For the adiabatic process, we have
"T_1V_1^{\\gamma-1}=T_2V_2^{\\gamma-1},\\\\\\space\\\\\nT_2=T_1\\bigg(\\frac{V_1}{V_2}\\bigg)^{{\\gamma-1}},\\\\\\space\\\\\nT_2=(27+273)\\bigg(\\frac{400}{500}\\bigg)^{\\gamma-1}=274\\text{ K, or 1\u00b0C.}"Now, calculate the initial pressure:
"P_1V_1^\\gamma=P_2V_2^\\gamma,\\\\\nP_1^{\\gamma-1}T_1^\\gamma=P_2^{\\gamma-1}T_2^\\gamma,\\\\\\space\\\\\nP_1=\\\\\nP_2=" According to the ideal gas law, for the isothermal compression we have
"P_2V_2=P_1V_3." Also, according to the same law, for the second and initial states of gas we have
"\\frac{P_2V_2}{T_2}=\\frac{P_1V_1}{T_1}."Combine the last two equations to determine "V_3":
"V_3=V_1\\frac{T_2}{T_1}=400\\cdot\\frac{274}{300}=364\\text{ cm}^3."
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