Tessellate S.T.E.M.S - Physics - College - Set 2 - Problem 4

A heat conducting piston can freely move inside a closed thermally insulate cylinder with an ideal gas. In equilibrium the piston divides the cylinder into equal parts, the gas temperature being equal T 0 T_0 . The piston is slowly displaced. Then the gas temperature as a function of the ratio η \eta of the volumes of the greater and smaller sections is :

( The adiabatic exponent of the gas is equal to γ \gamma .)

( a ) (a) T = T 0 [ ( η + 1 ) 2 4 η ] γ 1 2 T_0 \bigg[\dfrac {(\eta + 1)^2} {4\eta}\bigg]^\dfrac {\gamma - 1} {2}

( b ) (b) T = T 0 [ ( η 1 ) 2 4 η ] γ 1 2 T_0 \bigg[\dfrac {(\eta - 1)^2} {4\eta}\bigg]^\dfrac {\gamma - 1} {2}

( c ) (c) T = T 0 [ ( η + 1 ) 4 2 η ] γ + 1 2 T_0 \bigg[\dfrac {(\eta + 1)^4} {2\eta}\bigg]^\dfrac {\gamma + 1} {2}

( d ) (d) T = T 0 [ ( η 1 ) 2 4 η ] γ + 1 2 T_0 \bigg[\dfrac {(\eta - 1)^2} {4\eta}\bigg]^\dfrac {\gamma + 1} {2}


This problem is a part of Tessellate S.T.E.M.S.

b d c a

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