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Under anaerobic conditions, glucose is broken down in muscle tissue to form lactic acid according to the reaction \(\mathrm{C}_{6} \mathrm{H}_{12} \mathrm{O}_{6} \rightarrow 2 \mathrm{CH}_{3} \mathrm{CHOHCOOH}\). Thermodynamic data at \(T=298 \mathrm{K}\) for glucose and lactic acid are given in the following table: $$\begin{array}{lccc} & \Delta \boldsymbol{H}_{f}^{\circ}\left(\mathbf{k J} \mathbf{~ m o l}^{-1}\right) & C_{P, m}\left(\mathbf{J} \mathbf{K}^{-1} \mathbf{m o l}^{-\mathbf{1}}\right) & S_{m}^{\circ}\left(\mathbf{J} \mathbf{K}^{-\mathbf{1}} \mathbf{m o l}^{-\mathbf{1}}\right) \\ \hline \text { Glucose } & -1273.1 & 219.2 & 209.2 \\ \text { Lactic } & -673.6 & 127.6 & 192.1 \end{array}$$ Calculate, \(\Delta S\) for the system, the surroundings, and the universe at \(T=325 \mathrm{K}\). Assume the heat capacities are constant \\[ \text { between } T=298 \mathrm{K} \text { and } T=330 . \mathrm{K} \\]

Short Answer

Expert verified
The entropy changes at \(T = 325K\) are: - For the system: \(211\,J/(mol\cdot K)\) - For the surroundings: \(228\,J/(mol\cdot K)\) - For the universe: \(439\,J/(mol\cdot K)\)

Step by step solution

01

1. Calculate the Standard Enthalpy Change

To calculate the standard enthalpy change \(\Delta H\) for the given reaction, we'll use the standard enthalpies of formation \(\Delta H_{f}^{\circ}\) for the products and the reactants: \(\Delta H = \Sigma n_{products} \Delta H_{f,products}^\circ - \Sigma m_{reactants} \Delta H_{f,reactants}^\circ\) For this reaction, \(\Delta H = 2\Delta H_{f,LacticAcid}^\circ - 1\Delta H_{f,Glucose}^\circ\) Using the given data from the table: \(\Delta H = 2(-673.6\,kJ/mol) - 1(-1273.1\, kJ/mol)\) \(\Delta H = -1347.2 + 1273.1 = -74.1\,kJ/mol\)
02

2. Calculate the Standard Entropy Change at 298K

To calculate the standard entropy change \(\Delta S\) for the reaction at 298K, we'll use the standard molar entropies \(S_{m}^{\circ}\) for the products and the reactants: \(\Delta S^{\circ}_{298} = \Sigma n_{products} S_{m,products}^{\circ} - \Sigma m_{reactants} S_{m,reactants}^{\circ}\) For this reaction, \(\Delta S^{\circ}_{298} = 2S_{m,LacticAcid}^{\circ} - 1S_{m,Glucose}^{\circ}\) Using the given data from the table: \(\Delta S^{\circ}_{298} = 2(192.1\,J/(mol\cdot K)) - 1(209.2\, J/(mol\cdot K))\) \(\Delta S^{\circ}_{298} = 384.2 - 209.2 = 175\,J/(mol\cdot K)\)
03

3. Calculate Entropy Change for the System at 325K

To calculate the entropy change for the system at 325K, we need to account for both the standard entropy change \(\Delta S^{\circ}_{325}\) and the change in entropy due to the temperature change from 298K to 325K, using the heat capacities \(C_{P,m}\): \(\Delta S_{system} = \Delta S^{\circ}_{298} + \Delta S(T)\) The temperature-dependent term is given by: \(\Delta S(T) = \Sigma n_{products} C_{P,m,products}(T) - \Sigma m_{reactants} C_{P,m,reactants}(T)\) For this reaction, we can use the heat capacities \(C_{P, m}\) given in the table: \(\Delta S(T) = 2(127.6\, J/(mol\cdot K)) - 219.2\, J/(mol\cdot K)\) \(\Delta S(T) = 36\, J/(mol\cdot K)\) Therefore, the entropy change for the system at \(T = 325K\) is: \(\Delta S_{system} = 175 + 36 = 211\,J/(mol\cdot K)\)
04

4. Calculate Entropy Change for the Surroundings at 325K

The entropy change for the surroundings is given by the heat released in the reaction divided by the temperature: \(\Delta S_{surroundings} = -\frac{\Delta H}{T}\) Using the calculated standard enthalpy change \(\Delta H\) and the given temperature \(T = 325K\): \(\Delta S_{surroundings} = -\frac{-74.1\,kJ/mol}{325\,K}\) \(\Delta S_{surroundings} = 0.228\,kJ/(mol\cdot K) = 228\,J/(mol\cdot K)\)
05

5. Calculate Entropy Change for the Universe at 325K

The entropy change for the universe is the sum of the entropy changes for the system and the surroundings: \(\Delta S_{universe} = \Delta S_{system} + \Delta S_{surroundings}\) Using the calculated values from steps 3 and 4: \(\Delta S_{universe} = 211\,J/(mol\cdot K) + 228\,J/(mol\cdot K)\) \(\Delta S_{universe} = 439\,J/(mol\cdot K)\) So, the entropy changes at \(T = 325K\) are: - For the system: \(211\,J/(mol\cdot K)\) - For the surroundings: \(228\,J/(mol\cdot K)\) - For the universe: \(439\,J/(mol\cdot K)\)

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Enthalpy Change
Enthalpy change, denoted as \( \Delta H \), is a central concept in thermodynamics that represents the heat content during a chemical reaction under constant pressure. This value can be thought of as the total energy change, accounting for both internal energy and the energy associated with pressure and volume. In chemical reactions, the enthalpy change tells us how much heat is absorbed or released. \( \Delta H \) is calculated using the formula: \[ \Delta H = \Sigma n_{products} \Delta H_{f,products}^{\circ} - \Sigma m_{reactants} \Delta H_{f,reactants}^{\circ} \] where \( \Delta H_{f}^{\circ} \) indicates the standard enthalpies of formation for the respective substances at standard conditions (usually 298 K and 1 atm). A negative \( \Delta H \) indicates an exothermic process, where energy is released, while a positive value suggests an endothermic process, involving the absorption of energy.

In our exercise involving the conversion of glucose into lactic acid, the calculation of \( \Delta H \) revealed that the reaction is exothermic, releasing 74.1 kJ/mol at standard conditions, indicating that heat is being released to the surroundings as glucose is converted to lactic acid.
Entropy Change
Entropy, symbolized by \( S \), is a measure of disorder or randomness in a system. The change in entropy, \( \Delta S \) is a key factor in determining the spontaneity of a process. The formula for calculating the standard entropy change is: \[ \Delta S^{\circ}_{298} = \Sigma n_{products} S_{m,products}^{\circ} - \Sigma m_{reactants} S_{m,reactants}^{\circ} \] It involves subtracting the sum of entropies of reactants from the sum of entropies of products. A positive \( \Delta S \) indicates an increase in disorder, whereas a negative value means the system has become more ordered.

In the case of the process we're looking at, the entropy change for the system increased, suggesting that the products (lactic acid molecules) are less ordered than the reactants (glucose molecules). The step-by-step solution shows how to calculate the entropy change considering not just the reaction conditions but also the effect of a temperature change from the standard value.
Gibbs Free Energy
Gibbs free energy, represented by \( G \), combines the concepts of enthalpy (\( H \) and entropy (\( S \) into a single value that predicts the spontaneity of a reaction. The change in Gibbs free energy, \( \Delta G \) is given by the equation: \[ \Delta G = \Delta H - T\Delta S \] where \( T \) is the temperature in kelvins. A negative \( \Delta G \) indicates that a reaction is spontaneous, whereas a positive value suggests it is non-spontaneous under the given conditions. If \( \Delta G \) is zero, the system is at equilibrium.

While the exercise did not ask for a \( \Delta G \) calculation, understanding Gibbs free energy is crucial as it integrates the heat exchange with the surroundings (\( \Delta H \) and the change in system disorder (\( \Delta S \) to fully evaluate the feasibility of a reaction.
Chemical Reactions
Chemical reactions involve the transformation of reactants into products. These reactions are governed by the laws of thermodynamics, which dictate that energy is conserved, and often involve changes in enthalpy and entropy. The direction and extent to which a chemical reaction proceeds depend on various factors, including temperature, pressure, concentration of reactants and products, and the overall change in Gibbs free energy. Understanding the thermodynamic principles behind these reactions allows chemists to predict whether a reaction will occur and under what conditions it will be most favorable.

For example, the conversion of glucose to lactic acid that was analyzed in our exercise is a common biological reaction occurring under anaerobic conditions where organisms extract energy from glucose in the absence of oxygen.
Heat Capacity
Heat capacity is a term we encounter in the study of thermodynamics, referring to the amount of heat required to increase the temperature of a substance by a certain amount, usually one degree Celsius or one kelvin. The heat capacity at constant pressure (\( C_{P} \) is particularly relevant in chemical reactions occurring in open systems, where pressure remains constant. The formula to adjust entropy for temperature changes, utilizing \( C_{P} \) is as follows: \[ \Delta S(T) = \Sigma n_{products} C_{P,m,products} (T) - \Sigma m_{reactants} C_{P,m,reactants} (T) \] This allows us to understand how the entropy of a system evolves as the temperature changes. With a constant heat capacity assumption, it makes the calculation more straightforward as the same value applies across a temperature range—demonstrated in the thermodynamic calculation of the glucose-to-lactic acid reaction.

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Most popular questions from this chapter

The Chalk Point, Maryland, generating station supplies electrical power to the Washington, D.C., area. Units 1 and 2 have a gross generating capacity of \(710 .\) MW (megawatt). The steam pressure is \(25 \times 10^{6} \mathrm{Pa}\), and the superheater outlet temperature \(\left(T_{h}\right)\) is \(540 .^{\circ} \mathrm{C} .\) The condensate temperature \(\left(T_{c}\right)\) is \(30.0^{\circ} \mathrm{C}\) a. What is the efficiency of a reversible Carnot engine operating under these conditions? b. If the efficiency of the boiler is \(91.2 \%\), the overall efficiency of the turbine, which includes the Carnot efficiency and its mechanical efficiency, is \(46.7 \%,\) and the efficiency of the generator is \(98.4 \%,\) what is the efficiency of the total generating unit? (Another \(5.0 \%\) needs to be subtracted for other plant losses. c. One of the coal-burning units produces \(355 \mathrm{MW}\). How many metric tons (1 metric ton \(=1 \times 10^{6} \mathrm{g}\) ) of coal per hour are required to operate this unit at its peak output if the enthalpy of combustion of coal is \(29.0 \times 10^{3} \mathrm{kJ} \mathrm{kg}^{-1} ?\)

The maximum theoretical efficiency of an internal combustion engine is achieved in a reversible Carnot cycle. Assume that the engine is operating in the Otto cycle and that \(C_{V, m}=5 R / 2\) for the fuel-air mixture initially at \(273 \mathrm{K}\) (the temperature of the cold reservoir). The mixture is compressed by a factor of 6.9 in the adiabatic compression step. What is the maximum theoretical efficiency of this engine? How much would the efficiency increase if the compression ratio could be increased to \(15 ?\) Do you see a problem in doing so?

The amino acid glycine dimerizes to form the dipeptide glycylglycine according to the reaction \\[ 2 \text { Glycine }(s) \rightarrow \text { Glycylglycine }(s)+\mathrm{H}_{2} \mathrm{O}(l) \\] Calculate \(\Delta S, \Delta S_{\text {surr}},\) and \(\Delta S_{\text {universe}}\) at \(T=298 \mathrm{K}\). Useful thermodynamic data follow: $$\begin{array}{lccc} & \text { Glycine } & \text { Glycylglycine } & \text { Water } \\ \hline \Delta H_{f}^{\circ}\left(\mathrm{kJ} \mathrm{mol}^{-1}\right) & -537.2 & -746.0 & -285.8 \\ S_{m}^{\circ}\left(\mathrm{JK}^{-1} \mathrm{mol}^{-1}\right) & 103.5 & 190.0 & 70.0 \end{array}$$

An air conditioner is a refrigerator with the inside of the house acting as the cold reservoir and the outside atmosphere acting as the hot reservoir. Assume that an air conditioner consumes \(1.70 \times 10^{3} \mathrm{W}\) of electrical power and that it can be idealized as a reversible Carnot refrigerator. If the coefficient of performance of this device is 3.30 how much heat can be extracted from the house in a day?

The interior of a refrigerator is typically held at \(36^{\circ} \mathrm{F}\) and the interior of a freezer is typically held at \(0.00^{\circ} \mathrm{F}\) If the room temperature is \(65^{\circ} \mathrm{F}\), by what factor is it more expensive to extract the same amount of heat from the freezer than from the refrigerator? Assume that the theoretical limit for the performance of a reversible refrigerator is valid in this case.

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