2 moles of ideal gas is expanded isothermally & reversibly from 1 ...
No. of moles(n) = 2 moles.
Temperature(T) = 300 K.
V₂ = 10 L, and V₁ = 1 L.
Universal Gas Constant (R) = 8.31 J/moleK.
Using the formula,
Work done = -2.303nRTlog(V₂/V₁) [For Chemistry.]
∴ Work done = -2.303 × 2 × 8.31 × 300 × log(10/1)
∴ Work done = -11482.758 J.
∴ Work done = -11.483 kJ.
Now, Process is Isothermal, therefore, Internal Energy will also be zero.
Thus, Using first Law of thermodynamics (of Chemistry and not of physics)
∴ ΔU = ΔQ + w
∴ ΔQ = - w
∴ ΔQ = - (-11.483)
∴ ΔQ = 11.483 kJ ≈ 11.4 kJ.
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2 moles of ideal gas is expanded isothermally & reversibly from 1 ...
Since the process is isothermal, the temperature remains constant throughout the expansion. Therefore, we can use the ideal gas law to relate the initial and final states of the gas:
PV = nRT
where P is the pressure, V is the volume, n is the number of moles, R is the gas constant, and T is the temperature.
Since the number of moles and temperature are constant, we can write:
P1V1 = P2V2
where P1 and V1 are the initial pressure and volume, and P2 and V2 are the final pressure and volume.
Since we know that there are 2 moles of gas, we can also write:
n = 2
Now, let's assume that the initial pressure and volume are P1 and V1, and the final volume is 2V1. Then we can write:
P1V1 = P2(2V1)
or
P2 = P1/2
This means that the final pressure is half of the initial pressure.
Therefore, the gas expands isothermally from initial conditions of P1 and V1 to final conditions of P1/2 and 2V1.
2 moles of ideal gas is expanded isothermally & reversibly from 1 ...
I think correct ans is zero ,, because the process is isothermal reversible process ,, so in case of isothermal reversible process DT=0 so DH=0