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A gas, while expanding under isobaric conditions, does \(480 \mathrm{J}\) of work. The pressure of the gas is \(1.6 \times 10^{5} \mathrm{Pa}\), and its initial volume is \(1.5 \times 10^{-3} \mathrm{m}^{3} .\) What is the final volume of the gas?

Short Answer

Expert verified
The final volume of the gas is \(4.5 \times 10^{-3} \text{ m}^3\).

Step by step solution

01

Understand the Formula for Work Done

Under isobaric (constant pressure) conditions, the work done by the gas is given by the formula \( W = P \times \Delta V \), where \( W \) is the work done, \( P \) is the pressure, and \( \Delta V \) is the change in volume of the gas.
02

Substitute Known Values

We know the work done \( W = 480 \text{ J} \) and the pressure \( P = 1.6 \times 10^{5} \text{ Pa} \). We need to find the change in volume \( \Delta V = V_f - V_i \), where \( V_i = 1.5 \times 10^{-3} \text{ m}^3 \). Substitute these values into the work formula: \( 480 = 1.6 \times 10^{5} \times \Delta V \).
03

Solve for Change in Volume

Rearrange the formula to solve for \( \Delta V \): \( \Delta V = \frac{480}{1.6 \times 10^{5}} \). Calculate \( \Delta V \) to determine the change in volume.
04

Calculate \( \Delta V \)

Perform the division: \( \Delta V = \frac{480}{1.6 \times 10^{5}} = 3 \times 10^{-3} \text{ m}^3 \). This is the change in volume from the initial volume to the final volume.
05

Determine the Final Volume

Using the equation \( V_f = V_i + \Delta V \), substitute in the known values: \( V_f = 1.5 \times 10^{-3} \text{ m}^3 + 3 \times 10^{-3} \text{ m}^3 \).
06

Calculate the Final Volume

Add the initial volume and the change in volume: \( V_f = 4.5 \times 10^{-3} \text{ m}^3 \). This is the final volume of the gas.

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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 discussing the work done by a gas during an isobaric process, we are referring to the amount of energy transferred by the gas as it expands at constant pressure. The key formula to remember here is:
  • \( W = P \times \Delta V \)
  • Where:
    • \( W \) is the work done by the gas
    • \( P \) is the pressure
    • \( \Delta V \) is the change in volume
In our particular problem, the gas does work totaling 480 J. The pressure remains constant at \(1.6 \times 10^{5} \text{ Pa} \), highlighting the isobaric nature of the process. It's important to understand this relationship as it illustrates how pressure and volume changes translate to work being done. If there is a change in volume and the pressure stays the same, energy is being transferred either into or out of the system.
change in volume
The change in volume is a crucial part of understanding the isobaric process in thermodynamics. In this scenario, we are given the initial volume and need to calculate the change in volume, \( \Delta V \), during the gas expansion.

Knowing the work done by the gas (480 J) and the constant pressure (\(1.6 \times 10^{5} \text{ Pa} \)), we use the formula \( W = P \times \Delta V \) to find \( \Delta V \):
  • Rearranging gives us: \( \Delta V = \frac{W}{P} \)
  • Substituting the known values: \( \Delta V = \frac{480}{1.6 \times 10^{5}} \)
  • Calculating \( \Delta V \): \( \Delta V = 3 \times 10^{-3} \mathrm{m}^{3} \)
This means the volume of the gas increases by \( 3 \times 10^{-3} \mathrm{m}^{3} \) due to the work performed by the gas while expanding against constant pressure. Understanding the change in volume helps you visualize how the initial and final state of the gas relates under constant pressure.
final volume calculation
Determining the final volume of the gas after expansion is straightforward once you know the initial volume and the change in volume. In this exercise, the initial volume of the gas is given as \( 1.5 \times 10^{-3} \mathrm{m}^{3} \). With the change in volume known from previous steps, calculating the final volume involves a simple addition:
  • Use the equation: \( V_f = V_i + \Delta V \)
  • Substitute into it: \( V_f = 1.5 \times 10^{-3} \text{ m}^3 + 3 \times 10^{-3} \text{ m}^3 \)
  • Performing the addition gives us: \( V_f = 4.5 \times 10^{-3} \text{ m}^3 \)
This calculation clearly shows that the gas expanded to reach a final volume of \( 4.5 \times 10^{-3} \text{ m}^3 \). In real-life applications, understanding how to reach this final volume through calculations helps in examining the efficiency and effectiveness of a thermodynamic process.

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Most popular questions from this chapter

A Carnot engine operates with an efficiency of \(27.0 \%\) when the temperature of its cold reservoir is \(275 \mathrm{K}\). Assuming that the temperature of the hot reservoir remains the same, what must be the temperature of the cold reservoir in order to increase the efficiency to \(32.0 \% ?\)

Even at rest, the human body generates heat. The heat arises because of the body's metabolism - that is, the chemical reactions that are always occurring in the body to generate energy. In rooms designed for use by large groups, adequate ventilation or air conditioning must be provided to remove this heat. Consider a classroom containing 200 students. Assume that the metabolic rate of generating heat is \(130 \mathrm{W}\) for each student and that the heat accumulates during a fifty-minute lecture. In addition, assume that the air has a molar specific heat of \(C_{V}=\frac{5}{2} R\) and that the room (volume \(=1200 \mathrm{m}^{3},\) initial pressure \(=1.01 \times 10^{5} \mathrm{Pa}\), and initial temperature \(=21^{\circ} \mathrm{C}\) ) is sealed shut. If all the heat generated by the students were absorbed by the air, by how much would the air temperature rise during a lecture?

A Carnot air conditioner maintains the temperature in a house at \(297 \mathrm{K}\) on a day when the temperature outside is \(311 \mathrm{K}\). What is the coefficient of performance of the air conditioner?

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