Directly proportional
Inversely proportional
Equal
None of these
A. Directly proportional
Specific heat at constant pressure (Cp)
Specific heat at constant volume (Cv)
Joule-Thompson co-efficient
None of these
Phase rule variables are intensive properties
Heat and work are both state function
The work done by expansion of a gas in vacuum is zero
CP and CV are state function
RT d ln P
RT d ln f
R d ln f
None of these
Heat pump
Heat engine
Carnot engine
None of these
ds = 0
ds <0
ds > 0
ds = Constant
Minimum
Zero
Maximum
Indeterminate
Vapor compression cycle using expansion valve
Air refrigeration cycle
Vapor compression cycle using expansion engine
Carnot refrigeration cycle
The distribution law
Followed from Margules equation
A corollary of Henry's law
None of these
The available energy in an isolated system for all irreversible (real) processes decreases
The efficiency of a Carnot engine increases, if the sink temperature is decreased
The reversible work for compression in non-flow process under isothermal condition is the change in Helmholtz free energy
All (A), (B) and (C)
State functions
Path functions
Intensive properties
Extensive properties
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Zero
50%
Almost 100%
unpredictable
[∂(G/T)/∂T] = - (H/T2)
[∂(A/T)/∂T]V = - E/T2
Both (A) and (B)
Neither (A) nor (B)
More than
Less than
Equal to
Data insufficient, can't be predicted
Decreases in all spontaneous (or irreversible) processes
Change during a spontaneous process has a negative value
Remains unchanged in reversible processes carried at constant temperature and pressure
All (A), (B) and (C)
Isothermal
Adiabatic
Isobaric
Isochoric
Kp2/Kp1 = - (ΔH/R) (1/T2 - 1/T1)
Kp2/Kp1 = (ΔH/R) (1/T2 - 1/T1)
Kp2/Kp1 = ΔH (1/T2 - 1/T1)
Kp2/Kp1 = - (1/R) (1/T2 - 1/T1)
-1.87
0
1.26
3.91
If an insoluble gas is passed through a volatile liquid placed in a perfectly insulated container, the temperature of the liquid will increase
A process is irreversible as long as Δ S for the system is greater than zero
The mechanical work done by a system is always equal to∫P.dV
The heat of formation of a compound is defined as the heat of reaction leading to the formation of the compound from its reactants
Maxwell's equation
Thermodynamic equation of state
Equation of state
Redlich-Kwong equation of state
Zero
+ve
-ve
Dependent on the path
The surface tension vanishes
Liquid and vapour have the same density
There is no distinction between liquid and vapour phases
All (A), (B) and (C)
Heating occurs
Cooling occurs
Pressure is constant
Temperature is constant
0
< 0
< 1
> 1
dQ = dE + dW
dQ = dE - dW
dE = dQ + dW
dW = dQ + dE
RT ln K
-RT ln K
-R ln K
T ln K
-94 kcal
+94 kcal
> 94 kcal
< -94 kcal
Entropy
Gibbs free energy
Internal energy
All (A), (B) & (C)
0°C
273°C
100°C
-273°C
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