サインイン

An Otto engine is a four-stroke engine that uses a mixture of gasoline and air as the working fuel. The fuel is injected into the cylinder, and the piston is moved completely down so that the cylinder is at maximum volume. By moving the piston up, adiabatic compression takes place. The spark plug ignites the gasoline-air mixture, and the burning fuel adds heat to the system at a constant volume. The heated mixture expands adiabatically and gets further cooled by exhausting heat, and this cyclic process continues.

Equation1

The thermal efficiency in this ideal cycle is given in terms of the compression ratio and the ratio of specific heat capacities. This efficiency is always less than 100%. The compression ratio for typical Otto engines ranges from 8–10, and for premium gasoline, up to 13. By increasing the compression ratio, the efficiency can be improved. However, this increases the temperature significantly at the end of the adiabatic compression, which could lead to fuel explosion through pre-ignition. The theoretical efficiency is about 56%, assuming the gasoline-air mixture to be an ideal gas, neglecting friction and heat loss. However, the actual efficiency for a non-ideal gas is around 35%.

A diesel engine is also a four-stroke engine with one significant difference from the Otto engine; the diesel engine works on a self-ignition mechanism and hence does not have a spark plug. In this, the fuel is injected at a constant pressure into the cylinder just before the power stroke, and the high temperature developed ignites the fuel as it is injected. This is a major advantage of a diesel engine, as it prevents pre-ignition. Hence, the compression ratio can go as high as 20, improving the theoretical efficiency for an ideal gas to 65%–70%.

タグ
Otto EngineDiesel EngineFour stroke EngineGasoline air MixtureAdiabatic CompressionThermal EfficiencyCompression RatioSelf ignition MechanismFuel InjectionPre ignitionIdeal Gas EfficiencyNon ideal Gas Efficiency

章から 21:

article

Now Playing

21.4 : Otto and Diesel Cycle

熱力学の第二法則

1.1K 閲覧数

article

21.1 : 可逆的および不可逆的なプロセス

熱力学の第二法則

3.9K 閲覧数

article

21.2 : ヒートエンジン

熱力学の第二法則

2.6K 閲覧数

article

21.3 : 内燃機関

熱力学の第二法則

796 閲覧数

article

21.5 : 冷蔵庫とヒートポンプ

熱力学の第二法則

2.1K 閲覧数

article

21.6 : 熱力学の第二法則のステートメント

熱力学の第二法則

2.4K 閲覧数

article

21.7 : カルノーサイクル

熱力学の第二法則

2.7K 閲覧数

article

21.8 : カルノーサイクルの効率

熱力学の第二法則

2.4K 閲覧数

article

21.9 : カルノーサイクルと熱力学の第二法則

熱力学の第二法則

2.3K 閲覧数

article

21.10 : エントロピー

熱力学の第二法則

2.4K 閲覧数

article

21.11 : 可逆過程におけるエントロピー変化

熱力学の第二法則

2.4K 閲覧数

article

21.12 : エントロピーと熱力学の第二法則

熱力学の第二法則

2.6K 閲覧数

JoVE Logo

個人情報保護方針

利用規約

一般データ保護規則

研究

教育

JoVEについて

Copyright © 2023 MyJoVE Corporation. All rights reserved