Otto cycle

[′äd·ō ‚sī·kəl] (thermodynamics) A thermodynamic cycle for the conversion of heat into work, consisting of two isentropic phases interspersed between two constant-volume phases. Also known as spark-ignition combustion cycle.

Otto cycle

The basic thermodynamic cycle for the prevalent automotive type of internal combustion engine. The engine uses a volatile liquid fuel (gasoline) or a gaseous fuel to carry out the theoretic cycle shown in the illustration. The cycle consists of two isentropic (reversible adiabatic) phases interspersed between two constant-volume phases. The theoretic cycle should not be confused with the actual engine built for such service as automobiles, motor boats, aircraft, lawn mowers, and other small self-contained power plants.

The thermodynamic working fluid in the cycle is subjected to isentropic compression, phase 1–2; constant-volume heat addition, phase 2–3; isentropic expansion, phase 3–4; and constant-volume heat rejection (cooling), phase 4–1.

The Otto cycle is represented in many millions of engines utilizing either the four-stroke principle or the two-stroke principle. Evidence indicates that actual Otto engines offer peak efficiencies (25±%) at compression ratios of 15±. Above this ratio, efficiency falls. The most probable explanation is that the extreme pressures associated with high compression cause increasing amounts of dissociation of the combustion products. This dissociation, near the beginning of the expansion stroke, exerts a more deleterious effect on efficiency than the corresponding gain from increasing compression ratio. See Brayton cycle, Carnot cycle, Internal combustion engine, Thermodynamic cycle

Otto cycle

Piston descends, inlet valve opens. Air drawn in at constant pressure (Line 1–2). Otto cycle

Piston ascends, both valves closed. Pressure increases and volume decreases to point 3, combustion at constant volume results in sharp pressure rise to point 4. Otto cycle

Increased pressure at constant volume forces piston down, resulting in increases in volume and drop in pressure (Line 4–5). Otto cycle

Exhaust valve opens, releasing combustion charge with rapid drop in pressure at constant volume (Line 5–2). Piston rises and forces remaining gases out of exhaust at constant pressure (Line 2–1). Cycle begins again at point 1.A thermodynamic cycle for the conversion of heat into work, consisting of two isentropic phases interspersed between two constant-volume phases. It is the four-stroke cycle of operation that produces the power within the cylinders of an internal combustion engine. The cycle is named after Dr Nicolas Otto, who introduced it in 1876.

单词	otto cycle
释义	Otto cycle Otto cycle n (General Engineering) an engine cycle used on four-stroke petrol engines (Otto engines) in which, ideally, combustion and rejection of heat both take place at constant volume. Compare diesel cycle [C19: named after Nikolaus August Otto (1832–91), German engineer] Otto cycle Otto cycle [′äd·ō ‚sī·kəl] (thermodynamics) A thermodynamic cycle for the conversion of heat into work, consisting of two isentropic phases interspersed between two constant-volume phases. Also known as spark-ignition combustion cycle. Otto cycle The basic thermodynamic cycle for the prevalent automotive type of internal combustion engine. The engine uses a volatile liquid fuel (gasoline) or a gaseous fuel to carry out the theoretic cycle shown in the illustration. The cycle consists of two isentropic (reversible adiabatic) phases interspersed between two constant-volume phases. The theoretic cycle should not be confused with the actual engine built for such service as automobiles, motor boats, aircraft, lawn mowers, and other small self-contained power plants. The thermodynamic working fluid in the cycle is subjected to isentropic compression, phase 1–2; constant-volume heat addition, phase 2–3; isentropic expansion, phase 3–4; and constant-volume heat rejection (cooling), phase 4–1. The Otto cycle is represented in many millions of engines utilizing either the four-stroke principle or the two-stroke principle. Evidence indicates that actual Otto engines offer peak efficiencies (25±%) at compression ratios of 15±. Above this ratio, efficiency falls. The most probable explanation is that the extreme pressures associated with high compression cause increasing amounts of dissociation of the combustion products. This dissociation, near the beginning of the expansion stroke, exerts a more deleterious effect on efficiency than the corresponding gain from increasing compression ratio. See Brayton cycle, Carnot cycle, Internal combustion engine, Thermodynamic cycle Otto cycle Piston descends, inlet valve opens. Air drawn in at constant pressure (Line 1–2).Piston ascends, both valves closed. Pressure increases and volume decreases to point 3, combustion at constant volume results in sharp pressure rise to point 4.Increased pressure at constant volume forces piston down, resulting in increases in volume and drop in pressure (Line 4–5).Exhaust valve opens, releasing combustion charge with rapid drop in pressure at constant volume (Line 5–2). Piston rises and forces remaining gases out of exhaust at constant pressure (Line 2–1). Cycle begins again at point 1.A thermodynamic cycle for the conversion of heat into work, consisting of two isentropic phases interspersed between two constant-volume phases. It is the four-stroke cycle of operation that produces the power within the cylinders of an internal combustion engine. The cycle is named after Dr Nicolas Otto, who introduced it in 1876.
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