---
title: "Water in piston cylinder with stops, 200 kPa"
subject: "Fundamental of Thermodynamics & Heat Transfer"
chapter: 3
key: "semester_2/fundamental_of_thermodynamics_and_heat_transfer:water-piston-stops-200kpa-50c"
source: https://www.bctengineer.com/q/semester_2/fundamental_of_thermodynamics_and_heat_transfer/water-piston-stops-200kpa-50c
site: BCT Engineering
---

# Water in piston cylinder with stops, 200 kPa

Fundamental of Thermodynamics & Heat Transfer · Chapter 3: Properties of Common Substances

- Asked in: 2075 Baisakh, 8 marks
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_2/fundamental_of_thermodynamics_and_heat_transfer/water-piston-stops-200kpa-50c
- Whole chapter: https://www.bctengineer.com/md/semester_2/fundamental_of_thermodynamics_and_heat_transfer/chapter-3

## Question

A piston cylinder arrangement shown in figure below contains 2 kg of water initially at a pressure of 200 kPa and a temperature of 50°C. Heat is added until the piston reaches the upper stops where the total volume is 1.5 m³. It takes a pressure of 600 kPa to lift the piston. Sketch the process on P-v and T-v diagrams and determine the final temperature and the total work transfer.
[Figure: cylinder with H2O, piston resting at the bottom of the stops region, heat Q added from below.]

## Short answer

Heating water initially at 200 kPa, 50°C: constant-volume until 600 kPa, then constant pressure at 600 kPa to 1.5 m³. Using steam tables, final superheated temperature ≈ 704 °C, total work = 898.8 kJ.

## Answer

**Given:** m = 2 kg; State 1: 200 kPa, 50 °C; the piston needs 600 kPa to lift; heat is added until the piston reaches the upper stops, V₂ = 1.5 m³.

**State 1:** T_sat at 200 kPa = 120.2 °C, so water at 50 °C is compressed liquid. Use v₁ ≈ v_f(50 °C) = 0.001012 m³/kg (steam tables), so V₁ = 2 × 0.001012 = 0.00202 m³.

**Process:**
- 1 → a: the piston rests on the bottom stops (200 kPa < 600 kPa), so heating is at constant volume until P rises to 600 kPa.
- a → 2: the piston lifts and the pressure stays at 600 kPa (constant P) until it reaches the upper stops with V₂ = 1.5 m³.

```text
 P (kPa)
 600 |  a -------------------------- 2
     |  |
     |  |  1-a: const v (piston on stops)
 200 |  1
     +---------------------------------- v
      v1 = 0.00101                v2 = 0.75

 T (C)
 703.6|                               2
      |                             /
 158.8|      f ----------------- g /    a-f-g-2: 600 kPa isobar
      |     /
   50 |  1,a
      +---------------------------------- v
```
On the T-v diagram, 1 and a almost coincide, because heating a compressed liquid at constant volume raises its pressure sharply with almost no rise in temperature. Along the 600 kPa isobar the liquid warms to 158.8 °C (f), evaporates at constant temperature (f to g), and is then superheated to state 2.

**State 2:** v₂ = V₂/m = 1.5/2 = 0.75 m³/kg at P = 600 kPa. At 600 kPa, v_g = 0.3157 m³/kg < 0.75, so the steam is superheated. From the superheated table at 600 kPa:
- 700 °C: v = 0.7472 m³/kg
- 800 °C: v = 0.8246 m³/kg

T₂ = 700 + 100 × (0.75 − 0.7472)/(0.8246 − 0.7472) = **≈ 703.6 °C**

**Work:** work occurs only in a → 2 (constant P); the constant-volume heating 1 → a gives no work.
W = P (V₂ − V₁) = 600 × (1.5 − 0.00202) = **898.8 kJ**

**Answer: Final temperature ≈ 704 °C; total work transfer ≈ 899 kJ.**

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. Why is water at 200 kPa, 50 C taken as compressed liquid with v about vf(50 C)?
   A. 50 C is below Tsat = 120.2 C at 200 kPa
   B. 50 C is above Tsat at 200 kPa
   C. Its quality is 0.5
   D. The piston is resting on the stops
   Answer: A. Since T is below Tsat for its pressure, it is compressed liquid and v is approximated by vf at 50 C. (Key point: State 1 phase)

2. What happens in 1 to a while the piston sits on the bottom stops?
   A. Constant-pressure heating at 200 kPa
   B. Constant-volume heating until P reaches 600 kPa
   C. Isothermal expansion
   D. Adiabatic compression
   Answer: B. The piston needs 600 kPa to lift, so until then the volume is fixed and pressure rises. (Key point: First heating stage)

3. Why is state 2 (600 kPa, v = 0.75 m3/kg) superheated?
   A. v = 0.75 is less than vf
   B. Pressure is above the critical pressure
   C. v = 0.75 exceeds vg = 0.3157 at 600 kPa
   D. Quality there is 0.75
   Answer: C. When v is greater than vg at that pressure the steam is superheated; interpolation gives about 704 C. (Key point: State 2 phase)

4. Where is work done and what is its value?
   A. Over the whole process using 200 kPa: about 300 kJ
   B. Only in 1 to a: about 899 kJ
   C. Zero, because the piston stops fix the volume
   D. Only in a to 2 at 600 kPa: about 899 kJ
   Answer: D. The constant-volume stage gives no work; W = 600 x (1.5 - 0.00202) = 898.8 kJ. (Key point: Work)

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