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1
For a multicomponent system, the term chemical potential is equivalent to the
Discuss
Answer & Solution
Answer: Option C
Solution:
For multicomponent system the chemical potential is defined as partial Gibbs free energy.
$${\mu _i} = \left( {\frac{{\partial nG}}{{\partial {n_i}}}} \right)T,P,{n_j}$$
2
When liquid and vapour phase of multi-component system are in equilibrium (at a given temperature and pressure), then chemical potential of each component is
Discuss
Answer & Solution
Answer: Option A
Solution:
For thermodynamic equilibrium to satisfy by a system the system should satisfies three conditions
I. Temperature should be same between the phases.
II. Pressure should be same between the phases.(actually the system should not include in any of the work with the surroundings not only in expansion work).
III. Chemical potential between the phases should be same which ensures the equilibrium in mass transfer between the phases.
3
The partial pressure of each constituent present in an alloy is __________ the total vapor pressure exerted by the alloy.
Discuss
Answer & Solution
Answer: Option A
No explanation is given for this question. Let's Discuss on Board
4
Pick out the extensive property out of the following.
Discuss
Answer & Solution
Answer: Option B
Solution:
An extensive property is the one which depend on extent (mass) all the energies like Gibbs free energy, Helmholtz energy, internal energy are extensive properties.
5
Gibbs free energy per mole for a pure substance is equal to the
Discuss
Answer & Solution
Answer: Option B
Solution:
The chemical potential is nothing but partial molar gibbs free energy (since the partial molar functions tells about the change in total molar property with change in composition(moles) we consider partial molar functions as intensive properties),
$${\mu _i} = \left( {\frac{{\partial nG}}{{\partial {n_i}}}} \right)T,P,{n_j}$$
When there is only one component ,G(total molar gibbs free energy) becomes independent of composition(intensive property ) so the equation becomes $${\mu _i} = G\left( {\frac{{\partial {n_I}}}{{\partial {n_i}}}} \right)T,P,{n_j}$$
Hence, $${\mu _i} = G$$
6
A change in state involving a decrease in entropy can be spontaneous, only if
Discuss
Answer & Solution
Answer: Option A
Solution:
From second law of thermodynamics
$$\eqalign{ & TdS \geqslant \delta Q \cr & \Rightarrow TdS \geqslant dU + \partial W \cr} $$
For an irreversible process $$TdS \geqslant dU + \partial W > 0$$
So, the entropy will be greater than zero for an spontaneous(irreversible ) process only when the internal energy and work done are zero so, for an exothermic reaction since the internal energy is not zero we can say the entropy need not be greater than zero.
7
For water at 300°C, it has a vapour pressure 8592.7 kPa and fugacity 6738.9 kPa Under these conditions, one mole of water in liquid phase has a volume of 25.28 cm3 and that in vapour phase in 391.1 cm3. Fugacity of water (in kPa) at 9000 kPa will be
Discuss
Answer & Solution
Answer: Option B
Solution:
We know $$\ln \left( {\frac{f}{{{f^{sat}}}}} \right) = \frac{v}{{RT}}\left( {p - {p^{sat}}} \right)$$      substituting the suitable values we will get $$f=6753.5$$
8
The equation, Cp - Cv = R, is true for __________ gas.
Discuss
Answer & Solution
Answer: Option C
Solution:
$${C_P} - {C_V} = R,$$   is valid for ideal gas and we can prove this by using $$T-dS$$  equations.
9
Duringthe phase transition, __________ changes.
Discuss
Answer & Solution
Answer: Option B
Solution:
During the phase transition the pressure and temperatures remain constant and the volume changes since solids, liquids and gases have different volume.
10
The specific heat of saturated water vapour at 100°C is
Discuss
Answer & Solution
Answer: Option B
Solution:
The specific heat is the amount of heat required to change the temperature of the substance from by unit degree. Since during saturated conditions latent heat conversion only takes place and temperature remains constant the situation appears like the system is of infinite strength and there is no change in thermal energy and hence the heat capacity is infinity.