Answer:
[tex]Q = -105 J[/tex]
Also we know that for cyclic process change in internal energy is always ZERO
Explanation:
First gas is compressed isobarically such that its volume is half of initial volume
So its temperature is also half
So heat given in this process is given as
[tex]Q = nC_p \Delta T[/tex]
for diatomic gas we have
[tex]C_p = \frac{7}{2} R[/tex]
so we will have
[tex]Q = 0.200(\frac{7}{2}R)(160 - 320)[/tex]
[tex]Q = -930.7 J[/tex]
Now in adiabatic process heat is not transferred
so in this process
[tex]Q = 0[/tex]
so we have
[tex]T_1V_1^{1.4-1} = T_2V_2^{1.4-1}[/tex]
[tex](160)(\frac{V}{2})^{0.4} = T_2(V)^{0.4}[/tex]
[tex]T_2 = 121.26 K[/tex]
Now it is again reached to original pressure
so temperature will become initial temperature
so heat given in that part
[tex]Q_3 = nC_v\Delta T[/tex]
here we know that
[tex]C_v = \frac{5}{2}R[/tex]
[tex]Q_3 = (0.200)(\frac{5}{2}R)(320 - 121.26)[/tex]
[tex]Q_3 = 825.76 J[/tex]
So total heat given to the system is
[tex]Q = -930.7 + 0 + 825.76[/tex]
[tex]Q = -105 J[/tex]
Also we know that for cyclic process change in internal energy is always ZERO