dc.contributor | Universidade Estadual Paulista (UNESP) | |
dc.creator | Blinder, S M | |
dc.date | 2011-05-26T19:57:24Z | |
dc.date | 2011-05-26T19:57:24Z | |
dc.date | 2011-05-26 | |
dc.date.accessioned | 2017-04-05T17:08:06Z | |
dc.date.available | 2017-04-05T17:08:06Z | |
dc.identifier | http://acervodigital.unesp.br/handle/123456789/5359 | |
dc.identifier | http://objetoseducacionais2.mec.gov.br/handle/mec/8186 | |
dc.identifier.uri | http://repositorioslatinoamericanos.uchile.cl/handle/2250/832770 | |
dc.description | Knowledge in classical thermodynamics | |
dc.description | The Carnot cycle is an idealization for a heat engine operating reversibly between two reservoirs at temperatures T1 and T2 . The working substance is assumed to be one mole of an ideal gas with heat-capacity ratio γ=Cp/Cv . (For a monatomic ideal gas, γ has its maximum value at 5/3=~1.667.) The four steps of the cycle are most commonly plotted on a pressure-volume diagram, shown on the left, with alternate isotherms (red curves ofconstant temperature) and adiabatics or isentropics (blue curves of constant entropy). A simple alternative representation is therefore a rectangle on a temperature-entropy diagram, shown as an inset | |
dc.description | Componente Curricular::Educação Superior::Ciências Exatas e da Terra::Física | |
dc.relation | CarnotCycleOnIdealGas.nbp | |
dc.rights | Demonstration freeware using Mathematica Player | |
dc.subject | Ideal gas | |
dc.subject | Carnot cycle | |
dc.subject | Educação Superior::Ciências Exatas e da Terra::Física::Transferência de Calor; Processos Térmicos e Termodinâmicos | |
dc.title | Carnot cycle on ideal gas | |
dc.type | Software | |