---
title: "Actual VCR cycle with compressor efficiency"
subject: "Applied Thermodynamics"
chapter: 3
key: "semester_3/applied_thermodynamics:vcr-actual-compressor-efficiency-numerical"
source: https://www.bctengineer.com/q/semester_3/applied_thermodynamics/vcr-actual-compressor-efficiency-numerical
site: BCT Engineering
---

# Actual VCR cycle with compressor efficiency

Applied Thermodynamics · Chapter 3: Refrigeration

- Asked in: year not given, 8 marks
- Video: [Ideal and Actual Vapor-compression Refrigeration Cycles](https://www.youtube.com/watch?v=6F100qUXHlw) — Dr Kidd Engineering
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_3/applied_thermodynamics/vcr-actual-compressor-efficiency-numerical
- Whole chapter: https://www.bctengineer.com/md/semester_3/applied_thermodynamics/chapter-3

## Question

A refrigeration plant of 10 kW capacity uses R-134a between 0.14 MPa and 0.8 MPa. Vapour leaves the evaporator as dry saturated ($h = 239.16$ kJ/kg) and gains heat in the suction line so that it enters the compressor with $h_1 = 242.2$ kJ/kg. The isentropic compression ends at $h_{2s} = 278.6$ kJ/kg. The isentropic efficiency of the compressor is 75% and the motor-drive efficiency is 90%. Saturated liquid at 0.8 MPa has $h_3 = 95.47$ kJ/kg. Find (a) the actual compressor work per kg, (b) the mass flow rate, (c) the electrical power input, (d) the actual COP, and (e) the heat rejected in the condenser.

## Short answer

Actual compressor work per kg = 48.5 kJ/kg; mass flow rate = 0.0696 kg/s; shaft power input = 3.38 kW, electrical input = 3.75 kW; actual COP = 2.96 (shaft) / 2.66 (electrical); heat rejected = 13.6 kW.

## Answer

#### Refrigerating effect
Only the heat absorbed in the evaporator is useful cooling. The suction-line heat gain comes from outside the cold space, so:

$$
q_L = h_{evap\ exit} - h_4 = 239.16 - 95.47 = 143.69\ \text{kJ/kg}
$$

#### (a) Compressor work per kg
$$
\begin{aligned}
w_s &= h_{2s} - h_1 = 278.6 - 242.2 = 36.4\ \text{kJ/kg}\\
w_a &= \frac{w_s}{\eta_s} = \frac{36.4}{0.75} = 48.53\ \text{kJ/kg}
\end{aligned}
$$

Actual discharge enthalpy: $h_2 = 242.2 + 48.53 = 290.7$ kJ/kg.

#### (b) Mass flow rate
$$
\dot m = \frac{10}{143.69} = 0.0696\ \text{kg/s}
$$

#### (c) Power
$$
\begin{aligned}
P_{comp} &= \dot m\,w_a = 0.0696 \times 48.53 = 3.38\ \text{kW}\\
P_{elec} &= \frac{P_{comp}}{\eta_{motor}} = \frac{3.38}{0.9} = 3.75\ \text{kW}
\end{aligned}
$$

#### (d) Actual COP
Based on shaft power: $\text{COP} = 10/3.38 = 2.96$.
Based on electrical input: $\text{COP} = 10/3.75 = 2.66$.

(For comparison, the ideal COP with no losses is $143.69/36.23 = 3.97$.)

#### (e) Condenser heat rejection
$$
Q_H = \dot m (h_2 - h_3) = 0.0696 \times (290.7 - 95.47) = 13.59\ \text{kW}
$$

(Energy check: $10 + 0.21$ (suction-line gain) $+ 3.38 = 13.59$ kW.)

**Answer:** (a) 48.5 kJ/kg; (b) 0.0696 kg/s; (c) 3.38 kW at the shaft, 3.75 kW electrical; (d) 2.96 (shaft) or 2.66 (electrical); (e) 13.6 kW.

## Check yourself

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

1. In this plant, which enthalpy difference gives the refrigerating effect q_L?
   A. h1 - h4 (compressor inlet minus evaporator inlet)
   B. h(evaporator exit, dry saturated) - h4 = 239.16 - 95.47
   C. h2 - h3
   D. h2s - h1
   Answer: B. Cooling happens in the evaporator, so only heat gained up to the evaporator exit counts. Suction-line heat gain is from outside the cold space and is not useful cooling. (Key point: Refrigerating effect)

2. How is the actual compressor work per kg obtained from the isentropic work?
   A. w_a = w_s x eta_s = 36.4 x 0.75
   B. w_a = w_s / eta_s = 36.4/0.75 = 48.53 kJ/kg
   C. w_a = w_s / eta_motor
   D. w_a = h2s - h4
   Answer: B. Isentropic efficiency is ideal work divided by actual work, so actual work is larger: 36.4/0.75 = 48.53 kJ/kg. (Key point: Actual compressor work)

3. After finding m = 10/143.69 = 0.0696 kg/s and shaft power 3.38 kW, how is the electrical input found?
   A. 3.38 x 0.9 = 3.04 kW
   B. 3.38 / 0.9 = 3.75 kW
   C. 3.38 / 0.75 = 4.51 kW
   D. 10 / 2.96 = 3.38 kW
   Answer: B. The motor delivers shaft power with efficiency 0.9, so electrical input = shaft power / eta_motor = 3.75 kW. (Key point: Mass flow and electrical power)

4. Which statement about the results is correct?
   A. COP based on electrical input (2.66) is higher than on shaft power (2.96)
   B. Condenser heat Q_H = m(h2 - h3) uses the actual discharge enthalpy h2 = 290.7 kJ/kg, giving about 13.6 kW
   C. Condenser heat uses h2s = 278.6 because the isentropic state is the real exit
   D. The ideal COP of 3.97 is lower than the actual COP
   Answer: B. The real compressor discharges at h2 = h1 + w_a = 290.7 kJ/kg, so Q_H = 0.0696 x 195.23 = 13.6 kW. Actual COPs are below the ideal 3.97. (Key point: Actual COP and condenser heat)

## Related in Applied Thermodynamics

- [Ideal vapour compression cycle for 5 TR](https://www.bctengineer.com/question.md?key=semester_3%2Fapplied_thermodynamics%3Avcr-ideal-cycle-numerical) — Applied Thermodynamics, chapter 3
- [VCR cycle with subcooling and superheating](https://www.bctengineer.com/question.md?key=semester_3%2Fapplied_thermodynamics%3Avcr-subcooling-superheating-numerical) — Applied Thermodynamics, chapter 3
- [Ideal versus actual vapour compression cycle](https://www.bctengineer.com/question.md?key=semester_3%2Fapplied_thermodynamics%3Aideal-vs-actual-vcr-cycle) — Applied Thermodynamics, chapter 3
- [Simple vapour compression cycle](https://www.bctengineer.com/question.md?key=semester_3%2Fapplied_thermodynamics%3Asimple-vcr-cycle-ts-ph-diagrams) — Applied Thermodynamics, chapter 3

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