Work done during quasi-static, isothermal expansion from P_i to P_f

In summary, during a quasi-static, isothermal expansion from an initial pressure (P_i) to a final pressure (P_f), the system undergoes a slow and controlled process that allows it to remain in equilibrium with its surroundings. The work done by the system can be calculated using the integral of pressure with respect to volume, reflecting the transfer of energy as the gas expands while maintaining a constant temperature. This process is characterized by the absorption of heat from the surroundings to offset the work done, in accordance with the first law of thermodynamics.
  • #1
zenterix
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Homework Statement
(a) Show that the work done by an ideal gas during the quasi-static, isothermal expansion from an initial pressure ##P_i## to a final pressure ##P_f## is given by

$$W=nRT\ln\frac{P_f}{P_i}$$

(b) Calculate the work done when the pressure of 1 mol of an ideal gas is decreased quasi-statically from 20 to 1 atm, the temperature remaining constant at ##20^{\circ} C## (##R=8.31 J/mol\cdot deg##).
Relevant Equations
##W=-\int_{V_i}^{V_f} PdV##
I am posting this question after I thought I had easily solved the problem, but then when I checked the back of the book I saw that I was incorrect.

Here is what I did.

(a)

$$W=-\int_{V_i}^{V_f} PdV\tag{1}$$

$$V=V(P,T)-\frac{nRT}{P}\tag{2}$$

$$dV=\left ( \frac{\partial V}{\partial P}\right )_T dP+\left ( \frac{\partial V}{\partial T} \right )_P dT\tag{3}$$

$$=\frac{-nRT}{P^2}dP\tag{4}$$

Now we plug (4) into (1)

$$W=\int_{P_i}^{P_f} \frac{nRT}{P}dP=nRT\ln{\frac{P_f}{P_i}}\tag{5}$$

(b)

At this point I simply plugged the values into (5)

$$W=1\text{mol}\cdot 8.31 \mathrm{\frac{J}{mol ^\circ C}}\cdot 20^{\circ} \text{C}\cdot \ln{\frac{1\text{atm}}{20\text{atm}}}\tag{6}$$

$$=-7294\text{J}\tag{7}$$

The book answer says ##-3.17\times 10^3## J.
 
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  • #2
zenterix said:
(b)

At this point I simply plugged the values into (5)

$$W=1\text{mol}\cdot 8.31 \mathrm{\frac{J}{mol ^\circ C}}\cdot 20^{\circ} \text{C}\cdot \ln{\frac{1\text{atm}}{20\text{atm}}}\tag{6}$$

$$=-7294\text{J}\tag{7}$$

The book answer says ##-3.17\times 10^3## J.
Be careful: indicate that you converted the 20 °C to kelvin. Otherwise, I get the same answer as you.
 
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  • #3
zenterix said:
$$W=-\int_{V_i}^{V_f} PdV\tag{1}$$

$$V=V(P,T)-\frac{nRT}{P}\tag{2}$$
Where did you get Eqn. 2 from?

Incidentally, you could have done the initial derivation differently by using the product rule for differentiation: $$PdV=d(PV)-VdP$$At constant temperature, d(PV)=nRdT=0, so, at constant temperature, $$PdV=-VdP=-\frac{nRT}{P}dp$$
 
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  • #4
DrClaude said:
Be careful: indicate that you converted the 20 °C to kelvin. Otherwise, I get the same answer as you.
Indeed, I did use Kelvin.
 
  • #5
Chestermiller said:
Where did you get Eqn. 2 from?

Incidentally, you could have done the initial derivation differently by using the product rule for differentiation: $$PdV=d(PV)-VdP$$At constant temperature, d(PV)=nRdT=0, so, at constant temperature, $$PdV=-VdP=-\frac{nRT}{P}dp$$
Equation 2 comes from the equation of state for ideal gases. I think you may be asking because of the typo I have in that equation.

It should be

$$V=V(P,T)=\frac{nRT}{P}$$

I accidentally had a minus sign in place of the second equals sign.
 
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FAQ: Work done during quasi-static, isothermal expansion from P_i to P_f

What is a quasi-static process?

A quasi-static process is an idealized or hypothetical process that occurs infinitely slowly, allowing the system to remain in thermodynamic equilibrium at all times. This means that the process is reversible and can be reversed by an infinitesimally small change in external conditions.

What is meant by isothermal expansion?

Isothermal expansion refers to the expansion of a gas at a constant temperature. During this process, the temperature of the gas does not change, which implies that the internal energy of the gas remains constant if we are dealing with an ideal gas.

How is the work done calculated during a quasi-static, isothermal expansion?

The work done during a quasi-static, isothermal expansion of an ideal gas can be calculated using the formula: \( W = nRT \ln\left(\frac{V_f}{V_i}\right) \), where \( n \) is the number of moles of the gas, \( R \) is the universal gas constant, \( T \) is the absolute temperature, \( V_f \) is the final volume, and \( V_i \) is the initial volume. Alternatively, it can also be expressed in terms of pressure as \( W = nRT \ln\left(\frac{P_i}{P_f}\right) \).

Why is the temperature constant in an isothermal process?

The temperature remains constant in an isothermal process because the system is in thermal equilibrium with a heat reservoir at a fixed temperature. Any heat added to the system is used to do work, and the internal energy of an ideal gas remains constant, ensuring that the temperature does not change.

What is the significance of the logarithmic relationship in the work done formula?

The logarithmic relationship in the work done formula, \( W = nRT \ln\left(\frac{V_f}{V_i}\right) \) or \( W = nRT \ln\left(\frac{P_i}{P_f}\right) \), signifies that the work done depends on the ratio of the final and initial volumes or pressures. This relationship arises from the integration of the pressure-volume work equation for an ideal gas under isothermal conditions, reflecting the continuous and gradual nature of the quasi-static process.

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