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Applied and Environmental Microbiology, September 2007, p. 5875-5884, Vol. 73, No. 18
0099-2240/07/$08.00+0 doi:10.1128/AEM.00670-07
Copyright © 2007, American Society for Microbiology. All Rights Reserved.

Department of Chemical Engineering and Material Science,1 Department of Viticulture and Enology, University of California, One Shields Avenue, Davis, California 956162
Received 23 March 2007/ Accepted 28 June 2007
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These three variables are well-known critical factors for determining the kinetics of wine fermentations. Ough and Amerine performed extensive studies to characterize the effects of temperature on cell growth, sugar utilization, and ethanol production (25, 26). Others have studied yeast (Saccharomyces cerevisiae) sensitivity to ethanol at various temperatures (22, 27, 28). In addition, insufficient nitrogen has been well documented as an important factor that leads to stuck and sluggish fermentations (1, 2, 5, 14, 15, 20). Ough also studied the combined effects of initial nitrogen concentration and temperature on fermentation rates (23), while still others have studied the combined effects of initial sugar concentration, temperature, and pH on fermentation (9, 24). Overall, these works present a plethora of data that support the importance of understanding the effects of temperature and initial nitrogen and sugar concentrations on wine fermentation and that supply ample qualitative evidence of how each variable affects the overall rate of fermentation (sugar utilization). However, none of these previous studies presented a comprehensive model that includes all three of these variables and that can consistently predict problem fermentations.
Several physical and mathematical models have been developed for predicting wine fermentation kinetics. One of the first mechanistic models of enological fermentations that incorporated the relevant state variables, such as sugar concentration and temperature, was developed by Boulton in 1980 (7). Caro et al. also developed a similar mechanistic model for grape must fermentation which took into account other microbial functions, such as respiration and synthesis of products other than ethanol (8). Nanba et al. developed a kinetic wine fermentation model that incorporated yeast sensitivity to ethanol and temperature effects of yeast cell growth parameters (21). Other researchers have also developed more empirical models within an enological context (4, 13, 16). However, none of these models have been shown to acceptably predict problem fermentations with respect to temperature and initial conditions. A more comprehensive review of these models, along with others, can be found in the work of Marin (19).
One problem with the aforementioned mechanistic models is that the chosen limiting nutrient for cell growth was sugar. Substantial evidence has shown a strong link between nitrogen and yeast growth (2, 14, 20, 23), and a proven method for avoiding certain sluggish or stuck fermentations has been the addition of nitrogen sources (5). Therefore, the inclusion of nitrogen as a component for yeast growth is critical in a model aimed at predicting problem fermentations. The first enological model to include a nitrogen-limited cell growth mechanism was developed by Cramer et al. (11). Malherbe et al. also developed a model that incorporated nitrogen-limited growth (18). However, neither of these models successfully incorporates the effects of temperature in a manner that allows the prediction of sluggish and stuck fermentations.
Here we elaborate on the model previously presented by Cramer et al. (11) by including the effects of temperature. This model consists of five coupled ordinary differential equations (ODEs) that are combined with four one-dimensional regression models (describing the effects of temperature on three temperature-dependent model parameters and initial nitrogen conditions on one model parameter) to accurately predict the variation of sugar utilization for different temperatures and different initial concentrations of sugar and nitrogen. This is the first comprehensive model that predicts a transition from sluggish to normal to stuck wine fermentations with respect to increasing temperature.
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-amino nitrogen data were collected for one of each replicated pair of experiments by using procedures described below.
Fermentations and juice preparation.
For all fermentations, diluted Chardonnay juice was used, with sugar and nitrogen added back to appropriate levels. The purpose of diluting the juice was to create a medium where sugar and nitrogen levels could be manipulated, but all other nutrients were equal throughout the experiments. The juice was from the 2002 vintage and was supplied by Beringer Blass Wine Estates (Napa, CA) from a vineyard in Sonoma County, CA. The juice had the following measurements: °Brix, 25.4; titratable acidity, 7.5 g/liter; pH, 3.35; ammonia, 111 mg N/liter; and
-amino nitrogen concentration, 172 mg N/liter. Sulfur dioxide was added to the juice at 50 mg/liter. A yeast nutritional supplement (Superfood; The Wine Lab, Napa, CA) was also added to the juice at 500 mg/liter just prior to making dilutions.
In order to obtain the previously mentioned juice conditions, juice was diluted 3:1 (3 parts water or stock solutions to 1 part juice) to a total of 400 ml in a 500-ml Erlenmeyer flask. Sugar was added back by means of a 550-g/liter stock solution composed of 50% glucose (Sigma Chemical Company, St. Louis, MO) and 50% fructose (Sigma Chemical Company, St. Louis, MO) dissolved in sterile, filtered, deionized water. Nitrogen was added by means of a stock solution consisting of 10 g/liter diammonium phosphate (DAP; Sigma Chemical Company, St. Louis, MO). Fermentation flasks were made up to 400 ml with sterile deionized water.
The yeast used in all fermentations was Premier Cuvee (Red Star, Milwaukee, WI). Fermentations were performed in temperature-controlled incubators with shaker tables set at a constant 120 rpm. Temperature and agitation levels were maintained throughout the fermentation. Fermentations were monitored until the normal sugar and normal N flasks reached a constant sugar level for at least 2 days (300 to 800 h, depending on the temperature).
Fermentation sampling procedures.
Samples (approximately 3.5 ml/sample) were taken at appropriate times. Three milliliters of the sample was filtered through a 0.45-µm syringe filter into a 5.0-ml sterile test tube with a sealing cap and was frozen for later analysis. The remainder of the sample was used immediately for obtaining total cell count and viable cell count as well as for obtaining an optical density reading.
Viable and total cell concentration procedures.
For determining total and viable cell counts, a Bright-Line hemacytometer (Hausser Scientific, Horsham, PA) was used under a Zeiss light microscope at x400 magnification. A 100-µl sample was diluted with water such that when a final dilution with methylene blue at a 1:1 ratio was made, the final dilution would give a minimum of 100 cells and a maximum of 400 cells in the counting area of the hemacytometer. Samples were mixed on a vortex mixer at each stage of the dilution. The methylene blue used was 0.02% wt/vol in a citrate buffer. Cells were allowed to be in contact with methylene blue for at least 1 min, but not more than 5 min. Blue cells were counted as dead, and noncolored cells were counted as live. Five of the 25 squares in the hemacytometer grid were counted, and the result was multiplied by 5 to give a total count. Except for early in the fermentation when the cell number was very low, a minimum of 100 cells were counted. When time permitted, replicate counts were made using the chamber on the opposite side of the hemacytometer. Each cell count was converted to grams per liter of cell mass, assuming that each cell weighs 4 x 10–11 g and that the 25 squares in the hemacytometer grid were covered with 10 µl. Based upon replicate flask experiments, the standard deviations of total cell mass and viable cell mass estimates were a maximum of 0.63 g/liter and 0.48 g/liter, respectively, with a significantly smaller replication error found during the exponential growth phase (approximately the first 100 h), closer to 0.005 g/liter.
High-pressure liquid chromatography analysis for sugars and ethanol.
Samples were analyzed by high-pressure liquid chromatography for glucose, fructose, and ethanol (30). The system used was a Hewlett-Packard 1100 series with two HPX-87H columns (Bio-Rad; catalog no. 125-0140) in series, preceded by a cation H+ guard column (Bio-Rad; catalog no. 125-0140). The detector used was an HP 407A refractive index detector. Elution was isocratic using a mobile phase of 1.5 mM sulfuric acid at a flow rate of 0.6 ml/min. The column temperature was maintained at 50°C. The injection volume used was 20 µl. The columns were flushed with water for at least 1 h after every 18 to 24 samples.
Determination of total nitrogen concentration.
Before and during fermentations, total nitrogen was determined by separately measuring ammonia concentration and alpha amino acid concentration and summing the two values. Alpha amino acid concentration was measured using the procedure described previously by Dukes and Butzke (12). Ammonia was determined via an enzymatic kit produced by R-Biopharm (South Marshall, MI).
Determination of model parameters and generation of simulated fermentations.
Sugar, nitrogen, ethanol, total biomass, and viable biomass concentrations were used for parameter estimation. However, only the first seven observed time points of total and viable biomass were used. These time points were used because the model is thought to represent cell activity and not cell viability. However, cell activity is not yet easily measured (11). MATLAB software (version 7.0; The MathWorks, Inc., Natick, MA) was then used to find values for the seven model parameters. Markov chain Monte Carlo integration (MCMC) in conjunction with Bayesian parameter estimation (10) was used to determine the expectation and credible regions of all seven model parameters for each fermentation (see "Parameter estimation" below). All parameter regression surfaces were performed using Bayesian robust linear regression and MCMC methods (see "Regression modeling of model parameters" below). A function called "metrop2" in a free toolbox from the Laboratory of Computational Engineering (http://www.lce.hut.fi/research/mm/mcmcstuff/) was adapted to perform all MCMC procedures.
Fermentation model.
The nitrogen-limited model utilized in this paper was first proposed by Cramer et al. (11). It consists of five coupled ODEs:
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There are two minor differences between the previous model (11) and the model presented here. First, total cell mass has been included in the here-presented model. This inclusion does not change the model at all. Total cell mass is included in this work to later illustrate the difference between total and active cell mass. The second difference is that we no longer refer to active cell mass as viable cell mass. Cramer et al. (11) provided significant evidence that suggested live cells may not be completely active in terms of growth, utilization of sugar and nitrogen, and production of ethanol. Thus, we have formally acknowledged this in the model by renaming viable cell mass as active cell mass.
To adapt this model for temperature dependence, we first assume that the basic structure of the coupled ODEs does not vary with temperature. Only the parameters within the ODEs (µmax, k'd, ßmax, KN, KS, YX/N, and YE/S) are considered to be potential functions of temperature. Here, we find the temperature dependence of these parameters and then we model this temperature dependence by using robust polynomial regression (see "Regression modeling of model parameters" below). We developed the polynomial model simply to facilitate interpolation between data values from the temperatures studied. For this reason, it would be possible to utilize other regression models, lookup tables, neural networks, nonlinear regression of Arrhenius-type equations, or any other expression that describes the experimentally derived temperature dependence of the model parameters.
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FIG. 1. Experimental °Brix curves for three different initial conditions and six different temperatures. (a) Normal sugar and normal nitrogen. (b) High sugar and normal nitrogen. (c) Normal sugar and low nitrogen. Each different temperature is shown with a different symbol, and the fermentation for each temperature was performed in duplicate. The data from these duplicate fermentations give an indication of the small inherent experimental error observed for these measurements.
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Initial nitrogen conditions had a much stronger effect on the overall rate of sugar utilization. For example, at 11°C, the normal sugar and low-nitrogen fermentations dropped an average of 22.3 °Brix in 815 h. Likewise, normal sugar and low-nitrogen fermentations at all other temperatures had a significantly lower overall change in °Brix compared to normal sugar and nitrogen and high-sugar and low-nitrogen fermentations given the same change in time of fermentation.
Model fit.
All 18 fermentations (three initial conditions at six temperatures) were fit to the model, and each resulted in a corresponding set of model parameters. Figure 2 shows two plots of typical model fits for various fermentations. Notice that sugar, ethanol, and nitrogen are accurately fit to the model. More discrepancies exist between the fits for cell mass. At lower temperatures, total cell mass seems to gradually increase even after the exponential growth phase. The observed viable cell mass at lower temperatures gradually decreases; however, in order to more accurately fit the other state variables (sugar and ethanol), the model predicts that cell activity decreases more rapidly. In general, total cell mass is more accurately predicted for higher temperature fermentations and cell activity more closely follows the measured cell viability (Fig. 2). In Fig. 2b, we see that the experimental total cell mass does not increase after the exponential growth phase and that the viable cell mass more rapidly decreases. These model fit results are consistent with the results of Cramer et al. (11).
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FIG. 2. Typical model fits for two different fermentations. (a) Normal sugar and low-nitrogen fermentation at 15°C. (b) Normal sugar and normal nitrogen fermentation at 30°C. Both panel a and panel b show all five state variables: sugar, viable cell mass (filled circles), total cell mass (open circles and broken line), nitrogen, and ethanol. It should be noted that the model does not predict viable cell mass but rather active cell mass (solid line).
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FIG. 3. Three model parameters from equations 1 through 8 were shown to have a significant relationship with respect to temperature. Each parameter estimate shows the mean value from the MCMC integration () along with its 95% credible region (vertical lines). Regression surfaces (solid lines) also include a 95% credible region (dotted lines). The maximum specific growth rate (a) increases by a factor of 6 as temperature increases from 11 to 35°C. The ethanol sensitivity constant which causes cell inactivation (b) increases by a factor of 13 as temperature increases from 11 to 35°C. The maximum rate of sugar utilization (c) increases by a factor of 6 as temperature increases from 11 to 35°C. Also note that some of the data points were plotted slightly off-center so as to prevent the overlap of error bars.
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FIG. 4. One model parameter from equations 1 through 8 was found to have a significant relationship with respect to initial nitrogen concentration. The yield coefficient between cell mass and nitrogen was about two times greater at lower initial nitrogen concentrations. The mean value from the MCMC parameter estimation is shown () along with the 95% credible regions (vertical lines). Regression surfaces (solid lines) also include a 95% credible region (dotted lines). Also note that some of the data points were plotted slightly off-center so as to prevent the overlap of error bars.
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FIG. 5. Three model parameters from equations 1 through 8 were shown to not have a significant relationship with respect to temperature or initial conditions. These parameters (Monod constant for nitrogen-limited growth [a], Monod constant for sugar transport [b], and the yield coefficient between ethanol and sugar [c]) are plotted against temperature. Each parameter estimate shows the mean value from the MCMC integration () along with its 95% credible region (vertical lines). Notice that the error bars are typically larger than the variation between the estimated mean values. Also note that some of the data points were plotted slightly off-center so as to prevent the overlap of error bars. It should be noted that the error bars are the dominant features of these plots.
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This comprehensive model was then shown to accurately predict a transition from sluggish to normal to stuck fermentations as the temperature rose from 11 to 35°C. Figure 6 shows this transition for both normal sugar/normal nitrogen and normal sugar/low-nitrogen fermentations. In general, model fits are best near 20°C; at extreme temperatures, model fits are slightly less accurate. The underlying feature to recognize in Fig. 6 is that at low temperatures, the sugar utilization rate is low; at the midrange temperatures, fermentations seem more normal; and at high temperatures, sugar utilization starts out rapidly and is then followed by a sudden cessation of fermentation activity. Experimental data and model fits are a close match and both show these underlying phenomena, unlike previous models for wine fermentation kinetics.
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FIG. 6. The comprehensive model fits of sugar utilization for normal sugar/normal nitrogen and normal sugar/low nitrogen fermentations ranging from 11 to 35°C. Notice that the model is able to explain the experimental transition from sluggish fermentation activity at low temperatures to normal fermentation activity at midrange temperatures to stuck fermentation activity at high temperatures.
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FIG. 7. Predictions made by the comprehensive model for two different fermentations at extreme conditions. Experiments for both panel a and panel b start from high-sugar/low-nitrogen conditions; however, the experiment for panel a was run at a low temperature and that for panel b was carried out at a high temperature. The activity of both fermentations is relatively well predicted. The main differences between experimental and simulated predictions are the underestimations of viable (filled circles) and total (open circles and broken line) cell mass. However, sugar utilization is the most critical state variable to predict. Furthermore, it should be noted that the model predicts active cell mass and not viable cell mass. Thus, a difference between model prediction and observed data is expected.
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The model was also able to accurately predict fermentation activity at extreme conditions that had not been previously tested. From Fig. 6, we can see that model fits are typically less accurate at 11 or 35°C. However, data from fermentations using novel initial conditions (high sugar and low nitrogen) at these temperatures were shown to be accurately predicted by the model (Fig. 7). This shows that the model is robust across extreme conditions and could be used to predict problem fermentations at temperatures and initial conditions not yet observed, making it an interesting candidate for use in a practical winery setting.
The main discrepancy between the model fit and the data is the difference between experimental and model predictions of cell mass after the exponential growth phase. The difference between model predictions of cell activity and the experimentally observed cell viability is to be expected and is consistent with the results of Cramer et al. (11). This difference is likely due to cells that are inactive rather than dead. For example, ethanol may be preventing sugar transport into the cell, thus reducing sugar utilization even though the cells are not yet dead. Regardless of the reason, it seems certain that the cell viability measurements made are not a good measure of cell activity. This is the main reason that only the first seven data points from total and viable cell mass are included into the parameter estimation routine. This approach is well justified by the model's excellent prediction capabilities of sugar and ethanol (the most important state variables from an enologist's point of view). The model was also unable to predict that the total cell mass for many fermentations gradually increased after the exponential phase. This result may be due to the gradual degradation of nitrogen sources being generated from dead yeast cells. This source of nitrogen could then potentially be utilized by the active cells for cell reproduction. Regardless, not accounting for such additional cell growth had little to any effect on the final quantitative predictions of the other state variables.
Another small discrepancy between the model and the data is that the nitrogen measurements suggest that not all nitrogen is utilized during fermentation. Some small amount of nitrogen is typically left over in the fermentation. This leftover amount may be due to the inability of the yeast to utilize some types of nitrogen sources. However, fermentations at higher temperatures consistently resulted in higher residual nitrogen levels at the end of the fermentations (Fig. 7). This result could be due to cell growth inhibition at higher temperatures due to ethanol. Due to this added sensitivity of ethanol at higher temperatures, the cells may be unable to fully utilize all of the available nitrogen.
One interesting finding for the presented model is that the yield coefficient of cell mass on nitrogen turned out to significantly vary with respect to the initial nitrogen concentration (Fig. 4). The simplest and most likely explanation for this observation is that at higher concentrations of initial nitrogen, a different nutrient component could be growth limiting. This explanation would be consistent with the findings and data of Cramer et al. (11) and Malherbe et al. (18). A related potential explanation is that the cell mass yield is different for various forms of nitrogen. The juices in this work were first diluted, and then appropriate additions of DAP were added back to achieve the desired levels of nitrogen. The original juice contained 111 mg N/liter (ammonia) and 172 mg N/liter (
-amino nitrogen). After the dilution and addition of DAP, the low-nitrogen juices contained about equal parts nitrogen from ammonia and
-amino nitrogen. However, over 85% of the nitrogen in high-nitrogen juices was from ammonia. This difference in initial nitrogen composition could lead to differences in observed yield. As the temperature dependence of the fermentation is well predicted, regardless of the initial nitrogen level and composition, it is apparent that these two issues can be separated, leaving further explanation of the changes in biomass yield on nitrogen for further detailed study.
Despite these model discrepancies, the presented model accurately predicts the most important state variable: sugar concentration. Sugar utilization is of the utmost importance for any model that aims to aid in the prediction of stuck and sluggish fermentations. The accurate prediction of ethanol concentration, cell growth, cell activity, or nitrogen consumption gives valuable insight into microbial physiology; however, for the purposes of winemaking, accurate predictions of these variables are primarily important because they lead to the accurate prediction of sugar utilization. This model may be of value to winemakers because it always yields reasonable predictions of sugar utilization. Winemakers could potentially use this model to make decisions in the winery. For example, if a must is known to have a low level of nitrogen, a winemaker may typically supplement the natural level of available nitrogen with DAP to avoid a stuck or sluggish fermentation. However, certain winemakers may prefer to avoid the use of DAP because of the expense or because they believe it affects wine quality. The model presented in this paper could then be used to predict when the addition of DAP is critical and when it can be avoided.
Another important result to be stressed is that low-nitrogen fermentations are more sensitive to extremes in temperature. For example, Fig. 6 shows that for normal nitrogen conditions, any temperature between 11 and 25°C could be used to complete the fermentations (although 25°C would be the fastest). For low-nitrogen initial conditions, fermentation activity more easily becomes problematic at higher or lower temperatures. The optimal temperature range to complete low-nitrogen fermentations becomes smaller. While the experimental data at low-nitrogen levels were not allowed to go to completion, the model suggests that a temperature of 20°C would yield the greatest opportunity to finish a low-nitrogen-level fermentation.
While low levels of nitrogen have long been linked with problem fermentations, what the relationship between low levels of nitrogen and problem fermentations is has not been precisely determined. Some authors have linked low nitrogen to low cellular activity (2, 3), while others associated this condition with resulting low levels of biomass (11, 20). The data presented in this paper support the latter of these two hypotheses. Only one of the model parameters was shown to vary with respect to the initial nitrogen concentration. In addition, this one parameter (YX/N) only determines the amount of cell mass produced from a given quantity of nitrogen and does not directly affect the metabolic rates of reaction within a given cell. In the context of the fermentations used in this study, we can conclude that low levels of nitrogen contribute to the problematic fermentations because they result in fewer cells. However, this conclusion may not hold for other juices or strains of yeast which may react differently to low levels of nitrogen (15).
The adaptation of the presented model to industrial fermentations will be dependent upon collecting samples and determining the key state variables. These tasks must be carried out for several fermentations at different temperatures and conditions before predictions can be made. The empirical modeling methods presented below in "Parameter estimation" and "Regression modeling of model parameters" are carefully constructed to fully leverage all of the available information from the observed data and make optimal decisions with respect to parameter estimates and regression surfaces. However, these methods are not necessary for constructing a working model capable of predicting problematic fermentations. For example, a simple lookup table could be used to estimate model parameters that are temperature dependent (i.e., a regression model is not necessary to determine that fermentations at 11°C will result in a maximum specific growth rate of approximately 0.05 h–1). Future versions of this model may implement more-informative regression models for temperature dependence (e.g., mixtures of Arrhenius-type equations); however, these regression models will still be dependent upon data collected and parameters estimated for new systems.
In conclusion, we have shown that the presented model can accurately predict fermentation behavior across a wide variety of temperatures and initial conditions. This model is the first wine fermentation model that predicts a transition from sluggish to normal to stuck fermentations with respect to increasing temperature. Furthermore, the model could be used in a winery setting to determine the length of time required to finish a fermentation based on just the concentration of sugar and nitrogen in the juice, the optimal temperature to reach a minimum in sugar concentration, or whether the addition of a supplementary nitrogen source is critical. In order to adapt this model to various systems, it would be necessary for a winery to first collect data on the various state variables during the course of different fermentations. Once this collection of data has been achieved, a comprehensive model could be used to make predictions for new systems in different winery settings.
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is a vector of the noise parameters for each state variable (
X,
XA,
S,
E, and
N), n is the total number of points collected for each state variable, Xi is the experimental observed total cell mass at the ith observation, and
i is the model prediction for the total cell mass at the ith observation. Similarly, the circumflex marks the model prediction as opposed to the experimental value (no circumflex) for each of the other state variables as well. These model predictions are calculated using the model parameter values in b and equations 1 through 8.
Prior probabilities were then defined for each of the seven model parameters and each of the five noise parameters. For example, the prior probability over the maximum specific growth rate was
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) are the combined priors for all model and noise parameters and P(b,
|D) is the posterior distribution for all model and noise parameters given a set of data, D. This posterior is evaluated via MCMC integration to find the mean and credible regions shown for each model parameter shown in Fig. 3, 4, and 5 (10). |
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TABLE A1. Values used to define the prior probabilities over all model and noise parametersa
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![]() | (A4) |
![]() | (A5) |
is the noise parameter associated with k'd, log(
'di) is the estimation of k'd for the ith fermentation from the regression surface of equation A4, and fi is the standard deviation of the credible region for the ith parameter estimate. Essentially, all the fi values do is adjust the importance of the fit for each parameter value based upon the size of its credible regions. For example, the credible regions at high temperatures are larger in Fig. 3b. Thus, fi when T is 35°C is greater than fi when T is 11°C. No prior distributions were used for the regression surface parameters (a) or the noise parameter
. Thus, MCMC integration was used to evaluate likelihood in equation A5 and to estimate mean values and credible regions for the regression surface parameters (10). The values for all regression surfaces are summarized in Table A2. |
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TABLE A2. Estimated parameter values for each of the regression surfacesa
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Published ahead of print on 6 July 2007. ![]()
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