7. Figure 3 shows the expansion of an ideal gas from initial volume V; = 0.25 m³ and pressure P = 200 kPa to final volume V; = 1 m³ and pressure Pf = 50 kPa. P (kPa) 200 150 100 a) The process depicted in Figure 3 is one of four the following fundamental 50 processes: isobaric, isochoric, isothermal, and adiabatic. Which type of process is it? Why? Explain your answer. V (m² ) 0.25 0.5 0.75 Figure 3 b) Calculate the work done in this process. Show your work.

icon
Related questions
Question
### Problem Statement

Figure 3 shows the expansion of an ideal gas from an initial volume \( V_i = 0.25 \, m^3 \) and pressure \( P_i = 200 \, kPa \) to a final volume \( V_f = 1 \, m^3 \) and pressure \( P_f = 50 \, kPa \).

a) The process depicted in Figure 3 is one of the following four fundamental processes: isobaric, isochoric, isothermal, and adiabatic. Which type of process is it? Why? Explain your answer.

b) Calculate the work done in this process. Show your work.

### Diagram Explanation

The graph (Figure 3) is a plot of pressure \( P \) (in kilopascals) on the vertical axis versus volume \( V \) (in cubic meters) on the horizontal axis. 

- The curve starts at a high pressure and low volume point (200 kPa, 0.25 m\(^3\)) and ends at a low pressure and high volume point (50 kPa, 1 m\(^3\)).
- The curve slopes downwards, indicating that as the volume increases, the pressure decreases.
- This shape is characteristic of an isothermal process, where the temperature remains constant as the ideal gas expands.

### Explanation for Part (a)

The process shown in the graph is isothermal. This conclusion is based on the nature of the graph, which shows a hyperbolic relationship between pressure and volume, consistent with the ideal gas law \( PV = nRT \). In an isothermal process, the temperature remains constant, suggesting the product of pressure and volume is constant for a given amount of gas.

### Solution for Part (b)

To calculate the work done in an isothermal process, use the formula:

\[
W = nRT \ln\left(\frac{V_f}{V_i}\right)
\]

If the number of moles \( n \) and the temperature \( T \) are not given, we can express the work done as:

\[
W = \int_{V_i}^{V_f} P \, dV = nRT \ln\left(\frac{V_f}{V_i}\right)
\]

Under the assumption that the ideal gas is involved, and using the given pressures and volumes, the work done can be evaluated numerically, typically using specific gas
Transcribed Image Text:### Problem Statement Figure 3 shows the expansion of an ideal gas from an initial volume \( V_i = 0.25 \, m^3 \) and pressure \( P_i = 200 \, kPa \) to a final volume \( V_f = 1 \, m^3 \) and pressure \( P_f = 50 \, kPa \). a) The process depicted in Figure 3 is one of the following four fundamental processes: isobaric, isochoric, isothermal, and adiabatic. Which type of process is it? Why? Explain your answer. b) Calculate the work done in this process. Show your work. ### Diagram Explanation The graph (Figure 3) is a plot of pressure \( P \) (in kilopascals) on the vertical axis versus volume \( V \) (in cubic meters) on the horizontal axis. - The curve starts at a high pressure and low volume point (200 kPa, 0.25 m\(^3\)) and ends at a low pressure and high volume point (50 kPa, 1 m\(^3\)). - The curve slopes downwards, indicating that as the volume increases, the pressure decreases. - This shape is characteristic of an isothermal process, where the temperature remains constant as the ideal gas expands. ### Explanation for Part (a) The process shown in the graph is isothermal. This conclusion is based on the nature of the graph, which shows a hyperbolic relationship between pressure and volume, consistent with the ideal gas law \( PV = nRT \). In an isothermal process, the temperature remains constant, suggesting the product of pressure and volume is constant for a given amount of gas. ### Solution for Part (b) To calculate the work done in an isothermal process, use the formula: \[ W = nRT \ln\left(\frac{V_f}{V_i}\right) \] If the number of moles \( n \) and the temperature \( T \) are not given, we can express the work done as: \[ W = \int_{V_i}^{V_f} P \, dV = nRT \ln\left(\frac{V_f}{V_i}\right) \] Under the assumption that the ideal gas is involved, and using the given pressures and volumes, the work done can be evaluated numerically, typically using specific gas
Expert Solution
steps

Step by step

Solved in 3 steps with 3 images

Blurred answer