For adiabatic ideal gas near room temperature, what fraction of heat supplied is available for external work. If the gas is expanded at a constant pressure? At a constant temperature?
In the process of expansion at constant pressure p, assuming that the volume increases from "V_1" to "V_2" and temperature change from "T_1" to "T_2" , we have
"PV_1=nRT_1"
"PV_2=nRT_2"
In this process, the work done by the system on the outside world is "W = p(V_2-V_1)= nR\u0394T" and increase in internal energy of the system is
"\u0394U = C_v\u0394T"
"\\frac{W}{Q}=\\frac{W}{\\Delta U + W}=\\frac{nR}{C_v +nR}=\\frac{2}{7}"
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