Act like a helpful tutor and exlain me :
Give step-by-step solution with explanation and final answer:explain completeley , Carbon dioxide
(
CO
2
)
is compressed in a piston
-
cylinder assembly from p
1
=
0
.
7
bar, T
1
=
2
8
0
K to p
2
=
1
0
bar. The initial volume is
0
.
2
m
3
.
The process is described by pV
1
2
5
=
constant. Assuming ideal gas behavior and neglecting kinetic and potential energy effects, determine the work and heat transfer for the process, each in kJ
,
using constant specific heats evaluated at
3
0
0
K
,
and data from Table A
-
2
3
.
Part A Determine the work for the process, in kJ
.
Part B Determine the heat transfer process, in kJ
,
using constant specific heats.
Question:
Act like a helpful tutor and exlain me :
Give step-by-step solution with explanation and final answer:explain completeley , Carbon dioxide
(
CO
2
)
is compressed in a piston
-
cylinder assembly from p
1
=
0
.
7
bar, T
1
=
2
8
0
K to p
2
=
1
0
bar. The initial volume is
0
.
2
m
3
.
The process is described by pV
1
2
5
=
constant. Assuming ideal gas behavior and neglecting kinetic and potential energy effects, determine the work and heat transfer for the process, each in kJ
,
using constant specific heats evaluated at
3
0
0
K
,
and data from Table A
-
2
3
.
Part A Determine the work for the process, in kJ
.
Part B Determine the heat transfer process, in kJ
,
using constant specific heats.
This is AI generated Response.
Asked by: manish kumar
Created at: 2025-10-22 01:49:28
Final Answer:
RenderedRaw Text
Did you like this answer?
# Problem Overview
We are analyzing the compression process of carbon dioxide (\( \mathrm{CO_2} \)) in a piston-cylinder assembly. The initial and final states are given, and the process follows a specific relation. Our goal is to find:
- **Part A:** The work done during the process (in kJ).
**Part B:** The heat transfer the process ( kJ).
# Given Data
| Parameter | Value |
|------------------------------|-------------------------------------|
| Initial pressure, \( p_1 \) | .7 bar |
| Initial temperature, \( T_1 \) | 280 K |
| Final pressure, \( p_2 \) | 10 bar |
| Initial volume, \( V_1 \) | .2 m³ |
| Process relation | \( p V^{\frac{5}{2}} = \text{constant} \) |
| Gas behavior | Ideal gas |
| Specific heats (constant) | \( C_p \), \( C_v \) at 300 K (from Table A-23) |
---
# Step-by-Step Solution
## Part A: Find the work done, \( W \)
### Step 1: Find initial and final states
- Convert initial pressure from bar to kPa:
\[
p_1 = .7\, \text{bar} = 70\, \text{kPa}
\]
- Final pressure:
\[
p_2 = 10\, \text{bar} = 100\, \text{kPa}
\]
- Use ideal gas law:
\[
p V = R T
\]
where \( R \) for \( \mathrm{CO_2} \) (molar gas constant):
\[
R_{CO_2} = .1889\, \text{kJ/(kg·K)}
\]
### Step 2: Find initial specific volume, \( v_1 \)
\[
v_1 = \frac{V_1}{m}
\]
But since \( V_1 \) is given, and \( p_1, T_1 \) are known:
\[
p_1 v_1 = R T_1
\]
\[
v_1 = \frac{R T_1}{p_1} = \frac{.1889 \times 280}{70} \approx .756\, \text{m}^3/\text{kg}
\]
### Step 3: Find the final specific volume, \( v_2 \)
Given the process relation:
\[
p v^{\frac{5}{2}} = \text{constant}
\]
\[
p_1 v_1^{\frac{5}{2}} = p_2 v_2^{\frac{5}{2}}
\]
Solve for \( v_2 \):
\[
v_2 = v_1 \left( \frac{p_1}{p_2} \right)^{\frac{2}{5}}
\]
Calculate:
\[
v_2 = .756 \times \left( \frac{70}{100} \right)^{.4}
\]
\[
\left( \frac{70}{100} \right)^{.4} \approx (.07)^{.4} \approx .265
\]
\[
v_2 \approx .756 \times .265 \approx .2\, \text{m}^3/\text{kg}
\]
### Step 4: Find the mass of the gas
\[
m = \frac{V_1}{v_1} = \frac{.2}{.756} \approx .264\, \text{kg}
\]
---
### Step 5: Calculate the work done
For a polytropic process:
\[
W = \frac{p_2 V_2 - p_1 V_1}{1 - n}
\]
where \( n = \frac{5}{2} = 2.5 \). But it's easier to express in specific volume:
\[
W = m \times \frac{p_2 v_2 - p_1 v_1}{1 - n}
\]
Convert pressures to kPa:
\[
W = .264 \times \frac{100 \times .2 - 70 \times .756}{1 - 2.5}
\]
Calculate numerator:
\[
100 \times .2 = 200\, \text{kPa·m}^3
\]
\[
70 \times .756 \approx 52.92\, \text{kPa·m}^3
\]
Difference:
\[
200 - 52.92 \approx 147.08\, \text{kPa·m}^3
\]
Since the denominator:
\[
1 - 2.5 = -1.5
\]
Finally:
\[
W = .264 \times \frac{147.08}{-1.5} \approx .264 \times (-98.05) \approx -25.87\, \text{kJ}
\]
**Note:** Negative work indicates work done **on** the gas (compression).
---
## **Final Answer for Part A:**
\[
\boxed{
W \approx \mathbf{-25.87\, \text{kJ}}
}
\]
---
## Part B: Find the heat transfer, \( Q \)
### Step 1: Use the first law of thermodynamics:
\[
Q = \Delta U + W
\]
where:
\[
\Delta U = m C_v (T_2 - T_1)
\]
### Step 2: Find \( T_2 \)
Using ideal gas law at state 2:
\[
T_2 = \frac{p_2 v_2}{R} = \frac{100 \times .2}{.1889} \approx 1058\, \text{K}
\]
### Step 3: Find \( C_v \)
From Table A-23 (assuming typical values for \( \mathrm{CO_2} \) at 300 K):
\[
C_v \approx .658\, \text{kJ/(kg·K)}
\]
\[
C_p = C_v + R \approx .658 + .1889 \approx .847\, \text{kJ/(kg·K)}
\]
### Step 4: Calculate \( \Delta U \)
\[
\Delta U = m C_v (T_2 - T_1) = .264 \times .658 \times (1058 - 280)
\]
\[
= .264 \times .658 \times 778 \approx .264 \times 510.724 \approx 134.9\, \text{kJ}
\]
### Step 5: Calculate \( Q \)
\[
Q = \Delta U + W = 134.9 + (-25.87) \approx 109.03\, \text{kJ}
\]
**Positive \( Q \)** indicates heat **absorbed** by the system.
---
# **Final answers:**
### **Part A: Work done**
\[
\boxed{
W \approx -25.87\, \text{kJ}
}
\]
### **Part B: Heat transfer**
\[
\boxed{
Q \approx 109.03\, \text{kJ}
}
\]
---
# Summary
- The compression process involves approximately **26 kJ** of work **done on** the gas.
- About **109 kJ** of heat is **absorbed** by the system during this process.
If you need further clarification or details, feel free to ask!
VIPSolutions focuses on clear, step‑by‑step explanations so you can learn quickly. Whether you need an AI‑generated walkthrough or a short hint to get unstuck, each solution is organized for fast reading and easy review later.
Search similar questions, compare approaches, and bookmark the best answers for revision. Our goal is simple: quick, reliable study help that feels natural—not noisy.