LECTURE PHYSICAL CHEMISTRY 3rd EDITION ROBERT G. MORTIMER

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www.daykemquynhon.ucoz.com The value of the ratio q 3 /q 1 in a Carnot cycle therefore depends only on the temperatures of the reservoirs and not on their composition. The thermodynamic temperature, θ, is defined by where θ c is the thermodynamic temperature of the cold reservoir and θ h is the thermodynamic temperature of the hot reservoir. We require the thermodynamic temperature to be positive. The Carnot efficiency is now given by https://plus.google.com/+DạyKèmQuyNhơn Collected by Nguyen Thanh Tu Teacher MailBox : nguyenthanhtuteacher@hotmail.com
www.daykemquynhon.ucoz.com We now show that the thermodynamic temperature scale can coincide with the ideal gas temperature scale. Assume that the working fluid of a Carnot engine is an ideal gas with a constant heat capacity. For the first step of the Carnot cycle, from Eq.(2.4-10) For the third step, We can now locate the states at which steps 1 and 3 terminate by using Eq. (2.4-21) twice: https://plus.google.com/+DạyKèmQuyNhơn Collected by Nguyen Thanh Tu Teacher MailBox : nguyenthanhtuteacher@hotmail.com
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Part 1 Thermodynamics and the Macro
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LECTURE PHYSICAL CHEMISTRY 3rd EDITION ROBERT G. MORTIMER

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