Ratios, proportions, and mixtures of chlorophylls: corrections to spectrophotometric methods and an approach to diagnosis. I. M. Henderson Ecology Group Institute of Agriculture and Environment Massey University Palmerston North New Zealand. Supporting Information Appendix 1. Further detail and explanation of mathematical derivations were requested by a reviewer. For consistency, equations are numbered the same as in the main text and additional equations are given letter subscripts where needed. A. The relationship between an absorbance ratio and the proportions of a mixture. Let ai,j be the specific absorbance of one unit of chlorophyll i at the characteristic peak (λj) of chlorophyll j, Ai is the measured absorbance at wavelength λi, and Ci is the concentration of chlorophyll i in the sample . A mixture of two chlorophylls has proportion P of chlorophyll 1 and (1P) of chlorophyll 2, and the observed absorbances will be: π΄1 = πΆ1 π1,1 + πΆ2 π2,1 π΄2 = πΆ1 π1,2 + πΆ2 π2,2 Since π = πΆ1 ⁄(πΆ1 + πΆ2 ) π΄1 = πΆ1 π1,1 + πΆ1 ((1 − π)⁄π)π2,1 π΄2 = πΆ1 π1,1 + πΆ1 ((1 − π)⁄π)π2,2 In a ratio the concentration (C1) is eliminated and: ππ π΄ +(1−π)π π = π΄1 = ππ1,1 +(1−π)π2,1 2 1,2 2,2 (1) This can also be expressed in terms of the ratio (x) of the two chlorophylls: x = P/(1-P) so P = x/(x+1) and (1-P) = 1/(x+1). Substituting these into (1): π₯π +π π = π₯π1,1 +π2,1 1,2 2,2 (1a) The ai,j can also be expressed in terms of dimensionless ratios. The minimum value of r will be when only chlorophyll 2 is present so P = 0 and from (1), rmin = a2,1/a2,2. The maximum ratio is when only chlorophyll 1 is present, P = 1 and rmax = a1,1/a1,2. Let S be the ratio of specific absorbances at the respective peaks, a1,1/a2,2. Substituting these ratios into (1a) and simplifying gives: ππ₯+ππππ πππ₯ )+1 π = (ππ₯⁄π (1b) The inverse relationships are (from 1a): π π₯ = ππ2,1 −ππ2,2 1,2 −π1,1 And from (1b) 1 π π₯ = π ((π⁄ππππ −π πππ₯ )−1 ) (1c) The ratio x will be undefined when one of the chlorophylls is absent (r = rmax), so it will be more useful to express this relationship in terms of the proportion of one of the chlorophylls: π = π= π₯ π₯+1 = 1 (1+1⁄π₯) 1 (π⁄ππππ₯ )−1 ) 1+π( ππππ −π (2) This expression is undefined when r = rmin but in that case P is clearly zero which is an easier error to trap. Multiplying (2) through by (rmin – r) gives the alternative form π=π ππππ −π πππ −π+ππ ⁄ππππ₯ −π From which it can more easily be seen that this relationship will be linear in r only if S = rmax. B. What ranges of parameters are realistic? It would be possible to insert a wide range of parameter values into (2) but these may not be realistic for a combination of two chlorophyll spectra. The shape of a spectral peak can be approximated by a Gaussian curve (Aguirre-Gomez et al. 2001) and for the red peaks of chlorophylls in acetone the spread usually corresponds to a standard deviation of 8-10 nm. If the peaks are identical in height (S = 1) but differ by one standard deviation rmax will be 1.645 and rmin = 1/rmax = 0.608. This set of parameters is similar to those defining the upper curve in Fig. 2 of the main text. Given that these methods are likely to be considered when the peaks are distinct enough to provide resolution but still overlap considerably (e.g. the 10 nm difference between chlorophyll a and bacteriochlorophyll d) the general features of that curve are to be expected. However, if the peaks differed by 20 nm the range of ratios will be much greater (rmax = 7.4 and rmin = 0.14. If the specific absorbance coefficients (ai,i) of the two pigments differ (S ≠1) or the peak widths differ, other forms are possible. For example with a 9 nm difference between peaks, equal standard deviations but a1,1 50% higher than a2,2, rmax = 1.5, rmin = 0.67 and S = 1.5 so the relationship between P and r will be linear as in the middle curve of Fig. 2. The parameters of the lower curve in Fig. 2 can be obtained from the case of a 13 nm difference in peak location, 20% greater spread and 4-fold greater specific absorbance in the peak for one of the chlorophylls; an admittedly extreme case. C. Elaboration of the method of Moss (1967a & b) Moss (1967a) empirically established the relationship between the ratio of absorbances A 430/A410 and the proportion of phaeophytin in a mixture with chlorophyll a. In Moss (1967b) he shows how this proportion, and absorbance at 665nm, can be used to estimate concentrations of both pigments. Both pigments have red absorbance peaks close to 665nm but the specific absorbance of chlorophyll a is greater than that of phaeophytin a (90.8 and 55.2 L g-l cm-l are the values Moss used). Following Moss (1967b) but in the notation used here π΄665 = πΆ1 π1 + πΆ2 π2 Where C1 is the concentration of chlorophyll a, C2 the concentration of phaeophytin a and ai their respective specific absorbances. Let x = C1/C2 so: π΄665 = πΆ1 π1 + πΆ1 π π₯ 2 π₯π΄665 1 +π2 πΆ1 = π₯π And similarly: π΄ πΆ2 = π₯π 665 +π 1 2 Substituting x from (1c) πΆ1 = π΄665 π⁄ππππ₯ −1 )) ππππ −π (π1 +π2 π( πΆ2 = π΄665 π −π π (π2 + 1 ( ⁄ πππ )) π π ππππ₯ −1 The ratio of a1/a2 is sometimes called the acid ratio as it would be the ratio of absorbances at 665nm before and after addition of acid to convert chlorophyll to phaeophytin. This ratio is usually taken as 1.7 for pure chlorophyll a (Lorenzen 1967) but Moss (1967b) used the equivalent of 1.64. It is also convenient to use the inverse of the specific absorbance coefficients scaled to mg in equations; e.g. 1000/a1 = 11.01 mg cm L-1 using the figures of Moss, but 11.5 is more reasonable given recently derived specific absorbances of approximately 87 L g-1 cm-1 (Ritchie 2006). The absorbance peak of chlorophyll in 90% acetone is also now generally reported as 663 nm. With these modifications equations in a more familiar form can be produced: π (π ⁄ππππ₯ )−1 πΆβππ (mg L-1 ) = πΉ × π΄663 × 11.5⁄(1 + 1.7 ( 1 1 ππππ −π π )) −π )) πππ₯ )−1 πβπ (mg L-1 ) = πΉ × π΄663 × 11.5⁄(1.7 + π ((π⁄ππππ (3) (4) Where F = volume of acetone (ml) / (volume of lake water filtered (L) x cuvette path length (cm)) D. Corrections to the method of Parkin & Brock (1981). Parkin and Brock (1981) based the form of their equations on the proportion of absorbance at a particular wavelength due to each of the chlorophylls in a mixture. As before, let ai,j be the specific absorbance of chlorophyll i at the peak of chlorophyll j, Ci be the concentration of chlorophyll i in the sample, Di be the proportion of absorbance at the peak of chlorophyll i that is due to chlorophyll i, and P is the proportion of chlorophyll 1 (P = C1/(C1+C2)). πΆ1 π1,1 π·1 = πΆ 1 π1,1 +πΆ2 π2,1 1 Since πΆ2 = πΆ1 (π − 1) the concentrations can be eliminated and π·1 = π1,1 π1,1 +(π2,1 (1⁄π −1)) Substituting Eq. 2 for P π·1 = π1,1 π⁄ ππππ₯ −1 ))) ππππ −π π1,1 +(π2,1 (π( and noting that a2,1/a1,1 = rmin/S, this simplifies to: π·1 = π1,1 π⁄ ππππ₯ −1 )) ππππ −π π1,1 +(ππππ π1,1 ( Now the specific absorbance (a1,1) can be eliminated and simplified to π·1 = ππππ −π π π( πππ −1) ππππ₯ And rearranged to π·1 = ππππ₯ ((ππππ ⁄π )−1) ππππ −ππππ₯ (7) Following similar steps π·2 = π π−ππππ₯ πππ −ππππ₯ (8) (7-8) can be expressed in a similar form to that used by Parkin & Brock (1981, see Eq. 5a and 6a in main text) as π·1 = [(1⁄π × π) − π] (7a) π·2 = [(π × π) − π] (8a) Where c = (rmax x rmin)/(rmin - rmax), g = rmax /(rmin - rmax), e = 1/(rmin - rmax). Their full method could thus be written πΆβππ = [(π⁄π × π) − π] × π × 11.9 × πΉ (7b) π΅πΆβππ = [(π⁄π × π) − π] × π × 10.2 × πΉ (8b) Where a = absorbance at 663nm, d = absorbance at 654nm, F = volume of acetone (ml) / (volume of lake water filtered (L) x cuvette path length (cm)). 11.9 and 10.2 are derived from the inverse specific absorbance coefficients (1/ai,i) with units g cm L-1. Based on Parkin & Brock’s (1981) equations, likely values for the remaining parameters are c = −0.87, e = −0.99, g = −1.55. E. Corrections to the method of Caraco & Puccoon (1986) Equations 7b and 8b can be rearranged to closely match the form of Caraco & Puccoon’s (1986) equations. Their “Ext” parameters are the inverse of the type used by Parkin & Brock (1981) with units L mg-1 cm-1. Let r = a/d, b = g/f, d =g/e πΆβπ1 = πΉ × π΄1 (1⁄π − π) × (1000⁄πΈπ₯π‘1 × π) (11) πΆβπ2 = πΉ × π΄2 (π − π) × (1000⁄πΈπ₯π‘2 × π) (12) where Ai = Measured absorbance at the peak of chlorophyll i. The factor of 1000 is to give chlorophyll concentration in mg L-1. References Aguirre-Gomez, R., A. R. Weeks, and S. R. Boxall. 2001. The identification of phytoplankton pigments from absorption spectra. Int. J. Remote Sensing 22:315-338 [doi:10.1080/014311601449952]. Caraco, N., and A. H. Puccoon. 1986. The measurement of bacterial chlorophyll and algal chlorophyll a in natural waters. Limnol. Oceanogr. 31:889-893 [doi:10.4319/lo.1986.31.4.0889]. Lorenzen, C. J. 1967. Determination of chlorophyll and pheo-pigments: Spectrophotometric equations. Limnol. Oceanogr. 12:343-346 [doi:10.4319/lo.1967.12.2.0343]. Moss, B. 1967 a. A spectrophotometric method for the estimation of percentage degradation of chlorophylls to pheo-pigments in extracts of algae. Limnol. Oceanogr. 12:335-340 [doi:10.4319/lo.1967.12.2.0335]. Moss, B. 1967 b. A note on the estimation of chlorophyll a in freshwater algal communities. Limnol. Oceanogr. 12:340-342 [doi:10.4319/lo.1967.12.2.0340]. Parkin, T. B., and T. D. Brock. 1981. Photosynthetic bacteria production and carbon mineralization in a meromictic lake. Arch. Hydrobiol. 91:366-382. Ritchie, R. J. 2006. Consistent sets of spectrophotometric chlorophyll equations for acetone, methanol and ethanol solvents. Photosynth. Res. 89:27–41 [doi:10.1007/s11120-006-9065-9].