Work done by gas in adiabatic process

In summary: But this is the same as the previous equation - just rearranged.In summary, for an ideal gas in an adiabatic process, the work done is equal to (PfVf - PiVi) / (1 - γ). This is equivalent to the formula given in the link provided, and can also be derived using the first law of thermodynamics. The two equations are just rearranged versions of each other.
  • #1
collectedsoul
76
0
In an adiabatic process PVγ=constant

Now I thought the work done by an ideal gas in an adiabatic process was given by the equation here: http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/adiab.html

But while doing a GRE question the answer was given as PfVf - PiVi / 1 - γ

Is this correct (it must be!)? And if so why haven't I seen this equation anywhere before?
 
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  • #2
I think the two are equivalent. Reexpress the formula in the link using, for an adiabatic process, $$P_1 V_1^{\gamma} = P_2 V_2^{\gamma}$$
 
  • #3
collectedsoul said:
In an adiabatic process PVγ=constant

Now I thought the work done by an ideal gas in an adiabatic process was given by the equation here: http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/adiab.html

But while doing a GRE question the answer was given as PfVf - PiVi / 1 - γ

Is this correct (it must be!)? And if so why haven't I seen this equation anywhere before?

Did you mean that the GRE answer was W = (PfVf - PiVi) / (1 - γ) ?

Since it is a reversible adiabatic process (Q=0), the work done BY the gas has to be equal and opposite to its change in internal energy: W = - ΔU (first law).

For an ideal gas, ΔU = nCvΔT = nCv(γ-1)/(γ-1)ΔT = nRΔT/(γ-1) = Δ(PV)/(γ-1) = (PfVf - PiVi)/(γ-1).

AM
 
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  • #4
Alternatively, $$P_i V_i^{\gamma} = P_f V_f^{\gamma} = K \Rightarrow KV_i^{1-\gamma} = P_iV_i\,\,\text{and}\,\,KV_f^{1-\gamma} = P_fV_f$$
Then sub in.
 
  • #5


Yes, the equation given in the GRE question is correct. The work done by an ideal gas in an adiabatic process can be calculated using the equation W = (PfVf - PiVi) / (1 - γ), where Pf and Vf are the final pressure and volume of the gas, Pi and Vi are the initial pressure and volume of the gas, and γ is the adiabatic index.

This equation is derived from the first law of thermodynamics, which states that the change in internal energy of a system is equal to the heat added to the system minus the work done by the system. In an adiabatic process, there is no heat exchange between the gas and its surroundings, so the change in internal energy is equal to the work done by the gas.

The equation you have seen before, PVγ=constant, is known as the adiabatic equation of state. It is derived from the ideal gas law and is used to describe the relationship between pressure and volume in an adiabatic process. However, this equation does not directly give the work done by the gas.

The equation given in the GRE question is a more specific and accurate representation of the work done by an ideal gas in an adiabatic process. It takes into account the initial and final states of the gas, as well as the adiabatic index, which is a measure of the gas's ability to transfer heat. This equation is commonly used in thermodynamics and can be found in many textbooks and online resources.
 

FAQ: Work done by gas in adiabatic process

What is work done by gas in adiabatic process?

Work done by gas in adiabatic process is the energy transferred to or from a system as a result of a force acting on a moving object in an adiabatic process. In other words, it is the energy required to change the state of a gas from one pressure to another without any heat transfer.

What is the formula for work done by gas in adiabatic process?

The formula for work done by gas in adiabatic process is W = (P2V2 - P1V1) / (1-n), where W is the work done, P is the pressure, V is the volume, and n is the ratio of specific heats of the gas.

How is work done by gas in adiabatic process related to temperature and volume?

In an adiabatic process, if the volume of a gas decreases, the temperature of the gas increases and work is done by the gas. Similarly, if the volume of a gas increases, the temperature decreases and work is done on the gas.

What is the difference between isothermal and adiabatic processes?

The main difference between isothermal and adiabatic processes is that in an isothermal process, the temperature remains constant while the volume changes, whereas in an adiabatic process, there is no heat transfer and the temperature changes as the volume changes.

What are some real-life examples of adiabatic processes?

Some real-life examples of adiabatic processes include the compression of air in a bicycle pump, the expansion of air in a car engine, and the compression of a gas in a refrigerator. These processes are also commonly used in the production of compressed air and in the operation of gas turbines.

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