Work of Carnot Engine integral

In summary, the conversation discusses the process of choosing u and v transformations to be equal to constants and the reason for f(u,v) = 1 for the area in xy. The problem statement states that the work done by an ideal Carnot engine is equal to the area enclosed by two isotherms and adiabatic curves. The conversation also mentions the difficulty of integrating the area in xy due to the curved sides and the use of transformation to simplify the calculation. The conversation concludes by mentioning the use of perturbation methods and the 3rd Law of Thermodynamics.
  • #1
mathnerd15
109
0
I'm curious how do you choose the u and v transformations here to be equal to the constants and why is the f(u,v)=1 for the area- because you are summing infinitesimal x's and y's? I see that the area in xy is difficult to integrate because the sides are curved. is the transformation proven somewhere?
problem statement: the work done by an ideal Carnot engine is equal to the area enclosed by two isotherms and adiabatic curves. [tex]xy=a, xy=b, xy^{1.4}=c, xy^{1.4}=d[/tex][tex]\begin{bmatrix}\frac{\partial x}{\partial u}\ & \frac{\partial x}{\partial v}\\ \frac{\partial y}{\partial u} &\frac{\partial y}{\partial v}\\ \end{bmatrix}=\frac{5}{2v}, \int_{c}^{d}\int_{a}^{b}\frac{5}{2v}dudv=\frac{5}{2}(b-a)ln\frac{d}{c}[/tex]

by the way, how long does it take people to do these?
 
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  • #2
You don't do it as a double integral, but rather as a difference between integrals. You have a total of four curves, which you can integrate to get the area under the curve (down to the x axis), then you take the sum of the upper isotherm and adiabat, and you substract the lower isotherm and adiabat, and what is left is the area enclosed by the curves.

The reason you can do that is that the extreme points along x are the same for the upper curves and the lower curves.
 
  • #3
thanks very much! do you mean this derivation/equation isn't correct?

[tex][\int_{0}^{\infty}\frac{a-b}{x}dx+\int_{0}^{\infty }\frac{c^{5/7}-d^{5/7}}{x^{5/7}}dx]... \int_{0}^{1000}(\frac{1}{x})^{\frac{5}{7}}dx\approx25.189[/tex]
but then the integrals don't converge if you integrate to infinity though you can get numerical approximations...in some cases the adiabatic curves will be between the 2 hyperbolae
 
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  • #4
I don't understand what ##x## represents.
 
  • #5
as you know the isotherms seem to be represented by T(P,V)=xy=k graphs of constant temperature so I'd guess x is volume, y is pressure and on the P-V graph the adiabats asymptotically approach both the V and P axes so perhaps perturbation methods could be useful?
http://en.wikipedia.org/wiki/Adiabatic_process
here it says for an ideal gas the work done is the integral of one adiabatic curve between 2 isotherms on a P-V graph
 
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  • #6
mathnerd15 said:
http://en.wikipedia.org/wiki/Adiabatic_process
here it says for an ideal gas the work done is the integral of one adiabatic curve between 2 isotherms on a P-V graph
Exactly. So why are you integrating from ##0## to ##\infty##?
 
  • #7
I was just curious about the integral calculation
 
  • #8
can you construct a proof of the 3rd Law of Thermodynamics in this way since the integral doesn't converge at infinity it takes infinite work to transform a system into absolute zero state?
 
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Related to Work of Carnot Engine integral

1. What is the Work of Carnot Engine Integral?

The Work of Carnot Engine Integral is a mathematical concept used to calculate the maximum possible work output of a Carnot engine. It takes into account the temperature difference between the hot and cold reservoirs of the engine and the efficiency of the engine.

2. How is the Work of Carnot Engine Integral calculated?

The Work of Carnot Engine Integral is calculated using the formula W = Q_h (1 - T_c/T_h), where W is the work output, Q_h is the heat absorbed from the hot reservoir, T_c is the temperature of the cold reservoir, and T_h is the temperature of the hot reservoir. This formula is derived from the Carnot cycle, which is a theoretical cycle that represents the most efficient heat engine.

3. What is the significance of the Work of Carnot Engine Integral?

The Work of Carnot Engine Integral is significant because it represents the theoretical maximum work output of a heat engine. This means that no real engine can ever achieve this amount of work, as some energy is always lost due to factors such as friction and inefficiency. However, the Carnot cycle provides a benchmark for the maximum efficiency that can be attained by a heat engine.

4. How does the Work of Carnot Engine Integral relate to the laws of thermodynamics?

The Work of Carnot Engine Integral is closely related to the first and second laws of thermodynamics. The first law states that energy cannot be created or destroyed, but can only be converted from one form to another. The Work of Carnot Engine Integral takes into account the energy conversion in a heat engine, while the second law states that no engine can be 100% efficient in converting heat into work. The Carnot cycle and the Work of Carnot Engine Integral provide a theoretical limit for the maximum efficiency of a heat engine.

5. How is the Work of Carnot Engine Integral used in practical applications?

The Work of Carnot Engine Integral is primarily used in theoretical and educational contexts, as it represents the maximum efficiency that can be achieved by a heat engine. It is also used to compare the efficiency of real engines to the theoretical limit. However, it is not used in practical applications as it does not take into account real-world factors such as friction and energy losses. Engineers and scientists use other equations and principles to design and improve the efficiency of real heat engines.

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