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Heat Engines (HL) (HL IB Physics)

Revision Note

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Katie M

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Katie M

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Physics

Heat Engines

  • A heat engine is a device that converts thermal energy into mechanical work
  • Heat engines operate through a series of thermodynamic processes which form a closed cycle
    • A closed cycle is one in which the system returns to its initial state
  • A simple heat engine consists of a gas in a cylinder with a piston

2-4-7-heat-engine-piston-diagram

A simple heat engine converts thermal energy into mechanical work

  • The steps in the operation of a cyclic heat engine process are:

1. Extract heat from a hot reservoir

    • A hot reservoir (a source of thermal energy) at a high temperature T subscript H transfers heat Q subscript H into the engine

2. Use some of the extracted heat to perform work

    • The gas does mechanical work as it expands which pushes the piston out

3. Release excess heat into a cold reservoir

    • The gas is allowed to cool at constant volume, meanwhile, heat Q subscript C is released to the surroundings
    • Some of the energy transferred into the engine is released into a cold reservoir (a sink for excess heat) at a lower temperature T subscript C

4. Repeat cycle

    • Once the heat has been extracted, the piston is pushed down to compress the gas back to its original state
    • The process can then be repeated as many times as needed, continuously converting heat into mechanical work 

2-4-7-thermodynamic-heat-engine-diagram

  • For a cyclic heat engine process, the p-V diagram will form a closed loop
  • The area inside the loop is equal to the net work done during one cycle

2-4-7-heat-engine-pv-diagram

  • The net work done by the engine is:

increment W subscript o u t end subscript space equals space Q subscript H space minus space Q subscript C

  • Where:
    • increment W subscript o u t end subscript = useful work output of the heat engine (J)
    • Q subscript H = heat transferred from hot reservoir to engine (J)
    • Q subscript C = heat transferred from engine to cold reservoir (J)

Efficiency of Heat Engines

  • The goal of a heat engine is to transfer thermal energy into useful mechanical work as efficiently as possible
  • The thermodynamic efficiency of a heat engine can be calculated using

efficiency = fraction numerator u s e f u l space w o r k space o u t p u t over denominator t o t a l space e n e r g y space i n p u t end fraction

eta space equals space W subscript o u t end subscript over Q subscript H space equals space fraction numerator open parentheses Q subscript H space minus space Q subscript C close parentheses over denominator Q subscript H end fraction

eta space equals space 1 space minus space Q subscript C over Q subscript H

  • Where:
    • eta = efficiency of a heat engine
    • W subscript o u t end subscript = useful work output (J)
    • Q subscript H = total energy input from the hot reservoir (J)
    • Q subscript C = energy lost to the cold reservoir (J)

Worked example

The pressure-volume (pV) diagram shows part of a cycle ABCA of a heat engine.

The cycle consists of a change AB, followed by an adiabatic compression BC and then the gas cools at a constant volume to its original state.

2-4-7-heat-engine-efficiency-pv-diagram-worked-example

At C the pressure of the gas is 2.5 × 105 Pa. The total thermal energy transferred to the gas during the cycle is 1250 J.

(a)
Sketch, on the pV diagram, the complete cycle ABCA. 
(b)
State the names of processes AB and CA.
(c)
Estimate the net useful work done by the gas during the cycle.
(d)
Determine the efficiency of the heat engine.
 

Answer:

(a)

  • From B to C: adiabatic compression, so
    • The pressure increases to 2.5 × 105 Pa
    • The volume decreases to 2 × 10−3 m3 (same as A)
  • From C to A: the gas cools at a constant volume
    • The pressure decreases to 0.5 × 105 Pa
    • The volume stays at 2 × 10−3 m3 (same as A)

2-4-7-heat-engine-efficiency-pv-diagram-worked-example-ma

(b)

  • Process AB = isobaric expansion (constant pressure, volume increasing)
  • Process CA = isovolumetric temperature drop (constant volume, pressure/temperature decreasing)

(c)

  • The net useful work done by the gas during the cycle is given by the area enclosed by the loop

2-4-7-heat-engine-efficiency-pv-diagram-worked-example-ma1

  • Work done by the gas ≈ 5.25 × (0.5 × 105) × (2 × 10−3) = 525 J

(d)

  • The efficiency of a heat engine is given by

eta space equals space W subscript o u t end subscript over Q subscript H

  • Where
    • Useful work output, W subscript o u t end subscript = 525 J
    • Total energy input, Q subscript H = 1250 J

eta space equals space 525 over 1250 space equals space 0.42

  • Therefore, the heat engine has an efficiency of about 42%

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Katie M

Author: Katie M

Katie has always been passionate about the sciences, and completed a degree in Astrophysics at Sheffield University. She decided that she wanted to inspire other young people, so moved to Bristol to complete a PGCE in Secondary Science. She particularly loves creating fun and absorbing materials to help students achieve their exam potential.