! T-, T- C * 172 92 9 .0 8.2 A sto ria * . 11 C am as C reek . 28 34 42 D a y to n .2 9 89 58. 75 D oor .4 6 . 20 26 27 D ru m m er * . 26 89 • 1 04 .■ F ra n k fo rt- B syce . 21 68 78 Jo ry . 12 5. 7 L lo y d . 14 . 7 .2 ' M in id o k a .2 8 45 1 24 . 2 16 P o rtn e u f .3 8 88 82 130 P o rtn e u f su b so il .4 3 31 • 61 Sagem oor . 39 35 66 S t a n t o n ’s C r o s s i n g . 23 10. 8 fT e t o n i a .40 116 89 T racy*. . 36 12 18 W a h lu k e . 35 19 49 W h itn e y . 33 121 168 2 17 W illia m s . 15 43 58 85 W illa m e tte . 32 39 14 29 W in c h e ste r ' . 24 28 69 168 ' * Im p ed an ce v alu es m e a s u rin g C l" t T h e 10 a n d 20 m l a n d 144. 5 ^ g P $ S a m p le s d iffu se d 108 120 85 1 0 .0 9.3 7 .2 9 .0 ■ - 88 . . 81 28.2 . 14.5 " 153 24 ■ - 77 c a l c u l a t e d f r o m e q u a t i o n (36), a f t e r d iffu sio n . s p i k i n g r a t e s c o n t a i n e d e q u i v a l e n t t o 7 2. 3 a d d e d /g so il, r e s p e c tiv e ly . f o r 4 0 h o u r s , r a t h e r t h a n 24. V. ' . ' vv fuyg4 * - P 3T 9 M 383 c o p .2 i » " a a s e « ;, T ru m a n W S o il c h a r a c te r ! z a tio r h y d if f u s io n m e a s u re m e n ts X A M K A N o A bom m em O i - . u l c c x ^ V i '^ b y - J - R .* t> - >v s c j , C/4i-r>i n c r A l (i b 2 " F E B 8 Jfr F / V r ^ ? ZT r s . z -7 L /nr.i<r, .- L t A r ^ V M f ^ S T " 5^ A V /\ 5 / /« " " W t W " ~\ -ZL n O /;3 i3 ( U * . 3- T 7 ~