Closed cycle of an ideal gas

In summary, a closed cycle of an ideal gas refers to a thermodynamic process where the gas undergoes a series of transformations that return it to its initial state. Throughout the cycle, the gas may experience changes in pressure, volume, and temperature while exchanging heat and doing work. The net work done by the gas over one complete cycle is equal to the area enclosed by the cycle on a pressure-volume (P-V) diagram. This concept is fundamental in understanding heat engines and the principles of thermodynamics.
  • #1
imdesperate
2
1
Homework Statement
An ideal gas (degree of freedom = 5) is in a closed cycle like the given figure. Find the efficiency of the cycle.
Relevant Equations
##\Delta U = A + Q##
##\eta = \frac{-A}{Q_+}##
Capture.PNG

Hello PF, this is my first time posting here. I will try my best to make my formulas readable.

So I know what needed to be done:
The efficiency is calculated by the formula: ##\eta = \frac{-A}{Q_+}##
With ##A## being the total work done in the cycle, ##Q_+## being the heat absorbed in the cycle. The opposite of ##Q_+## is ##Q_-## being the heat released.

Heat ratio ##\gamma = 1 + \frac2 i = 1 + \frac2 5 = \frac7 5 ## (notated degree of freedom as i).

First, I calculated the pressure and volume of each state using the relation of each process.
For process (1-2): isothermal, I calculated ##p_2## using
##p_1 * V_1 = p_2 * V_2##
##p_2 = \frac5 3 * 10^5 Pa##
For process (2-3): adiabatic, I calculated ##V_3## using
##p_2 * (V_2)^\gamma = p_3 * (V_3)^\gamma##
##V_3 = 12.96 * 10^{-3} m^3##
For process (3-4): isobaric, so ##p_3 = p_4 = 10^5 Pa##.
For process (4-1): isochoric, so ##p_4 = p_1= 3* 10^{-3} m^3##.

Then, I can calculate the work done for each process.

(1-2): isothermal, ##A_{12} = nRT\ln(\frac{V_1}{V_2}) = pV\ln(\frac{V_1}{V_2}) = -1647.92 J##
(2-3): adiabatic, ##A_{23} = \frac{p_2 * V_2 - p_3 * V_3} {\gamma - 1} = 509.25 J##
(3-4): isobaric, ##A_{34} = p * (V_3 - V_4) = 996.3 J##
(4-1): isochoric, ##A_{41} = 0 J##
So ##A = A_{12} + A_{23} + A_{34} + A_{41} = -142.37 J##

I proceeded to calculate the heat absorbed or released for each process.

(1-2): isothermal, ##Q_{12} = -A_{12} = 1647.92 J > 0## so ##Q_{12}## is ##Q_{+12}##
(2-3): adiabatic, ##Q_{23} = 0 J##
(3-4): isobaric, ##Q_{34} = n * C_p * (T_4 - T_3)##. with ##C_p = (\frac i 2 + 1)R## (##R## is the gas constant)
(4-1): isochoric, ##Q_{41} = n* C_v *(T_1 - T_4)##, with ##C_v = \frac{iR}{2}##

The problem starts here, I was not given the moles for the gas (I have confirmed this with my teacher).

I tried to calculate the temperature T for each state. By using the relation of each process, I managed to figure out the relation between the temperature: $$T_1 = T_2 = \frac{5T_3}{\frac{V3}{V4}} = 5T_4$$.

I've gotten these through

(1-2): isothermal, ##T_1 = T_2##;
(3-4): isobaric, ##T_3 = (\frac{V_3}{V_4})T_4##;
(4-1): isochoric, ##T_1 = 5T_4##.

I've used using the formula ##\Delta U = A + Q## to try and find any kind of equation to calculate the temperature, but I've gotten nowhere, all the results I got are the same relation I'd gotten from earlier ##(T_1 = T_2 = \frac{5T_3}{\frac{V3}{V4}} = 5T_4)##

I would like a hint on where to start!
 
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  • #2
You don't need the number of moles to calculate the efficiency. The efficiency is a ratio with ##n## in the numerator and the denominator which will eventually cancel. First express all pressures and volumes in terms of ##p_1## and ##V_1##.

A convenient way to summarize your results would be to make a Table as show below and fill in the entries. Use symbols instead of numbers. You can always substitute numbers at the very end. I already put in the zero that you found, there are more. Be sure that the totals are what they should be over a complete cycle. The total in column ##W## divided by the sum of the positive entries in column ##Q## is the efficiency.
$$\Delta U$$$$Q$$$$W$$
$$1\rightarrow 2$$
$$2\rightarrow 3$$
$$3\rightarrow 4$$
$$4\rightarrow 1$$$$0$$
$$\rm{TOTAL}$$
 
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Likes WWGD and imdesperate
  • #3
Well I did it.
I used ##T_1 = 5T_4## to figure out ##Q_{41}## is positive. Then, I put them all in the formula and converted all pressures and volumes into ##p_1## and ##V_1##. I also converted all the temperatures into the form ##\frac{pV}{nR}## which made ##nR## cancel out. Finally I got ##0.0306## as the answer.

Thank you so much!
 
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Likes WWGD
  • #4
imdesperate said:
Well I did it.
I used ##T_1 = 5T_4## to figure out ##Q_{41}## is positive. Then, I put them all in the formula and converted all pressures and volumes into ##p_1## and ##V_1##. I also converted all the temperatures into the form ##\frac{pV}{nR}## which made ##nR## cancel out. Finally I got ##0.0306## as the answer.

Thank you so much!
I got a higher value or the efficiency by an order of magnitude. You don't show the numbers that went in your calculation. If you wish to pursue this further, please show your efficiency calculation so that we can pinpoint the problem with it. Remember, the efficiency is the total work done by the gas divided by the total amount of heat that enters the gas.
 

FAQ: Closed cycle of an ideal gas

1. What is a closed cycle of an ideal gas?

A closed cycle of an ideal gas refers to a thermodynamic process in which the gas undergoes a series of transformations that return it to its initial state. During this cycle, the gas may absorb heat, perform work, and undergo changes in pressure and volume, but ultimately, the overall change in internal energy and temperature is zero when the cycle is complete.

2. What are the main types of closed cycles for ideal gases?

The main types of closed cycles for ideal gases include the Carnot cycle, Otto cycle, and Diesel cycle. The Carnot cycle is an idealized model that represents the maximum efficiency of a heat engine, while the Otto and Diesel cycles are practical models used in internal combustion engines, each having distinct processes for compression and combustion.

3. How is work done by an ideal gas in a closed cycle?

Work done by an ideal gas in a closed cycle can be calculated using the area enclosed by the process path on a pressure-volume (P-V) diagram. The work is positive when the gas expands (doing work on the surroundings) and negative when the gas is compressed (work done on the gas). The total work done in the cycle is the net area enclosed by the path on the P-V diagram.

4. What is the significance of the first law of thermodynamics in a closed cycle?

The first law of thermodynamics states that energy cannot be created or destroyed, only transferred or transformed. In a closed cycle, this means that the heat added to the system minus the work done by the system equals the change in internal energy. Since the internal energy returns to its original state after the cycle, the net change is zero, leading to the conclusion that the heat added to the system is equal to the work done by the system over the entire cycle.

5. How does the efficiency of a closed cycle relate to the ideal gas behavior?

The efficiency of a closed cycle for an ideal gas is determined by the ratio of the work output to the heat input. For ideal gases, the efficiency can be maximized by optimizing the processes involved in the cycle, such as maximizing the temperature difference between the heat source and sink in the Carnot cycle. However, real gases may deviate from ideal behavior, affecting the efficiency and performance of the cycle.

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