Indeterminate
Zero
Negative
None of these
B. Zero
The values of (∂P/∂V)T and (∂2P/∂V2)T are zero for a real gas at its critical point
Heat transferred is equal to the change in the enthalpy of the system, for a constant pressure, non-flow, mechanically reversible process
Thermal efficiency of a Carnot engine depends upon the properties of the working fluid besides the source & sink temperatures
During a reversible adiabatic process, the entropy of a substance remains constant
The melting point of wax
The boiling point of a liquid
Both (A) and (B)
Neither (A) nor (B)
Enthalpy remains constant
Entropy remains constant
Temperature remains constant
None of these
Solution
Formation
Dilution
Combustion
A closed system does not permit exchange of mass with its surroundings but may permit exchange of energy.
An open system permits exchange of both mass and energy with its surroundings
The term microstate is used to characterise an individual, whereas macro-state is used to designate a group of micro-states with common characteristics
None of the above
Only ΔE = 0
Only ΔH =0
ΔE = ΔH = 0
dQ = dE
He
N2
O2
H2
Heating occurs
Cooling occurs
Pressure is constant
Temperature is constant
Amount of energy transferred
Direction of energy transfer
Irreversible processes only
Non-cyclic processes only
270
327
300
540
0
∞
+ve
-ve
A refrigeration cycle violates the second law of thermodynamics
Refrigeration cycle is normally represented by a temperature vs. entropy plot
In a refrigerator, work required decreases as the temperature of the refrigerator and the temperature at which heat is rejected increases
One ton of refrigeration is equivalent to the rate of heat absorption equal to 3.53 kW
2
0
3
1
Two different gases behave similarly, if their reduced properties (i.e. P, V and T) are same
The surface of separation (i. e. the meniscus) between liquid and vapour phase disappears at the critical temperature
No gas can be liquefied above the critical temperature, howsoever high the pressure may be.
The molar heat of energy of gas at constant volume should be nearly constant (about 3 calories)
Zero
+ve
-ve
Dependent on the path
Pressure must be kept below 5.2 atm
Temperature must be kept above - 57°C
Pressure must be kept below 5.2 atm. and temperature must be kept above 57°C
Pressure and temperature must be kept below 5.2 atm. and - 57°C respectively
Volume
Mass
Critical temperature
None of these
Freezing
Triple
Boiling
Boyle
Specific heat
Latent heat of vaporisation
Viscosity
Specific vapor volume
Not a function of its pressure
Not a function of its nature
Not a function of its temperature
Unity, if it follows PV = nRT
∞
0
Maximum
Minimum
Isothermal
Isentropic
Isobaric
Adiabatic
Reversible isothermal
Irreversible isothermal
Reversible adiabatic
None of these
Minimum temperature attainable
Temperature of the heat reservoir to which a Carnot engine rejects all the heat that is taken in
Temperature of the heat reservoir to which a Carnot engine rejects no heat
None of these
Reversible isothermal volume change
Heating of a substance
Cooling of a substance
Simultaneous heating and expansion of an ideal gas
μi = (∂F/∂ni)T, P, ni
μi = (∂A/∂ni)T, P, ni
μi = (∂F/∂ni)T, P
μi = (∂A/∂ni)T, P
Virial co-efficients are universal constants
Virial co-efficients 'B' represents three body interactions
Virial co-efficients are function of temperature only
For some gases, Virial equations and ideal gas equations are the same
Entropy
Gibbs free energy
Internal energy
All (A), (B) & (C)
Isothermal
Adiabatic
Isentropic
None of these
448
224
22.4
Data insufficient; can't be computed