Find the overall chanhe in internal energy between the initial and final states per unit mass of waterProblem 03.047 -
Piston—cylinder
device fitted with
stops
Water initially at 200
kPa and 300°C is
contained in a piston—
cylinder device fitted
with stops. The water is
allowed to cool at
constant pressure until
it exists as a saturated
vapor and the piston
rests on the stops.
Then the water
continues to cool until
the pressure is 100 kPa.
Es
| Wat
| 300°C
Question:
Find the overall chanhe in internal energy between the initial and final states per unit mass of waterProblem 03.047 -
Piston—cylinder
device fitted with
stops
Water initially at 200
kPa and 300°C is
contained in a piston—
cylinder device fitted
with stops. The water is
allowed to cool at
constant pressure until
it exists as a saturated
vapor and the piston
rests on the stops.
Then the water
continues to cool until
the pressure is 100 kPa.
Es
| Wat
| 300°C
This is AI generated Response.
Asked by: manish kumar
Created at: 2026-02-20 07:43:54
Final Answer:
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Let's break down the problem step by step.
## **Given Data**
- **Initial State:**
- Pressure, \( P_1 = 200 \) kPa
- Temperature, \( T_1 = 300^\circ \)C
- **Intermediate State:**
- Water cools at constant pressure (200 kPa) until it becomes a saturated vapor (\( x=1 \)), and the piston hits the stops.
- **Final State:**
- Water continues to cool at constant volume until the pressure drops to \( P_3 = 100 \) kPa.
## **Step 1: Find Initial State Properties (\( u_1 \))**
At \( P_1 = 200 \) kPa and \( T_1 = 300^\circ \)C:
- From steam tables:
- At 200 kPa, the saturation temperature \( T_{sat} \approx 120.23^\circ \)C.
- Since \( T_1 = 300^\circ \)C \( > T_{sat} \), the water is superheated.
- Superheated steam tables at \( P = 200 \) kPa, \( T = 300^\circ \)C:
- **Internal energy \( u_1 \) ≈ 2725.5 kJ/kg**
---
## **Step 2: Intermediate State (\( u_2 \)), Saturated Vapor at 200 kPa**
- At 200 kPa, saturated vapor (\( x=1 \)):
- From steam tables:
- \( u_g \) (internal energy of vapor at 200 kPa) \( = 2506.5 \) kJ/kg
So, \( u_2 = 2506.5 \) kJ/kg
---
## **Step 3: Final State (\( u_3 \)), Pressure Drops to 100 kPa at Constant Volume**
- From Step 2, the specific volume at the end of step 1 (when the piston hits the stops) is:
- \( v_2 = v_g \) at 200 kPa \( = .88578 \) m³/kg
- At 100 kPa (final state), the specific volume remains \( v_3 = v_2 = .88578 \) m³/kg.
At 100 kPa:
- \( v_f = .001043 \) m³/kg
- \( v_g = 1.694 \) m³/kg
Since \( v_f < v_3 < v_g \), the final state is a mixture.
### **Quality at final state:**
\[
x_3 = \frac{v_3 - v_f}{v_g - v_f} = \frac{.88578 - .001043}{1.694 - .001043}
= \frac{.884737}{1.692957}
\approx .523
\]
### **Internal energy at final state:**
\[
u_3 = u_f + x_3 (u_g - u_f)
\]
From steam tables at 100 kPa:
- \( u_f = 419.04 \) kJ/kg
- \( u_g = 2506.5 \) kJ/kg
\[
u_3 = 419.04 + .523 \times (2506.5 - 419.04)
\]
\[
u_3 = 419.04 + .523 \times 2087.46
\]
\[
u_3 = 419.04 + 1091.77
\]
\[
u_3 \approx 151.81 \text{ kJ/kg}
\]
---
## **Step 4: Overall Change in Internal Energy**
\[
\Delta u = u_3 - u_1 = 151.81 - 2725.5 = -1214.7 \text{ kJ/kg}
\]
---
## **Summary Table**
| State | P (kPa) | T (°C) | Quality | v (m³/kg) | u (kJ/kg) |
|-------|---------|--------|---------|-----------|-------------|
| 1 | 200 | 300 | - | - | 2725.5 |
| 2 | 200 | 120.23 | 1. | .88578 | 2506.5 |
| 3 | 100 | ? | .523 | .88578 | 151.81 |
---
## **Final Answer**
\[
\boxed{
\text{The overall change in internal energy per unit mass is} \ \Delta u = -1214.7 \text{ kJ/kg}
}
\]
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