Question #88249
34. A horizontal cylindrical tube is divided into four parts with the help of
two fixed partitions A and B and a movable piston C. The tube and the
piston C are made from heat insulating materials whereas the fixed
partitions A and B are made from a conducting material. Volume
itial volume between
the fixed partition B and piston C is V2. These volumes are filled with
an ideal mono-atomic gas at pressure po and temperature To. Outside
the piston C, pressure is also po. Quantity AQ of heat is slowly
transferred through the partition A to the gas trapped between the
partitions A and B. Find temperatures of the gases on both sides of thebetween the fixed partitions A and B is Vi arpartition B and heat transferred through it.
1
Expert's answer
2019-04-19T10:30:52-0400

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Using first law of thermodynamics for volume between AB


QA=ΔU1+QBQ_A=\Delta U_1+Q_B

Using first law of thermodynamics for volume between BC

QB=ΔU2+A2Q_B=\Delta U_2+A_2

The increment of internal energy for ideal gas between AB

ΔU1=32ν1RΔT\Delta U_1=\frac{3}{2} \nu_1 R \Delta T

The increment of internal energy for ideal gas between BC

ΔU2=32ν2RΔT\Delta U_2=\frac{3}{2} \nu_2 R \Delta T

Ideal gas between BC produce work

A2=p0ΔVA_2=p_0 \Delta V

but, from Mendeleev-Clapeyron equation

p0ΔV=ν2RΔTp_0 \Delta V=\nu_2 R \Delta Tp0V1=ν1RΔTp_0 V_1=\nu_1 R \Delta Tp0V2=ν2RΔTp_0 V_2=\nu_2 R \Delta T

So, we have equation

QA=32ν1RΔT+32ν2RΔT+ν2RΔTQ_A=\frac{3}{2} \nu_1 R \Delta T+\frac{3}{2} \nu_2 R \Delta T +\nu_2 R \Delta TΔT=TT0\Delta T= T-T_0T=[QAp0(32V1+52V2)+1]T0T=[\frac{Q_A}{p_0(\frac{3}{2}V_1+\frac{5}{2}V_2)}+1]T_0

For heat trough partition B

QB=ΔU2+A2=52p0V2RT0RΔTQ_B=\Delta U_2+A_2=\frac{5}{2} \frac{p_0 V_2}{RT_0} R \Delta TQB=V235V1+V2QAQ_B=\frac{V_2}{\frac{3}{5}V_1+V_2} Q_A

Answer

Temperature gases is equal and most be

T=[QAp0(32V1+52V2)+1]T0T=[\frac{Q_A}{p_0(\frac{3}{2}V_1+\frac{5}{2}V_2)}+1]T_0

Heat trough partition B

QB=V235V1+V2QAQ_B=\frac{V_2}{\frac{3}{5}V_1+V_2} Q_A


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