a) The temperature at the beginning can be found from the condition
"\\frac{p_1V_1}{T_1}=\\frac{p_2V_2}{T_2}," where
"V_1=V_2:"
"\\frac{p_1}{T_1}=\\frac{p_2}{T_2},\\\\\n\\space\\\\\nT_2=T_1\\frac{p_2}{p_1}=2763\\text{ K}." Hot!
b) The adiabatic law (and keep in mind that for isochoric process "V_1=V_2"):
"p_2V_1^\\gamma=p_3V_3^\\gamma=\\text{ const}=c,\\\\\n\\space\\\\\nV_3=V_1\\bigg(\\frac{p_2}{p_3}\\bigg)^{1\/\\gamma}=0.14\\bigg(\\frac{41.4}{2.76}\\bigg)^{(1\/1.41)}=0.95\\text{ m}^3."c) The word adiabatic means that no energy of heat is lost or supplied.
d) The work done in the adiabatic process while gas transferred from state 2 (0.14 cubic m, 41.4 bar) to state 3 (2.76 bar, 0.95 cubic m):
"W=\\int^3_2pdV=\\int^3_2\\frac{c}{V^{1.41}}dV=-\\frac{c}{0.41V^{0.41}}\\bigg|^3_2=\\\\\n\\space\\\\\n=-\\frac{c}{0.41V_3^{0.41}}+\\frac{c}{0.41V_2^{0.41}}=\n\\space\\\\\n\\space\\\\\n=-\\frac{p_3V_3^{1.41}}{0.41V_3^{0.41}}+\\frac{p_2V_2^{1.41}}{0.41V_2^{0.41}}=\\frac{p_2V_2-p_3V_3}{0.41}=774146\\text{ J}."
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