General Allometric Equations for Rates of Nutrient Uptake, Ingestion, And Respiration in Plankton...

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NOTES Limnol. Oceanogr., 34(7), 1989, 1290-1299 0 1989, by the American Society of Limnology and Oceanography, Inc. General allometric equations for rates of nutrient uptake, ingestion, and respiration in plankton organisms Abstract-General allometric equations are de- rived for rates of nutrient uptake, ingestion, and respiration by plan ktonic organisms. Previous studies commonly calculated parameters a and b in the allometric equation H = aMb by linear regressions on log-transformed data. This prac- tice results in variability between data sets in estimates of both a and b, making meaningful comparisons difficult. This problem is overcome by assuming the mass-specific form of b to be -0.25, based on accumulated empirical evi- dence. Values of a arc then recalculated from published data, with log transformations and an assumed regression slope of -0.25. Resulting regressions predict values of a (in pg Co.25 d-l) at 20°C as follows: 3.6 for nutrient uptake by phy- toplankton and bacteria; 63 and 13 for ingestion and respiration by particle-feeding heterotrophs. It is hypothesized that organisms that take up dissolved nutrients from solution (autotrophs and osmotrophs, e.g. phytoplankton and bacteria) have lower specific respiration rates (i.e. smaller a) when compared with organisms (either uni- cellular or multicellular) that ingest particulate material. Body size is an important determinant of many physiological and ecological rates (Pe- ters 1983). Allometric equations have been derived inter alia for metabolic, respiration, ingestion, excretion, photosynthetic, and growth rates for a wide variety of organisms, ranging in size from viruses to large mam- mals (Fenchel 1974; Banse 1976; Blueweiss et al. 1978; Calder 1984). Allometric models are potentially useful in estimating ecolog- Acknowledgments We thank Peter Ryan, Charles Griffiths, Trevor Pro- byn, and Scott Turner for commenting on the manu- script, and Pierre Legendre, Rob Peters, Dave Caron, Peter Verity, and Les Underhill for helpful discussion. The comments of four anonymous referees improved the manuscript. This study forms part of the Systems Analysis Proj- ect of the Benguela Ecology Programme, funded by the South African National Committee for Oceanographic Research. ical flows in ecosystem studies, particularly because organism size is being used increas- ingly as a basis for characterizing marine plankton communities (Cousins 1985; Dickie et al. 1987). As a consequence of the many studies estimating allometric equa- tions, however, there are several different allometric models, often for the same pro- cess and group of organisms (see Table I). This multiplicity can lead to distracting ar- guments as to which model is “best” (Eco- nomos 19’79; Heusner 1982; Feldman and McMahon 1983), as well as making it dif- ficult to decide which model to use. Dis- crepancies among the values of allometric parameters may result in inconsistencies be- tween estimates of ecological flows, espe- cially if organisms over a wide range of body sizes are being considered. Rather than em- phasizing differences between models, there is a need to synthesize existing information and derive general allometric equations that highlight similarities in allometry and make the models useful for predictive purposes (Platt 198 5). This note aims to remove some of the sources of these discrepancies among pub- lished allometric regressions for planktonic organisms, using literature data to calculate allometric equations for a wide range of or- ganism sizes and a number of different pro- cesses. The equations developed here, how- ever, may not be the best predictors of physiological rates when a study is confined to only a narrow range of body size or to a single taxonomic group of organisms. A novel approach is adopted in fitting param- eters to allometric equations; it is assumed that the rate processes of organisms scale by the same, constant exponent with body masses, in keeping with theoretical and em- pirical evidence as to the power-form of the general allometric equation. Rate coeffi- 1290

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NOTES

Limnol. Oceanogr., 34(7), 1989, 1290-1299 0 1989, by the American Society of Limnology and Oceanography, Inc.

General allometric equations for rates of nutrient uptake, ingestion, and respiration in plankton organisms

Abstract-General allometric equations are de- rived for rates of nutrient uptake, ingestion, and respiration by plan ktonic organisms. Previous studies commonly calculated parameters a and b in the allometric equation H = aMb by linear regressions on log-transformed data. This prac- tice results in variability between data sets in estimates of both a and b, making meaningful comparisons difficult. This problem is overcome by assuming the mass-specific form of b to be -0.25, based on accumulated empirical evi- dence. Values of a arc then recalculated from published data, with log transformations and an assumed regression slope of -0.25. Resulting regressions predict values of a (in pg Co.25 d-l) at 20°C as follows: 3.6 for nutrient uptake by phy- toplankton and bacteria; 63 and 13 for ingestion and respiration by particle-feeding heterotrophs. It is hypothesized that organisms that take up dissolved nutrients from solution (autotrophs and osmotrophs, e.g. phytoplankton and bacteria) have lower specific respiration rates (i.e. smaller a) when compared with organisms (either uni- cellular or multicellular) that ingest particulate material.

Body size is an important determinant of many physiological and ecological rates (Pe- ters 1983). Allometric equations have been derived inter alia for metabolic, respiration, ingestion, excretion, photosynthetic, and growth rates for a wide variety of organisms, ranging in size from viruses to large mam- mals (Fenchel 1974; Banse 1976; Blueweiss et al. 1978; Calder 1984). Allometric models are potentially useful in estimating ecolog-

Acknowledgments We thank Peter Ryan, Charles Griffiths, Trevor Pro-

byn, and Scott Turner for commenting on the manu- script, and Pierre Legendre, Rob Peters, Dave Caron, Peter Verity, and Les Underhill for helpful discussion. The comments of four anonymous referees improved the manuscript.

This study forms part of the Systems Analysis Proj- ect of the Benguela Ecology Programme, funded by the South African National Committee for Oceanographic Research.

ical flows in ecosystem studies, particularly because organism size is being used increas- ingly as a basis for characterizing marine plankton communities (Cousins 1985; Dickie et al. 1987). As a consequence of the many studies estimating allometric equa- tions, however, there are several different allometric models, often for the same pro- cess and group of organisms (see Table I). This multiplicity can lead to distracting ar- guments as to which model is “best” (Eco- nomos 19’79; Heusner 1982; Feldman and McMahon 1983), as well as making it dif- ficult to decide which model to use. Dis- crepancies among the values of allometric parameters may result in inconsistencies be- tween estimates of ecological flows, espe- cially if organisms over a wide range of body sizes are being considered. Rather than em- phasizing differences between models, there is a need to synthesize existing information and derive general allometric equations that highlight similarities in allometry and make the models useful for predictive purposes (Platt 198 5).

This note aims to remove some of the sources of these discrepancies among pub- lished allometric regressions for planktonic organisms, using literature data to calculate allometric equations for a wide range of or- ganism sizes and a number of different pro- cesses. The equations developed here, how- ever, may not be the best predictors of physiological rates when a study is confined to only a narrow range of body size or to a single taxonomic group of organisms. A novel approach is adopted in fitting param- eters to allometric equations; it is assumed that the rate processes of organisms scale by the same, constant exponent with body masses, in keeping with theoretical and em- pirical evidence as to the power-form of the general allometric equation. Rate coeffi-

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Notes 1291

cients for each process are then calculated. This procedure avoids the problem of ob- taining dissimilar estimates of the two al- lometric parameters for different data sets and allows comparisons to be made be- tween rate coefficients for different allo- metric processes.

The earliest work in quantifying allome- tric processes was done chiefly on body size- metabolic rate relationships (e.g. Kleiber 1932; Brody et al. 1934; Hemmingsen 1960). These and subsequent studies found that a simple power function best described the relationship; the general allometric equa- tion has the form

R=aMb (1) where R can be one of many rates, M is body mass, a is the rate coefficient, and b is the scaling parameter. R has dimensions [time(t)]- l for mass-specific rates, A4 has di- mensions [mass (A4) 1, and b is dimension- less, therefore a has dimensions (t)-1(A4-b. (See list of symbols and abbreviations.)

There is considerable debate as to the “true” value of b. Several theoretical expla- nations have been proposed to explain al- lometry (Peters 1983), and attempts have been made to derive b theoretically, initially from the now discredited surface law (see Schmidt-Nielsen 1970) but more recently from the results of dimensional analysis and the theory of biological similitude (Gunther 1975; Economos 1979; Platt and Silvert 198 1; Heusner 1982). The latter studies are based on the theorem that all natural laws can be expressed as relationships between dimensionless quantities (Stahl 1962). Us- ing this theorem, Heusner (1982) calculated a value of -0.33 for b as a mathematical consequence of homomorphism, but Platt and Silver-t ( 198 1) calculated values of - 0.3 3 for aquatic organisms and -0.25 for ter- restrial organisms. Empirical evidence, however, is divided (Table 1). Some studies indicate a value of -0.25 for both aquatic and terrestrial organisms (e.g. Fenchel 1974; Blueweiss et al. 1978), whereas other studies indicate a value of -0.33 (e.g. Baldock et al. 1980; Banse and Mosher 1980). In the absence of consensus as to the true value of b or its underlying theoretical basis, the val- ue supported best by real data should be

Symbols and abbreviations

a

a,

b

Rate coefficient in allometric equation, pg CO25 d-1

Allometric coefficients for rates of inges- tion (a,), production (a,), and respira- tion (a,), pg Co 25 d-l

Exponent in allometric equation, dimen- sionless

GGE I I Inax M MNGE N

Gross growth efficiency Ingestion rate, d-l Maximal ingestion rate, d-l Organism mass, pg C Maximum net growth efficiency Total number of data points for each rate

process n Number of data points from single data

source NGE Net growth efficiency R Rate variable, d-l R, Respiration rate of particle-feeding hetero-

trophs, d-l RF

u’ V V max P

Respiration rate of phytoplankton and bacteria, d-l

Assimilation efficiency, d-l Nutrient uptake rate, d-l Maximal nutrient uptake rate, d-l Growth rate, d-l

used (Lavigne 1982). Estimated values of b range between about -0.1 and -0.4 (see Peters 1983). Most values of b are close to -0.25 (Lavigne 1982; Calder 1984) how- ever, and we decided to use a value of - 0.25 for b in all calculations described below.

Most studies have been primarily con- cerned with estimating b, with little atten- tion being paid to a (Platt 1985). Literature estimates of a are influenced by the corre- sponding estimates of b, because of the prac- tice of estimating these two parameters si- multaneously (by using linear regressions on log/log-transformed data). To avoid this problem, we extracted appropriate data from the literature, body masses and rate pro- cesses were log-transformed, and regression estimates of a were calculated assuming a value of b of -0.25.

Data were obtained from a number of sources, in some cases secondhand, having been converted from different units and temperatures by others. Some data were ob- tained from figures, which may have re- sulted in some error in estimation, espe- cially because axes are usually logarithmic. Calculations were done to two significant figures throughout. Units were not always

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1292 Notes

Table 1. Allometric equations for rates of growth, ingestion, and respiration of different groups of organisms. Parameters a and b were converted to values compatible with carbon masses (pg C) and mass-specific rates (d-l) at 20°C.

Organisms a b

Growth Virus-mammals Virus-mammals Ciliates and amoebae Ciliates Copepod

Ingestion Marine amphipod Detritivores Invertebrates

Respiration Rat-steer Mouse-elephant Bacteria-mammals Marine plankton Unicellular algae Marine amphipod Daphnia Zooplankton Crustacea Copepod

20 -0.25 Fenchel 1974 16 -0.26 Blueweiss et al. 1978 9.4 -0.3 11 Baldock et al. 1980

12 -0.247 Taylor and Shuter 198 1 9.2 -0.15 Ross 1982a

68 -0.25 Dagg 1976 76 -0.258 Cammen 1980 54 -0.306 Capriulo 1982

- - -

33 0.4

12 10 15 16 17

-0.25 Kleiber 1932 -0.266 Brody et al. 1934 -0.25 Hemmingsen 1960 -0.309 Ikeda 1970 -0.10 Banse 1976 -0.225 Dagg 1976 -0.15 Lampert 1977 -0.312 Ikeda and Motoda 1978 -0.268 Ivleva 1980 -0.25 Ross 1982a

comparable among studies. Where neces- sary, data were converted to standard units of mass (pg C) and specific rates (d- ‘) with the conversions presented in Table 2. The respiratory quotient (RQ) (Table 2) was as- sumed to equal one (Parsons et al. 1977) because most of the respiration data were for unstarved animals (Ikeda 1970; Ross 1982a; Fenchel and Finlay 1983). Hourly rates were converted to daily rates by mul- tiplying by 24, and all data were standard- ized to 20°C with Q10 values from the ap- propriate sources (see below). Where practical, data were combined into a single set. Often the raw data were not readily available (not presented or difficult to ex- tract from graphical representations). When this problem occurred and the published ex-

ponent was close to -0.25, the published rate coefficients were compared to the ones calculated below. Data sources are de- scribed in detail below and summarized in Table 3.

Bacteria and phytoplankton are grouped together here because both take up dis- solved nutrients from solution (Azam et al. 1983); they are distinguished from particle- feeding heterotrophs. Growth rates (p) of phytoplankton and bacteria are often lim- ited by nutrient availability (McCarthy 198 1; Laake et al. 1983a). Uptake rates (v) of the limiting nutrient therefore may be equated approximately to growth rates on an ecological time scale. Data for calculated maximum values of V and p with corre- sponding cell sizes were used to estimate the

Table 2. Conversions used to standardize all body mass data to units of pg C. Respiratory quotient--Q (see text).

Conversion Reference

1 pm3 = 1 wet pg Fenchel and Finlay 1983 1 pg dry = 0.4 C pg Peters 1983 1 pg wet = 0.07 C pg Peters 1983

1pgC=1p102x 12+22.4xRQ Parsons et al. 1977 1 nJ = 0.05 pl 0, Peters 1983

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Notes 1293

uptake coefficient

in the

allometric

equa- tion. Cell dim

ensions (pm

) and maxim

al spe-

cific growth

rates (d-l) for

four strains

of bacteria

(n =

4) at 2°C were taken

from

tables 1 and 3 of Laake et al. (1983b).

Cell volum

es were estim

ated with

the formula

for a cylinder

and converted

to carbon

masses with

the relationship 1 pm

3 = 0.12 1 pg C (Laake et al. 1983b). G

rowth rates were

standardized to 20°C with

a Q10 of 2.45. In

pure cultures,

bacterial isolates

of these

strains followed

the Arrhenius curve

from

5°C to > 15°C (Laake et al.

1983b), so the

extrapolation to 20°C is justified.

Cell car-

bon (pg C) and specific

growth rates (h-l)

for unicellular algae (n = 14) were read from

figure 1 of Banse (1976), who used data from

a num

ber of sources and standardized

them

to 20°C. Cell carbon

(pg C) and m

aximal

specific growth

rates (h-l)

for freshwater

green algae (n = 26) were similarly

read from

figure 1 of Schlesinger et al. (198 1). All these

data span a size range from

0.3 to loo-pm

esd (equivalent spherical

diameter)

and were com

bined into

a single data set (N = 44) for param

eter estim

ation (Table

3). Data from

Taguchi (1976)

for specific phytosynthetic

rates of marine

diatoms,

converted to 20°C

with a Q

lo of 2.0, were an order of m

agni- tude faster than those for sim

ilar-sized phy-

toplankton cells in the data sets described

above and therefore were om

itted from

the

regression. M

aximal

specific ingestion rates have been

shown to decrease with increasing

body size both

within species (Dagg

1976) and

be- tween

species (Fenchel

1980; Paffenhiifer

197 1; Ikeda 1977;

Ross 1982~;

Capriulo 1982).

Maxim

al ingestion

rates (h-l) and

cell volumes

(pm’)

for 17 species of ciliates

at 20”-22°C (n = 18) were read from

figure

2 of Fenchel(l980). Daily

rations and body

masses (pg C) for the copepod

Calanus hel- golandicus at 15°C (n = 5) were taken from

table 5 of Paffenhijfer

(197 l), and rates were standardized

to 20°C with a Q

lo of 3.0 (Ross 1982a). M

aximal

daily rations

(d-l) and dry

masses (pg) for

five species of m

arine co-

pepod at 20°C (n = 24) were obtained from

table

2 of Ikeda (1977).

Ingestion rates (pg

C d-l) and body

masses (pg C) for the eu-

phausiid Euphausia pac$ca

at 12°C (n =

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1294 Notes

27) were read from figure 2 of Ross (1982a) and standardized to 20°C with a Qlo of 3.0 (Ross 1982a). All these data were combined into a single data set (N = 74) with ingestion rates for body sizes ranging from 8- to 4,450- pm esd (Table 3).

Banse (1982) presented allometric equa- tions for respiration rates of unicellular or- ganisms from data of Hemmingsen (1960) (for procaryotes and eucaryotes combined) and Dewey (1976) (for eucaryotes). These equations yielded estimates for b of -0.24 and -0.26 respectively-very close to the value of -0.25 assumed here. The mean (1.7) of the two estimated values of a (1.54 and 1.89) was therefore used as the respi- ration rate (RV) coefficient for phytoplank- ton and bacteria.

Data for respiration rates (R,) and body masses of particle-feeding heterotrophs over a wide range of body sizes were taken from the literature and combined into one data set (see Table 3). Respiration rates (nl 0, cell-l h- ‘) and cell volumes (pm’) for grow- ing free-living protozoa at 20°C (n = 48) were extracted from table 1 of Fenchel and Finlay (1983) and converted to standard units of mass and specific rates. An addi- tional 14 data points were obtained from table 1 of Caron et al. (1989), who also pre- sented the data of Fenchel and Finlay ( 19 8 3). Respiration rates (pg C d- l) and body masses (pg C) for the euphausiid E. pacz$ca at 12°C (n = 92) were read from figure 2 of Ross (1982a), and a Qlo of 2.0 (Ross 1982a) was used to convert the rates to 20°C. Respi- ration rates (~10, d- ‘) and dry masses (mg) for marine plankton (n = 103) were ob- tained from table 3 of Ikeda (1970). The measurements were made at temperatures ranging from 5.1” to 30.3”C; they were stan- dardized to 20°C with a Qlo of 2.0 (Ross 1982a). Specific respiration rates &l O2 mg- 1 h- l) and body masses (mg wet) for 27 species of marine copepods were taken from table 1 of Gaudy and Boucher (1983) and con- verted to 20°C with their Qlo of 2.14. These five data sets (N = 284) cover a range of body sizes from 5- to 4,600-pm esd (Table 3).

Body masses and rate variables were log- transformed. Thus the form of the allo- metric Eq. 1 becomes

log[rate] = log a + b log M. (2)

An a priori assumption was made that b was equal to - 0.25, and a was calculated by substituting b = -0.25 and the mean values of log(rate) and log M into Eq. 2, assuming that the regression passes through the means of both variables as for ordinary least-squares regressions (Zar 1984). This procedure probably does not give the best statistical regression line through the data points, but it is believed that it provides the best estimates of the rate coefficients a in the allometric models that have been pro- posed, where b is set at -0.25. The variation that is explained by the “forced” regression lines was investigated by estimating coeffi- cients of determination (r2) between the lines of -0.25 slope and the data points (Zar 1984).

Estimated allometric equations of slope - 0.25 are presented in Table 4. The esti- mated rate coefficient for uptake rates of phytoplankton and bacteria Vmax is an order of magnitude smaller than that for ingestion rates I,,, of particle feeders (Table 4). Sim- ilarly, the rate coefficient for phytoplankton and bacterial respiration rates (R,) is much smaller than the coefficient for respiration rates of particle-feeding heterotrophs (RI).

There is much scatter about the regres- sions for rates of uptake (Fig. l), ingestion (Fig. 2) and respiration of particle-feeding heterotrophs (Fig. 3). The scatter is partially due to natural variability; not all organisms are exactly alike, and cells in different phys- iological states will have different reaction times for physiological processes (see Fen- chel and Finlay 1983). Some of the vari- ability is also probably due to measurement error and errors in estimating body carbon with general conversions (Table 2). For ex- ample, in Fig. 3 most of the protozoan data appear to lie below the regression line. This offset can be attributed to underestimating body carbon when converting from vol- umes because a simple linear conversion was used (Table 2), whereas a nonlinear conversion would probably be more appro- priate, as has been found for phytoplankton cells (e.g. Strathmann 1967). Fenchel and Finlay (1983), using different units for or- ganism size, have shown that there are no

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Notes 1295

Table 4. Allometric models for maximal nutrient uptake rates (V,,,,,) of phytoplankton and bacteria, and maximal ingestion rates (I,,,) and respiration rates (R,) of particle-feeding heterotrophs. The equation for res- piration rates of phytoplankton and bacteria (R,,), modified from Banse 1982, is also presented. Units of a are pg Co 25 d-l. Values of r2 were calculated for the variation of data points about the line of slope -0.25.

Equation N

V,,,,, (d-l) = 3.6 A4 (pg C)-O 25 44 0.77 Z,,,,, (d-l) = 63 M (pg C))O 25 74 0.85

R, (d-l) = 14 M (pg C)-Oz5 284 0.43 R, (d-l) = 1.7 M(pgC))025 - -

significant differences between the allome- tric relationships for respiration rates of particle-feeding protozoan and metazoan invertebrates. Similar conversions are used by most workers (e.g. Finlay 1977; Banse 1982; Fenchel and Finlay 1983; Peters 1983) because it is not always possible to take measurements in units that are useful for ecological interpretation and the same lim- itations and potential sources of error prob- ably apply to many physiological studies. Despite this problem, the forms of the al- lometric relationships remain remarkably consistent, giving some confidence in the “average” rate constants calculated here.

When allometric equations calculated by previous studies are compared (Table l), it is evident that there is not always agreement between parameter estimates. This dispar- ity is expected, taking into account potential sources of error in measurements and con- version factors used by most workers as well as statistical problems related to small sam-

Body mass(pg C)

Fig. 1. Allometric model describing the size de- pendence of maximal specific uptake rates (I’,,,) of phytoplankton and bacteria. The line passes through the centroid of the data (geometric means) and has a fixed slope of -0.25. Details given in text and Table 4.

- 1021 1 ‘; 0 al H 10' 6 .- iii % .G 10° 3 E 'R r"

10“

;+;+

+ +

- . . ..-1 . . ..“.I . ---“-I - -..-., . ..-“1 . ..“-a . 1 . ‘rm(

10' IO2 lo3 lo4 lo5 lo6 lo7 lo8 log 1o'O

Body mass(pg C)

Fig. 2. As Fig. 1, but for maximal specific ingestion rates (ImaX) of particular-feeding heterotrophs.

ple sizes and small mass ranges (Calder 1984). These factors confound the problem of deciding which allometric model is ap- propriate for use in mass budgets and energy balance equations in ecological studies of plankton communities. Complications in applying allometric models arise from the fact that allometric equations for different rate processes for the same group(s) of or- ganisms often have different values for the exponent b (Table 1). For example, the model of Capriulo ( 1982) for ingestion rates of invertebrates has an exponent of - 0.306, and the model of Ivleva (1980) for respi- ration rates of crustaceans has an exponent of -0.268. For two animals with body masses of 10 and lo6 pg C, these models predict maximal specific ingestion rates of 27 and 0.39 d- * and specific respiration rates of 8.6 and 0.2 1 d- *. Percentage respiration relative to ingestion for the smaller species is thus 32% and for the larger one 54%, with this difference becoming larger as the size difference increases. This disparity implies that growth and respiration do not change

lo*

Bodymass(pgC)

Fig. 3. As Fig. 1, but for specific respiration rates (R,) of particle-feeding heterotrophs.

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1296 Notes

among species in the same fashion with body size, which is unrealistic because growth ef- ficiencies are generally size invariant from species to species (Humphreys 1979).

It should be noted that these arguments do not apply to ingestion, respiration, and growth efficiencies within species, because changes in physiological relationships dur- ing growth result in characteristic growth curves within individual species. By stan- dardizing the value of b to - 0.25 in this study, this unrealistic source of interspecific variation has been removed. A similar pro- cedure was advocated by Smith (1984) to analyze allometric data. He discussed a number of problems associated with allo- metric techniques and suggested some al- ternative methods, including a priori models (e.g. setting the exponent to a constant val- ue) instead of a posteriori ones derived sole- ly from the data.

Values of rate coefficients for particle feeders calculated in regressions in Table 4 can be compared with literature values (es- timated from data not used in the regres- sions) after they have been converted to standard units and a temperature of 20°C. These values are all associated with expo- nents of (or very close to) -0.25. The rate coefficient for ingestion rates was estimated to be 66 (pg Co.25 d- ‘) by Dagg (1976) for a marine copepod, 54 (pg Co.25 d-l) by Ca- priulo (1982) for a range of invertebrates, and 82 (pg Co.25 d- ‘) by Cammen (1980) for benthic deposit feeders and detritivores. The second value was associated with an expo- nent of -0.306, and the value of a would increase above 54 if the value of b is - 0.25. Our estimate of 63 (pg Co.25 d- l) is com- parable to these estimates. The rate coeffi- cient for respiration rates of particle feeders was estimated to be 14 (pg Co.25 d- *) (Table 4). Values of 13.7 (pg Co.25 d-l) for poikilo- therms (Banse 1982) and 16 (pg Co.25 d-l) for crustaceans (n = 247) (Ivleva 1980) are similar to this estimate.

Values of rate coefficients (a) are impor- tant in ecological models and mass budgets. Relative magnitudes of a for different pro- cesses affect growth efficiencies.. Compari- sons of relative values of a (calculated in this study) with theoretical and measured growth efficiencies make it possible to assess

how realistic the calculated values are. For the discussion below, only organisms grow- ing at maximal rates are considered because intraspecific growth efficiencies change as individuals age, usually peaking and then decreasing as organisms reach maturity (Parsons et al. 1977). Therefore, all rela- tionships described are for maximal rates and are intended for use in interspecific comparisons among a large size range of organisms. In growing organisms, a sub- stantial proportion of the daily carbon mass balance is composed of ingestion and res- piration:

production = ingestion - respiration. (3)

All three processes are body-size-depen- dent. Equation 3 can be rewritten in allo- metric terms:

apMb = a,Mb - a,Mb. (4) If it is assumed that the scaling parameter b is the same for all rates for organisms growing maximally, it follows that the rate coefficient for production (a,) depends on the difference between the rate coefficients for ingestion (a,) and respiration (a,):

ap = a, - aR. (5)

Values of a for rates of uptake and res- piration (Table 4) can be substituted into Eq. 5. Therefore, for a phytoplankton or bacterial cell growing under optimal con- ditions at 20°C in the absence of grazing, maximal net carbon production will be (3.6 - 1.7) f 3.6 = 53% of gross carbon pro- duction, i.e. maximum net growth efficiency (MNGE) for carbon will be 53%. This es- timate is slightly lower than values based on theoretical arguments; Fenchel and Fin- lay ( 1983) propose that MNGE should be 67% for procaryotic microorganisms, and Penning de Vries et al. (1974) theoretically derive general MNGE values between 60 and 70% for autotrophs. These relation- ships are appropriate for cells growing op- timally, and net growth efficiency (NGE) will decrease as conditions become suboptimal. Measured NGE values for bacteria growing on various substrates range from 26 to 70% (Lucas 1986), and phytoplankton respira- tion is generally accepted as constituting

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Notes 1297

some 10-45% of photosynthesis (Raymont 1980) which includes values estimated with Eq. 5.

For grazers and predators similar calcu- lations can be made, although efficiencies of heterotrophs should be larger than those of autotrophs because autotrophs incur ex- tra metabolic costs in assembling organic monomers from their inorganic constitu- ents (Calow 1977). Particle-feeding hetero- trophs grazing optimally with abundant food supply have MNGE values for carbon cal- culated as

MNGE=l-R’ U’I a,Mb

=I-----

U ‘a,Mb (6)

where u’ is assimilation efficiency. Because body mass terms in allometric equations for R, and Z cancel, the equation reduces to

MNGE=l -% U’al ’ (7)

Substituting values of a, and aR (Table 4) and Eq. 7 and assuming U’ = 90% (Barthel 1983; Miller and Landry 1984) we assume MNGE is size-independent and has a value of 75% for particle-feeding heterotrophs growing optimally at 20°C. This value is larger than that calculated for autotrophs and bacteria in keeping with the prediction of Calow (1977). He estimated that “the best possible efficiency” that can be ex- pected from any growing heterotroph is be- tween 70 and 80%, which theoretical range includes the value estimated here. These theoretical estimates are also supported by measured values. Ross ( 19823) measured NGE values of up to 74% for larval stages of E. paciJica. The copepod Eurytemora af- finis was predicted to have a gross growth efficiency (GGE) of 60% when growing at 15°C (Ikeda and Motoda 1978) and max- imum GGE for Daphnia pulex was esti- mated to be 60% at 20°C (Sushchenya 1970). If we assume 90% assimilation efficiency, these GGE values are equivalent to NGE values of 67%.

It has frequently been stated that respi- ration rates for similarly sized unicells and multicellular poikilotherms differ by a fac-

tor of eight or nine (Hemmingsen 1960; Banse 1982) with unicells believed to have slower rates. In this study, two different al- lometric equations for respiration rates have been presented. One was obtained from the literature and can be applied to unicellular phytoplankton and bacteria (Table 4). The other was calculated from combined data of unicellular ciliates and marine inverte- brates (Table 4; Fig. 3). These equations thus do not conform to the usual unicell-multi- cell division. The grouping of ciliate respi- ration rates with those of other unicellular organisms has been questioned by Fenchel and Finlay (1983) because most of the cil- iate rates were faster than predicted for uni- cells. After selecting only those data for ac- tively growing ciliates, Fenchel and Finlay showed that the ciliate line is similar to that calculated by Hemmingsen (1960) for mul- ticellular organisms.

Ciliate assimilation rates can be calculat- ed from ingestion rates Z,,, (Table 4) with the calculated rate coefficient (a = 63) and an assumed assimilation efficiency of 80% (Stoecker 1984). If we adopt the “unicell” respiration equation with a coefficient of 1.7 (Table 4) NGE is calculated from Eq. 7 to be 97%-an impossibly large value; Calow ( 19 7 7) predicted theoretical maximum ef- ficiencies of 90-95%. Fenchel (1980) ques- tioned the application of a “unicell” respi- ration rate to ciliates by Laybourn and Finlay (1976) because their estimates were an order of magnitude too small. Therefore, when the mass balance of organisms is taken into account, it is clearly unrealistic to describe all unicell respiration rates by a single uni- cell respiration model.

Based on the analyses described above, we propose that respiration rates for plank- tonic organisms be distinguished on the ba- sis of method of food uptake. On the one hand, organisms that rely chiefly on dis- solved nutrients from solution (e.g. phyto- plankton and bacterioplankton) conform to the traditional unicell model and have slow- er respiration rates than similar-sized or- ganisms that feed mainly on particulate ma- terial. On the other hand, unicellular predators such as microflagellates and cil- iates have fast respiration rates, similar to the size-specific rates observed for multi-

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1298 Notes

cellular animals. They are therefore grouped with other particle feeders. This grouping resolves the problem of apparently unreal- istically large net growth efficiencies of cil- iates and is consistent with the hypothesis that maximal net growth efficiencies for or- ganisms grazing under optimal food con- ditions, whether ciliates or copepods, re- main constant (Humphreys 1979).

The allometric models developed here are not intended to replace earlier models in predicting rates of nutrient uptake, inges- tion, and respiration for planktonic organ- isms. When allometric models are used to estimate a number of material (or energy) flows for a wide size range of planktonic organisms, however, consistency is required between estimates of the scaling parameter b for the different processes. In such cases, it is believed that the models in Table 4 are preferable to others in which the allometric scaling parameter b differs, and these stan- dardized models should be used together in community and ecosystem studies.

Coleen L. Maloney John G. Field

Marine Biology Research Institute University of Cape Town Rondebosch 7700, South Africa

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Submitted: 17 June 1988 Accepted: 28 June 1989 Revised: 7 August 1989