This file was created by scanning the printed publication. Errors identified by the software have been corrected; however, some errors may remain. Stream Channel Characteristics under Natural and Grazed Conditions (continued) STREAM CHANNEL PROPERTIES The following is a listing of stream channel properties associated with this riparian type. Analysis employed follows methods outlined in Chapter 5 (ECODATA Data Bases and ECOPAC Analysis Software) of the_ Ecosystem Classification Handbook, U.S. Forest Service, Northern Region. Property Stream Channel Characteristics under Natural and Grazed Conditions Property Natural Conditions Under Prolonged Season Long Grazing 2-4 Unchanged Valley Bottom Gradient (%) <3 Unchanged Rosgen Classification C6 C6 to C3 or C4 Bankful Width (ft) 5 - 15 5 - >15 Depositional Features None Point Bars 1.5 - 2.0 1.3-1.8 Width/Depth Ratio 2.5 >3.0 Pool Embeddedness % Dominant Particle Size 70 50 S 30-60 FS Glide Embeddedness % Dominant Particle Size 27 40 S 75 - 80 20-50 FS Stream Order Sinuosity 3 Under Prolonged Season Long Grazing Riffle Em bedded ness % Dominant Particle Size 30 S 4 -10 10 - 30 SG Percent Undercut 80 40-80 Width Undercut (ft.) 1.1 .5 Stream Overhanging Plant Cover Trees Shrubs Herbs .5 .5 .5 0 .5 .5 - 10 .5 .5 100 0 .5 70 - 80 1-3 0 0 60 1-3 10 10 .5 .5 50 1-3 30 10 80-90 60-80 Streambank Plant Cover Trees Shrubs Herbs Streambank Ground Cover Bare Soil Gravel Rock Litter Wood Moss Basal Vegetation 10 - 20 Natural Conditions Percent Stable Banks 30 A METHOD FOR PHOTOSYNTHETIC CALIBRATION OF PROCESS MODELS FOR CONIFER ECOSYSTEMS A. Koehn and G. I. McDonald light compensation point, and the Michaelis-Menton constant for light. The Michaelis-Menton constant we refer to in this paper is not exactly the same as the MichaelisMenton constant of enzyme kinetics; rather it is the calculated value from nonlinear regression analysis. This poster synopsis describes procedures to estimate calibration parameters for the assimilation portion of a process-based forest ecology model known as Forest-BGC (Running and Coughlan 1988). Calibration will facilitate site-specific simulation of key system processes involving carbon, water, and nitrogen cycles. We describe a procedure using a Clark-type oxygen electrode system to make laboratory estimates of maximum mesophyll conductance, MATERIALS AND METHODS Data collected from two trees in February 1990 were used to illustrate calibration procedures. Tree 123 was a control tree, shaded only by the greenhouse structure (35 percent full sun), and tree 144 was from the shade treatment which received 20 percent of the light of the control treatment. A. Koehn is Ph.D. candidate at the University ofldaho, Moscow, ID. G. I. McDonald is Research Pathologist, U.S. Department of Agriculture, Forest Service, Intermountain Research Station, Moscow, ID. 244 was covered by the electrolyte, a 2 cm2 piece of cigarette paper, and a teflon membrane of the same size. The system was calibrated by injecting 1 cm3 of air into the chamber and recording the change in voltage (the capillary matting already in the chamber). The system calibration calculations were: Photosynthetic oxygen evolution rates were measured using the leaf-disc electrode system designed by Delieu and Walker (1981, 1983) and manufactured by Hansatech Instruments Ltd., England. The system consisted of a Clark-type electrode that measures oxygen polargraphically. Light was supplied by the Hansatech LS-2 unit consisting of a 100-watt photo lamp, a heat-reflecting mirror to reduce the infrared content of the emitted light, a system oflenses to produce a beam of light with low variation of intensity across the beam and little divergence from parallel, and three slots that accept 50-mm2 neutral density filters to give precise control of the desired light intensity. The lamp housing was cooled by a highoutput 12-v d.c. fan, which blows filtered air across the bulb and heat-reflecting mirror. Photon flux density of each light level was measured using an Omnidata Model ES-240 quantum sensor. Oxygen evolution was measured at 20 ± 1 °C and saturating CO2 (5 percent CO2), The CO2 concentration was controlled by a sodium carbonatelbicarbonatelborate buffer solution, which wets a capillary matting in the bottom of the chamber. Temperature control was provided by a controlled-temperature water circulator. Oxygen evolution was measured at eight different photon flux densities (PFD's): 30, 50, 95, 170, 230, 430, 820, and 1,500 J.1moleslm 2/s (full sun for the summer averages approximately 1,600 J.1moleslm 2/s). Dark respiration was measured with the lights off at the beginning of the sampling session. Five voltage readings were recorded with a Polycorder 700 data recorder in 300-microsecond intervals every 15 seconds for 3 minutes at each PFD and for dark respiration (fig. 1). The five voltage readings from each 15-second interval were averaged to provide one reading. Twelve readings were obtained over a 3-minute period at one PFD. The electrolyte used for the electrode was one part saturated KCL solution, one part 0.4 M borate buffer at pH 9.0, and two parts 1.0 M sodium bicarbonate adjusted to pH 9.0 with 1 M sodium carbonate solution. The electrode 1. correction for standard temperature and pressure: X = J.1moles Oil cm 3 of air at 20 °C. =9.37 (PlPo) (2731T); PlPo =exp (-A/8,500), (A = altitude in meters) = 9.37 (0.91) (273/293) = 7.94 J.1moles 0il cm 3 of air at 20 °C. 2. J.1moles 0lmv = 7.94 J.1moles O/mv during calibration. Oxygen evolution rates were calculated using linear regression on the data points for the 3-minute readings for each photon flux density (fig. 2). Electrode sensitivity to temperature changes that occur with increasing light intensity was compensated for by completing a blank (tissue absent) run over all PFD's. Difference between the slopes of the regression lines (fig. 2) was the rate of 02 evolved (or in the case of dark respiration, 02 uptake). Needle area was measured using a high-resolution monochrome TV camera, a PCVISIONplus Frame-grabber, and Java video analysis software. Micromoles of 0/m2/s for the needle sample was calculated as follows: 1. J.1moleslmv (value from calibration) * mv outputlleaf area =J.1moleslleaf area 2. corrected slope from regression of J.1moleslleaf area vs. time = J.1moles 0fleaf area/second 3. (J.1moles of 0fleaf area (mm 2)/sec) * 1,000,000 mm2/m2 = J.1moles of 02 evolvedlm2/s. At low photon flux densities (up to 95 J.1moleslm2/s), the rate of photosynthesis is directly proportional to PFD and quantum yield (photon yield) is constant and maximal (Bjorkman and Demmig 1987). Quantum yield is a measure of the efficiency with which light is converted to stable photosynthetic products. On the assumption that plants use the same photosynthetic pathways and are equally efficient in converting photons into chemically bound energy, one would expect them to have identical quantum yields as long as the functional integrity remains intact (Bjorkman and Demmig 1987). We mention quantum yield because it is a potential quantitative indicator of the effect of stress on the photosynthetic system. Quantum yield is equal to the slope of the photosynthetic rate vs. PFD at low light levels. The light compensation point and dark respiration are also derived from the same linear regression analysis (figs. 3 and 4). The method used to extract values of calibration parameters P and K from 02 evolution data was a nonlinear regressi;n analy~is. Enzfitter (Leatherbarrow 1987) is a nonlinear regression program designed to analyze enzyme kinetics. The model for the anaylsis was the MichaelisMenton enzyme kinetics equation and fit of actual to model was adequate (fig. 5). Photosynthesis values used in this analysis are net photosynthesis + dark respiration. 17.36 en .... ..J • 17.34 0 > ~ 17.32 ..J :E Z 17.3 • ..J « Z • • 17.28 CJ en 17.26 ..J ..J W 0 • 17.24 17.22 0 300 600 900 1200 TIME IN MICROSECONDS Figure 1-Five voltage readings shown in this graph illustrate the variation in the Polycorder 700 signal. 245 3000 2500 C W ~ 0 > w Z NEEDLES 2000 ~ 1 w CJ BlANK + > >< 0 O~~~--~--r-~--~--~~---r--'---'--'~ o 15 30 45 60 75 90 105 120 135 150 165 TIME IN SECONDS Figure 2-02evolution rate for a 3-minute period at one PFD is calculated from the difference in slope (J.unoles O.jm2/s vs. time) between needle and blank. Each data point is composed of the mean of five readings (fig. 1). These calculations are made for all nine PFD's (including dark respiration). - ~ (I) 20 18 '1 E 18 UJ W DARK RESPIRATION • 1.104 mlcroMOLES 02"'-1 S-1 O QUANTUM YIELD • .071 ..loroMOLEaIPHOTON 2 14 Y • .071X - 1.104 ..... 12 0 ::E e .si - 10 8 E 8 Z 4 ~ :l 2 0 ..... 0 > W ON COMPENaATION POINT. 15.48 mlcroMOlEa O2 m- 2 a- 1 0 -4 0 10 20 30 40 60 80 70 80 PHOTON FLUX (mlcroMOLES m-2s-1 ) Figure 3-Linear regression on the PFD's up to 95 J.UTl0les/m2/s calculates the light compensation point, quantum yield, and dark respiration. This graph shows the results for tree 123. 246 90 100 -cr ""'0 E tJ) W ..J 20 18 -2 -1 DARK RESPIRATION • 2.471 microMOLES 02m I 16 O 2 QUANTUM YIELD • .164 mlcroMOLES/PHOTON 14 Y • .164X - 2.471 12 0 :i 10 ~ 8 .. . 0 E z COMPENSATION POINT· 15.07mlcroMOLES 02m-2.-1 8 0 4 ..J 2 > W 0 i= => 0 0 C'II -2 -4~--~--~--~----~--~--~--~----~--~--~ o 10 20 40 30 50 60 70 90 80 100 quantum yield, and dark respiration. This graph shows the results for tree 144. PHOTON FLUX (microMOLES m-2s-1 ) 40 Z 36 i=, =>0 ..J(';I 30 0_ 01 >E WtJ) (';IW O..J 110 I-:i CJe =>0 * TREE 1« TREE 123 26 o2 • 20 V MAX • SUBSTRATE K M + SUBSTRATE 15 10 C·- 6 a. 0 OE a::- o Figure 4-Linear regression on the PFD's up to 95 J.l1Tloles/m 2/s calculates the light compensation point, '~""*'*"""""''''*''''''''''''''''''''''''''''''*'''''''' .............................................. * -6 0 200 400 600 800 1000 1200 1400 1600 = SUBSTRATE PHOTON FLUX (microMOLES m-2s-1) The anaylsis provides estimates of V (= P in the assimilation model) and K (= Micha~ns-Me~ton constant for light, the light intensity at 1/2 P mil:.)' Parameters derived from the laboratory measurement of 02 evolution-maximum photosynthesis (PMAX), the Michaelis-Menton constant for light (Km), dark respiration, and the light compensation point (fig. G)-were used to calibrate the photosynthesis assimilation model used in Forest-BGC. To calibrate the Forest-BGC assimilation equation, modifications were made as described elsewhere (McDonald these proceedings). The equation we used was: where: ICC Figure 5-Results of nonlinear regression used to calculate V max and ~ for the MichaelisMenton enzyme kinetics model. Values used here represent net photosynthesis + dark respiration. = internal CO2 concentration =59,259 ° ubars = 5 percent CO2 in 2 measurement cells MCC = maximum stomatal conductance 0.008 mls (Lohammer and others 1980) MMC = maximum mesophyll conductance PMAXlICC (Landsberg 1986) LMCS = Light-dependent mesophyll conductance scaler = (current light-light compensation point)/ (current light + Michaelis-Menton constant). Jlmoles CO/m 2/s = (ICC*MCC*MMC*LMCS)/ (MCC + MMC*LMCS); Jlmoles CO2 = 0.75 02 evolved 247 RESULTS AND DISCUSSION Since Forest-BGC assimilation is computed from this equation, the procedure described has the potential to calibrate the process model for specific species growing on specific sites with a specific growth history. These parameters taken singly or in combination may also provide useful quantitative indicators of system stress. Results of calibrating the assimilation model with data from the two different Douglas-fir seedlings are shown in figure 7. The calibrated model was then inserted into Forest-BGC.- Output from Forest-BGC after calibration for some assumed situations is shown elsewhere (fig. 6 in McDonald these proceedings). Photosynthesis values in this figure are net photosynthetic rates. Our calibration procedure, using the Hansatech 02 evolution cells, seems to be capable of providing the necessary parameters for the assimilation portion of Forest-BGC. Lohammer and others' (1980) equation appears to represent the actual data points (fig. 7). - ACKNOWLEDGMENTS This research is funded by Stillinger Funds from the University of Idaho and the Intermountain Research Station. 40 1(1) '1 E en 36 0 :E 26 W ..J * 30 ...0 20 E 16 * MICHAELIS-MENTEN. CONSTANT £ Z 0 10 -- i= ~ ..J 0 > W 0 MAXIMUM RATE OF PHOTOSYNTHESIS 5 SLOPE. QUANTUM YIELD LIGHT COMPENSATION POINT 0 DARK RESPIRATION N 1200 400 800 800 1000 1200 1400 1600 PHOTON FLUX (mlcroMOLES m-2s-1) - ... '(I) Figure 6-Photosynthetic parameters calculated from the 02 evolution data using linear and nonlinear regression techniques. 40 ~------------------------------------~-------------,40 - OF 144 MODEL o 144 ACTUAL '1 E en w 36 ..J 0 :E 25 25 E 20 20 - 16 15 --_. OF 123 MODEL 30 * 35 123 ACTUAL 30 £ E Z 0 i= ~ 10 }I~·-· 10 *-*...""-' .*.......... --_._.....*. - ..J 5 > W 0 ~------------------------------------------------------~o 6 0 0 N -6 L---~~--~----~----~----~----~----~----~-5 800 800 200 400 1000 1200 0 1400 1800 PHOTON FLUX (mlcroMOLES m-2s-1) 248 Figure 7-02 evolution for trees 123 and 144 plotted on calibrated assimilation model output. Values represent net photosynthesis.