Due to current
i=2 A flowing through the resistance
R, the rate of energy dissipated in resistance is the source of energy for workdone by the gas.
Rate of energy supplied by resistance.
dQdt=i2R=(2)2×10=40 J/s
Using first law of thermodynamics:
dQ=dU+dW
⇒dQdt=dUdt+dWdt.....(i)
(for adiabatic walls of cylinder no heat is last, which is supplied by resistance)
Also to maintain the temperature of gas inside cylinder
ΔT=0 i..e dU = 0 or
dUdt=0
We can write the work done by gas,
dW=PdV
⇒dWdt=PdVdt
Let area of cross -section of pistion is
A, thus the change in volume of gas due to piston displacement will be;
dV=Adx
or,
dWdt=P(Adx)dt=PA(dxdt).....(ii)
The force on piston due to gas is,
Fgas=P×A=PA
Applying equilibrium condition on piston (v = constant, a = 0)
⇒PA=mg
∴P=mgA
Substituting in equation (ii),
dWdt=mgA×A×(dxdt)
or
dWdt=mg(dxdt)=mgv ....(iii)
Here
dxdt=v=constant
From Eq. (i) & (iii):
dQdt=0+mgv
⇒40=(1×10)v
∴v=4 m/s
Why this question?Tip: In this problem the heat is supplied to thegas by resistance and that heat is completelyavailable for work done by gas (adiabatic walls ΔQ=0).Thus the power dissipated in resistance must be able toovercome the power of gravity only then piston canmove with constant velocity.