Thermodynamics: Isobutane entropy and power problem

In summary, for part A, the power generated by the adiabatic expander can be calculated using the first law of thermodynamics and the ideal gas equation of state. For part B, the change in entropy for this operation is zero, as no heat is added to the system.
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Homework Statement


Isobutane flows through an expander (like a turbine) at 680 moles/sec where it undergoes a change in state from 4826 kPa and 260 degrees Celsius to 483 kPa and 195 degrees Celsius.

a) If the expander is adiabatic how much power is generated by the expander?
b) What is the change in entropy for this operation?

Homework Equations


TC = 408.1 K
PC = 3650 kPa
CigR = A + BT + C(T^2) + D/(T^2) where T is in K, A = 1.667, B = 37.853*10-3, C = 11.945*10-6, and D = 0.

The Attempt at a Solution


I have no idea where to go with this problem for parts A and B. Can someone please give me a way to go about solving this problem
 
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?For part A, you need to use the first law of thermodynamics. It states that the change in internal energy (ΔU) is equal to the heat added to the system (Q) minus the work done by the system (W). Since this is an adiabatic process, no heat is added (Q=0) so ΔU=W. The power generated by the expander will be equal to the rate of change of internal energy with respect to time, or P=ΔU/Δt. You can calculate the change in internal energy by using the ideal gas equation of state. The change in internal energy can be calculated as follows:ΔU = nRT(1/P1 - 1/P2)where n is the number of moles of gas, R is the universal gas constant, T is the temperature and P1 and P2 are the initial and final pressures, respectively. Therefore, the power generated by the expander is:P = nRT(1/P1 - 1/P2)/ΔtFor part B, you need to use the second law of thermodynamics. It states that the change in entropy (ΔS) is equal to the heat added to the system (Q) divided by the temperature (T). Since this is an adiabatic process, no heat is added (Q=0) so ΔS=0. Therefore, the change in entropy for this operation is zero.
 

FAQ: Thermodynamics: Isobutane entropy and power problem

1. What is thermodynamics and why is it important?

Thermodynamics is the study of how energy is transferred and transformed in physical systems. It is important because it helps us understand and predict the behavior of matter and energy in various processes and systems, such as engines, refrigerators, and chemical reactions.

2. What is isobutane and how is it related to thermodynamics?

Isobutane is a colorless and odorless gas that is commonly used as a refrigerant in air conditioning and refrigeration systems. It is also used as a fuel in some engines. In thermodynamics, isobutane is used as an example to study the relationship between entropy and power in a closed system.

3. What is entropy and how does it relate to isobutane in thermodynamics?

Entropy is a measure of the disorder or randomness of a system. In thermodynamics, it is related to the amount of energy that is unavailable for work in a system. For isobutane, the entropy can be calculated based on its temperature and pressure, and it can help us understand the efficiency of the system in terms of power output.

4. What is the power problem in thermodynamics and how does it apply to isobutane?

The power problem in thermodynamics refers to the challenge of maximizing the power output of a system while minimizing its entropy production. In the case of isobutane, the power problem can be seen in the trade-off between increasing the pressure to increase power output, but also increasing the entropy production, which reduces efficiency.

5. How can isobutane be used to illustrate the second law of thermodynamics?

The second law of thermodynamics states that the total entropy of a closed system will always increase over time. Isobutane can be used as an example to demonstrate this law, as it shows that even though work can be obtained from a system, there will always be some energy that is lost and cannot be used again.

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