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Question: In a cyclic process ABCA for an ideal gas . In AB , BC and CA processes \(50J\) , \(20J\) and \(5J\)...

In a cyclic process ABCA for an ideal gas . In AB , BC and CA processes 50J50J , 20J20J and 5J5J heat is supplied to an ideal gas . In process AB internal energy of gas increases by 60J60J and in process BC work done by gas is 30J30J . The increases in internal energy of gas in process CA is :
A.50J50J
B.50J - 50J
C.75J75J
D.55J55J

Explanation

Solution

A cyclic process in simple terms is a process that returns to the same thermodynamic state at which it started . In a cyclic process the sum of the internal energy of all the processes involved is always zero .

Complete step by step answer:
Let us first write down all the values which are given to us
Process AB - q=50Jq = 50J , ΔU=60J\Delta U = 60J
Process BC - q=20Jq = 20J , w=30Jw = - 30J (since work is done by the gas so we take it as negative )
Process CA - q=5Jq = 5J
Now , we know according to first law of thermodynamics
ΔU=q+w\Delta U = q + w
ΔU\Delta U = Change in internal energy of the system
qq = Total Heat transferred into the system
ww = Net work done on the system
On substituting the values of process AB in above equation we get ,
60J=50J+w60J = 50J + w
w=10J\Rightarrow w = 10J
On substituting the values of process BC we get ,
ΔU=20J30J\Delta U = 20J - 30J
ΔU=10J\Rightarrow \Delta U = - 10J
Now , for process CA we have to find the increase in internal energy
As we know that the sum of internal energy in a cyclic process is zero , therefore we can find the internal energy of process CA with the help of internal energy of processes AB and BC .
So , ΔU=ΔUAB+ΔUBC+ΔUCA=0\Delta U = \Delta {U_{AB}} + \Delta {U_{BC}} + \Delta {U_{CA}} = 0
So on substituting the values we get
0=60J10J+ΔUCA0 = 60J - 10J + \Delta {U_{CA}}
ΔUCA=50J\Rightarrow \Delta {U_{CA}} = - 50J
Hence the increase in internal energy in process CA is 50J - 50J .
Hence the option B is correct .

Additional Information:
Alternatively this question can be solved by first taking out the work done by the gas in process CA and then taking out its internal energy .
As internal energy of the total process is zero therefore the work done is equal to the heat supplied , that is , (q=w)(q = - w) and the total heat supplied is given as 75J75J .
So work done in process CA is
wAB+wBC+wCA=75{w_{AB}} + {w_{BC}} + {w_{CA}} = - 75
10J30J+wCA=75J10J - 30J + {w_{CA}} = 75J
wCA=55J\Rightarrow {w_{CA}} = - 55J
So , internal energy is
ΔU=5J55J=50J\Delta U = 5J - 55J = - 50J

Note:
According to the first law of thermodynamics, change in internal energy of the system is equal to the sum of the total heat transferred into the system and the total work done on the system. it also varies at different conditions.