the handbook of food engineering practice crc press chapter 10 ...

the handbook of food engineering practice crc press chapter 10 ... the handbook of food engineering practice crc press chapter 10 ...

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Table 5. Analytical expressions for calculation of Γ for different temperature functions. Function Q 10 Approach Arrhenius Approach Sine wave Γ=I o (a o b) Γ≈I o E a a o RT m T m +a o Square wave Γ= 1 2 [ea ob +e -a o b 1 ] Γ= 2 exp[ E A a o RT m (T m +a o ) ] +1 2 exp[ -E A a o RT m (T m -a o ) ] Spike wave j=0 Random Γ= e bT m E A a o Γ= ea ob -e -a o b exp[ RT m (T m +a o ) ] - exp[ -E A a o RT m (T m -a o ) ] 2a o b Γ= E A a o 2RT m (T m +a o ) n n ∑ e bT j ∆t j ∑ exp( -EA ) ∆t j RTj j=0 Γ= exp( -EA ) RTm I o (x) is a modified Bessel function of zero order. Its values can be calculated from an infinite series expansion, I o (x)=1+ x2 2 2 + x4 2 2 4 2 + x 6 2 2 4 2 6 2 +..., or found in Mathematical Handbooks (Tuma, 1988). From Γ of a variable temperature distribution the effective reaction rate and temperatures k eff andT eff and the value of the quality function for the particular deterioration mode are calculated. Comparison of this value to the experimentally obtained quality value, for variable temperature functions covering the range of practical interest is the ultimate validation of the developed kinetic models. This methodology was applied by Labuza and coworkers for various food reaction systems and agreement or deviation from predicted kinetic behavior was assessed (Berquist and Labuza, 1983; Kamman and Labuza,1981; Labuza et al. 1982; Riboh and Labuza, 1982; Saltmarch and Labuza,1982; Taoukis and Labuza,1989). 44

Figure 8. Characteristic fluctuating temperature distributions used to verify validity of kinetic models. a o is the amplitude of the sine, square and spike wave functions. Alternatively the effect of variable temperature distribution can be expressed through an equivalent time (t eq ), defined as the time at a reference temperature (is) resulting in the same quality change (i.e. same value of quality function) as the variable temperature. The practicality of t eq is that if the chosen T ref is the suggested keeping temperature e.g. 4°C for chilled products, it will directly give the remaining shelf life at that temperature. Note that if the mean temperature is chosen as the reference temperature, T ref =T m , then t eq /t=Γ. Further a short mention of the Equivalent point method is relevant. This approach has been used for evaluation and modelling of thermal processes (Nunes and Swartzel, 1990) and the response of Time Temperature Indicators (TTI) (Fu and Labuza, 1993). The same methodology would apply for quality loss during the shelf life of foods. Using the expression of the quality function 45

Table 5. Analytical ex<strong>press</strong>ions for calculation <strong>of</strong> Γ for different temperature functions.<br />

Function Q <strong>10</strong> Approach Arrhenius Approach<br />

Sine wave Γ=I o (a o b) Γ≈I o<br />

E a a o<br />

RT m T m +a o<br />

Square wave Γ= 1 2 [ea ob +e<br />

-a o b 1<br />

] Γ= 2 exp[ E A a o<br />

RT m (T m +a o ) ] +1 2 exp[<br />

-E A a o<br />

RT m (T m -a o ) ]<br />

Spike wave<br />

j=0<br />

Random Γ=<br />

e bT m<br />

E A a o<br />

Γ= ea ob -e<br />

-a o b<br />

exp[ RT m (T m +a o ) ] - exp[<br />

-E A a o<br />

RT m (T m -a o ) ]<br />

2a o b Γ=<br />

E A a o<br />

2RT m (T m +a o )<br />

n<br />

n<br />

∑<br />

e bT j ∆t j<br />

∑<br />

exp( -EA ) ∆t j RTj<br />

j=0<br />

Γ=<br />

exp( -EA ) RTm<br />

I o (x) is a modified Bessel function <strong>of</strong> zero order. Its values can be calculated from an<br />

infinite series expansion, I o (x)=1+ x2<br />

2 2 + x4<br />

2 2 4 2 + x 6<br />

2 2 4 2 6 2 +..., or found in Ma<strong>the</strong>matical<br />

Handbooks (Tuma, 1988).<br />

From Γ <strong>of</strong> a variable temperature distribution <strong>the</strong> effective reaction rate and<br />

temperatures k eff andT eff and <strong>the</strong> value <strong>of</strong> <strong>the</strong> quality function for <strong>the</strong> particular<br />

deterioration mode are calculated. Comparison <strong>of</strong> this value to <strong>the</strong> experimentally obtained<br />

quality value, for variable temperature functions covering <strong>the</strong> range <strong>of</strong> practical interest is<br />

<strong>the</strong> ultimate validation <strong>of</strong> <strong>the</strong> developed kinetic models. This methodology was applied by<br />

Labuza and coworkers for various <strong>food</strong> reaction systems and agreement or deviation from<br />

predicted kinetic behavior was assessed (Berquist and Labuza, 1983; Kamman and<br />

Labuza,1981; Labuza et al. 1982; Riboh and Labuza, 1982; Saltmarch and Labuza,1982;<br />

Taoukis and Labuza,1989).<br />

44

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