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 About RF Cafe Copyright: 1996 - 2024Webmaster:    Kirt Blattenberger,     BSEE - KB3UON RF Cafe began life in 1996 as "RF Tools" in an AOL screen name web space totaling 2 MB. Its primary purpose was to provide me with ready access to commonly needed formulas and reference material while performing my work as an RF system and circuit design engineer. The World Wide Web (Internet) was largely an unknown entity at the time and bandwidth was a scarce commodity. Dial-up modems blazed along at 14.4 kbps while typing up your telephone line, and a nice lady's voice announced "You've Got Mail" when a new message arrived... All trademarks, copyrights, patents, and other rights of ownership to images and text used on the RF Cafe website are hereby acknowledged. My Hobby Website: AirplanesAndRockets.com

The Carnot Cycle

An ideal cycle would be performed by a perfectly efficient heat engine—that is, all the heat would be converted to mechanical work. A 19th-century French scientist named Nicolas Carnot conceived a thermodynamic cycle that is the basic cycle of all heat engines. He showed that such an ideal engine cannot exist. Any heat engine must expend some fraction of its heat input as exhaust. The second law of thermodynamics places an upper limit on the efficiency of engines; that upper limit is less than 100 percent. The limiting case is now known as a Carnot cycle.

The Carnot Cycle

 (1) Isothermal expansion of gas in cylinder as heat is added from source. Piston moves from V1 to V2, doing work on the system.
 (2) Heat source is removed and isolated. Adiabatic expansion continues until volume V3 is reached, performing additional work, at temperature T2.
 (4) Heat source is removed and isolated. Adiabatic compression continues until volume V4 is reached, performing additional work, at temperature T2.
 (3) Isothermal compression of gas in cylinder as work is done by the system on the piston. Heat is be transferred to T2.
Isothermal: Process in which no temperature change occurs in a closed system. Adiabatic: Process in which no heat is transferred into or out of a closed system.

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