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Heat Engines: Converting Thermal Energy into Mechanical Energy, Study notes of Physics

This document from phy 101 lecture #22 explores the importance of heat engines in converting thermal energy into mechanical energy. The lecture covers the historical context, the simplest heat engine, and the stirling engine. It also discusses the principles of thermodynamics and the ideal gas law. Students will learn about the role of heat engines in the industrial revolution and the basics of how they work.

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Uploaded on 09/17/2009

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Download Heat Engines: Converting Thermal Energy into Mechanical Energy and more Study notes Physics in PDF only on Docsity! PHY 101 Lecture #22 Heat Engines 1 PHY 101 Lecture #22: Heat Engines Prof. Peter R. Saulson saulson@physics.syr.edu http://physics.syr.edu/courses/PHY101/ Office Hrs: Tues 10 ā€“11:30, Physics 263-4, 3-5994 PHY 101 Lecture #22 Heat Engines 2 Outline 1. Why are heat engines important? 2. Worldā€™s simplest heat engine 3. Stirling engine PHY 101 Lecture #22 Heat Engines 5 Chemical energy resources and the Industrial Revolution Much more energy is available in chemical form than in gravitational form. Coal in 18th, 19th centuries 20th cent. added petroleum and natural gas Only way to release coalā€™s stored chemical energy is by burning. Directly for heating: OK For work: need to be able to convert thermal energy into mechanical energy. Hence, the need for heat engines. PHY 101 Lecture #22 Heat Engines 6 How best to convert thermal energy into mechanical energy? Technological taming of heat began ca. 1700. Thomas Savery 1698 & Thomas Newcomen 1705 both made practical steam engines Better steam engines due to James Watt, starting in 1769, before the understanding of physics of energy. Physics questions: What is the best way to get mechanical energy from thermal energy? Can 100% of thermal energy be converted to work? PHY 101 Lecture #22 Heat Engines 7 Worldā€™s Simplest Engine Gas piston setup can be used to convert thermal energy into mechanical form. 0. Starting position: gas is cool, piston is down. 1. Add mass (from lower shelf) to piston. 2. Warm up the gas. Piston rises. 3. Remove mass onto higher shelf. 4. Cool down the gas. Piston sinks. After this cycle, Ugrav has been added to the outside world. (ā€œWork was done.ā€) This cycle can be repeated indefinitely. PHY 101 Lecture #22 Heat Engines 10 Stirling engine One of the simplest forms to analyze. Mechanization of steps of heating, expansion, cooling, compression. Four steps in cycle: 1. Expansion while held at high temperature TH. 2. Move gas (at constant volume) from hot reservoir to cool reservoir, lowering temperature to TL . 3. Compression while held at TL. 4. Move gas (at constant volume) from cool reservoir to hot reservoir, raising temp to TH. PHY 101 Lecture #22 Heat Engines 11 Parts of a Stirling engine 1. Hot reservoir (e.g. hot plate or cup of tea), 2. Cool reservoir (bins for cool water or ice), 3. Air space, communicating with hot reservoir, cool reservoir, and power piston, 4. ā€œDisplacer pistonā€ shuttles air between hot and cold reservoirs, 5. Power piston to turn crank, 6. Crank, with clever bends to sequence motions of displacer piston and power piston, and 7. Flywheel for rotational inertia (here, propeller.) PHY 101 Lecture #22 Heat Engines 12 What makes Stirling engine go? Engine goes because warm airā€™s pressure pushes power piston. Warm air does work W = Pāˆ†V. But, to make a cycle, you have to compress the air again. Why donā€™t you need to do as much work to compress the gas as you got out of it during expansion? Compress the gas when it is cool. Pressure is lower. Work Pāˆ†V to compress is less. PHY 101 Lecture #22 Heat Engines 15 Pressure vs. Volume at constant Temperature At any given temperature, pressure goes down as volume increases. At any given volume, pressure is higher at higher temperature. PHY 101 Lecture #22 Heat Engines 16 Work from power stroke Expansion while T, p are high. Work W= Pāˆ†V by expanding gas is large. PHY 101 Lecture #22 Heat Engines 17 Work consumed by return stroke Work done to compress gas on return stroke takes energy out of spinning parts. But T is low, so P is low, so work W = Pāˆ†V is smaller than in power stroke.
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