/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 22 A gas at a pressure of 2.00 atm ... [FREE SOLUTION] | 91Ó°ÊÓ

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A gas at a pressure of 2.00 atm undergoes a quasistatic isobaric expansion from 3.00 to 5.00 L. How much work is done by the gas?

Short Answer

Expert verified
The work done by the gas during the quasistatic isobaric expansion is \(405.3 \, Joules\).

Step by step solution

01

Identify the given values and the formula for work done in an isobaric process

We are given the following: Pressure (P) = 2.00 atm Initial volume (V1) = 3.00 L Final volume (V2) = 5.00 L The formula for work done in an isobaric process is: Work (W) = Pressure × Change in Volume
02

Convert the pressure to a consistent unit

Since we are working with the volume in liters, we need to convert the pressure from atm to the consistent unit, which is Joules. We can use the conversion factor: 1 atm = 101.325 J/L So, Pressure (P) = 2.00 atm × 101.325 J/L = 202.65 J/L
03

Calculate the change in volume

Now, we have to find the change in volume during the isobaric expansion process: Change in Volume = Final Volume - Initial Volume = V2 - V1 Change in Volume = 5.00 L - 3.00 L = 2.00 L
04

Calculate the work done by the gas

Finally, we can use the formula for work done in an isobaric process to calculate the work done by the gas: Work (W) = Pressure × Change in Volume W = 202.65 J/L × 2.00 L W = 405.3 J So, the work done by the gas during the quasistatic isobaric expansion is 405.3 Joules.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Work Done by Gas
When a gas undergoes expansion or compression, it can do work on its surroundings or have work done on it.
In an isobaric process, which means the pressure remains constant, we need to calculate the work done during the expansion of the gas. The formula for work done in an isobaric process is: \[W = P \times \Delta V\]Where:- \(W\) is the work done by the gas, - \(P\) is the constant pressure, and - \(\Delta V\) is the change in volume of the gas.
The work done is positive if the system (gas) does work on the surroundings, as in expansion. Conversely, it is negative if work is done on the system.
In the given exercise, the gas expands from 3.00 L to 5.00 L under a constant pressure of 2.00 atm, doing 405.3 Joules of work on its surroundings.
Quasistatic Expansion
A quasistatic process is a hypothetical process that happens infinitely slowly, so that the system is always in equilibrium.
This idealization allows us to assume each state of the gas as a state of thermal and mechanical equilibrium. In practice, a true quasistatic process can't occur because processes take time and systems achieve equilibrium gradually.
For calculations, however, assuming quasistatic conditions simplifies analysis and provides good approximations.
During the quasistatic isobaric expansion of the gas, it goes from one volume to another at equilibrium, allowing the direct application of the work formula for isobaric processes. Thus, it enables straightforward application of the work done formula for this case.
Pressure-Volume Work
Pressure-volume work is a key concept in thermodynamics related to the energy transferred in the form of work. When a system expands or is compressed, the energy exchange involves pressure and volume change.
In the formula \(W = P \times \Delta V\), pressure-volume work is specifically related to scenarios where there's a volume change at constant pressure (isobaric process).
The important details in calculating this work:
  • Ensure the pressure is in the correct units (e.g., converting atm to J/L if volume is in liters).
  • Calculate the change in volume by subtracting the initial volume from the final volume.
  • Multiply the consistent pressure by the calculated change in volume.
This approach allows for a straightforward calculation of the work done, as demonstrated in the example where 405.3 J of work is calculated for the given gas expansion.

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Most popular questions from this chapter

The insulated cylinder shown below is closed at both ends and contains an insulating piston that is free to move on frictionless bearings. The piston divides the chamber into two compartments containing gases A and B. Originally, each compartment has a volume of \(5.0 \times 10^{-2} \mathrm{m}^{3}\) and contains a monatomic ideal gas at a temperature of \(0^{\circ} \mathrm{C}\) and a pressure of 1.0 atm. (a) How many moles of gas are in each compartment? (b) Heat Q is slowly added to A so that it expands and \(\mathrm{B}\) is compressed until the pressure of both gases is 3.0 atm. Use the fact that the compression of \(\mathrm{B}\) is adiabatic to determine the final volume of both gases. (c) What are their final temperatures? (d) What is the value of Q?

A cylinder containing three moles of a monatomic ideal gas is heated at a constant pressure of 2 atm. The temperature of the gas changes from \(300 \mathrm{K}\) to \(350 \mathrm{K}\) as a result of the expansion. Find work done (a) on the gas; and (b) by the gas.

An ideal gas expands isothermally along AB and does 700 J of work (see below). (a) How much heat does the gas exchange along AB? (b) The gas then expands adiabatically along BC and does 400 J of work. When the gas returns to A along CA, it exhausts 100 J of heat to its surroundings. How much work is done on the gas along this path?

Four moles of a monatomic ideal gas in a cylinder at \(27^{\circ} \mathrm{C}\) is expanded at constant pressure equal to \(1 \mathrm{atm}\) until its volume doubles. (a) What is the change in internal energy? (b) How much work was done by the gas in the process? (c) How much heat was transferred to the gas?

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