Work done by ideal gas processes

In summary, work done by ideal gas processes is represented by the equation Wgas = pΔV and can be either positive or negative depending on the convention used. In the energy equation, work is represented as Wnet,ext and can be positive or negative depending on whether it is work done on or by the gas. The convention used for work in these equations can change depending on the focus of attention.
  • #1
ahyaa
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Hello all,

In my physics textbook they discuss work done by ideal gas processes. The equation they give is Wgas = pΔV. I'm trying to figure it out if this is work done ON the gas by the surroundings, or work done BY the gas on surroundings.

From a previous chapter, they presented the conservation of energy equation as Ei + Wnet,ext = Ef. Work in this equation is the net, external work on the system, such that +W is work by the surroundings on the system, and -W is work by the system on the surroundings. It would seem from this preliminary chapter that we would be defining any W as work ON the system by surroundings.

However Wgas can't possibly be work done ON the gas, because if a gas is expanding, it supposedly has +Wgas even though it is doing work on the surroundings (therefore Wnet,ext should be negative). Could anybody confirm my thinking and does anybody know a good way to distinguish these two?
 
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  • #2
You pretty much have it. It all depends on the convention used, so if you take
$$
W_\mathrm{gas} = p \Delta V
$$
then ##W_\mathrm{gas} > 0## for work done by the gas (i.e., ##\Delta V > 0##).

In the energy equation
$$
E_i + W_\mathrm{net,ext} = E_f
$$
##W_\mathrm{net,ext} > 0## for work done on the gas. Therefore,
the total work will read
$$
W_\mathrm{net,ext} = -W_\mathrm{gas} + W_\mathrm{other}
$$

I must say that it is a strange convention: you usually would take the sign of ##W## to mean on/by directly. But it happens that depending on the situation, you would take one convention or the other depending on if the gas is the focus of attention or not. I know a textbook where the convention changes between two chapters, as it goes from looking at the properties of ideal gases to heat engines.
 
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  • #3
Rather than keeping track of which convention is being used, I remember that work is positive when the force is exerted in the direction of motion. So for an expanding gas, the force exerted on the surroundings (by the gas) is in the direction of motion, while the force exerted on the gas (by the surroundings) is against the direction of motion. So, positive work is done on the surroundings, negative work is done on the gas.
 
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FAQ: Work done by ideal gas processes

What is work done by an ideal gas?

The work done by an ideal gas is the energy transferred to or from the gas due to a change in volume. This can occur during a compression or expansion process.

What is the equation for work done by an ideal gas?

The equation for work done by an ideal gas is W = PΔV, where W is work, P is pressure, and ΔV is the change in volume.

What are some examples of ideal gas processes?

Some examples of ideal gas processes include isothermal, adiabatic, isobaric, and isochoric processes. These processes involve changes in pressure, volume, and temperature of an ideal gas.

How does work done by an ideal gas relate to the first law of thermodynamics?

The first law of thermodynamics 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 the case of an ideal gas, the work done is equal to the change in internal energy of the gas, as there is no heat transfer.

What factors affect the work done by an ideal gas?

The work done by an ideal gas is affected by factors such as the initial and final volume of the gas, the pressure of the gas, and the type of process (isothermal, adiabatic, etc.). The work done can also be influenced by external factors such as friction or heat exchange with the surroundings.

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