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The Otto Cycle

1876
  • Nicolaus Otto
  • Alphonse Beau de Rochas
Cutaway model of a spark-ignition engine illustrating the Otto Cycle processes.

(generated image for illustration only)

The ideal Otto cycle is a thermodynamic model for spark-ignition engines. It consists of four internally reversible processes: isentropic compression (1-2), constant volume (isochoric) heat addition (2-3), isentropic expansion (3-4), and constant volume (isochoric) heat rejection (4-1). This cycle forms the theoretical basis for analyzing the performance of gasoline engines, assuming an ideal gas as the working fluid.

The Otto cycle is visualized on a Pressure-Volume (P-V) diagram, forming a closed loop. The analysis begins at state 1, at the start of the compression stroke, with the piston at bottom dead center (BDC).

Process 1–2: Isentropic Compression. The piston moves from BDC to top dead center (TDC), compressing the air-fuel mixture. In this idealized, adiabatic process, there is no heat transfer to or from the system, so entropy remains constant. Work is done on the gas, increasing its internal energy, which manifests as a rise in both pressure and temperature.

Process 2–3: Constant-Volume Heat Addition. At TDC, the spark plug ignites the mixture. The combustion is assumed to be instantaneous, occurring while the volume does not change (an isochoric process). This adds heat (\(Q_{in}\)) to the working fluid, causing a sharp increase in temperature and pressure to state 3, the point of maximum cycle pressure and temperature.

Process 3–4: Isentropic Expansion (Power Stroke). The high-pressure gas from combustion expands, pushing the piston from TDC back to BDC. This expansion is also idealized as adiabatic and reversible (isentropic). The expanding gas does work on the piston, which is the useful work output of the cycle. As the gas expands, its pressure and temperature decrease.

Process 4–1: Constant-Volume Heat Rejection. At BDC, the exhaust valve is assumed to open, and the pressure instantly drops back to the initial pressure of state 1. This is modeled as an isochoric process where heat (\(Q_{out}\)) is rejected from the working fluid to the surroundings, completing the cycle and returning the fluid to its initial state.

UNESCO Nomenclature: 2212
– Thermodynamics

Type

Abstract System

Disruption

Revolutionary

Usage

Widespread Use

Precursors

  • Carnot cycle theory
  • laws of thermodynamics
  • invention of the piston and cylinder mechanism
  • development of spark ignition systems
  • Alphonse Beau De Rochas’s prior theoretical description (1862)

Applications

  • gasoline internal combustion engines
  • rotary engines (wankel engine)
  • performance analysis of spark-ignition engines
  • automotive engineering education
  • basis for modified cycles like the miller and atkinson cycles

Patents:

  • US Patent 194047

Potential Innovations Ideas

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Related to: Otto cycle, thermodynamics, isentropic, isochoric, internal combustion engine, four-stroke, p-v diagram, spark-ignition, ideal gas, heat engine.

Historical Context

The Otto Cycle

1865
1869
1871
1876
1877
1880
1882-01-01
1865
1868
1870
1873
1877
1880
1882-01-01
1883

(if date is unknown or not relevant, e.g. "fluid mechanics", a rounded estimation of its notable emergence is provided)

Related Invention, Innovation & Technical Principles

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