Henry's law
Law of mass action
Hess's law
None of these
B. Law of mass action
0.5
3.5
4.5
8.5
Isothermal
Adiabatic
Isentropic
None of these
Low pressure and high temperature
Low pressure and low temperature
Low temperature and high pressure
High temperature and high pressure
Fugacity
Activity co-efficient
Free energy
None of these
RT ln K
-RT ln K
-R ln K
T ln K
2.73
28.3
273
283
Temperature
Pressure
Composition
All (A), (B) and (C)
Cp of monatomic gases such as metallic vapor is about 5 kcal/kg.atom
The heat capacity of solid inorganic substance is exactly equal to the heat capacity of the substance in the molten state
There is an increase in entropy, when a spontaneous change occurs in an isolated system
At absolute zero temperature, the heat capacity for many pure crystalline substances is zero
Zero
Positive
Negative
Indeterminate
0.15
1.5
4.5
6.5
-273
0
-78
5
Number of intermediate chemical reactions involved
Pressure and temperature
State of combination and aggregation in the beginning and at the end of the reaction
None of these
Saturated vapour
Solid
Gas
Liquid
Sub-cooled
Saturated
Non-solidifiable
None of these
Adiabatic expansion
Joule-Thomson effect
Both (A) and (B)
Neither (A) nor (B)
Decrease in velocity
Decrease in temperature
Decrease in kinetic energy
Energy spent in doing work
5 & 3
3.987 & 1.987
1.987 & 0.66
0.66 & 1.987
Heat capacity of a crystalline solid is zero at absolute zero temperature
Heat transfer from low temperature to high temperature source is not possible without external work
Gases having same reduced properties behaves similarly
None of these
35 K
174 K
274 K
154 K
Bertholet equation
Clausius-Clapeyron equation
Beattie-Bridgeman equation
None of these
Temperature vs. enthalpy
Temperature vs. enthalpy
Entropy vs. enthalpy
Temperature vs. internal energy
A gas may have more than one inversion temperatures
The inversion temperature is different for different gases
The inversion temperature is same for all gases
The inversion temperature is the temperature at which Joule-Thomson co-efficient is infinity
No
Any real
Only ideal
Both (B) and (C)
Ideal
Very high pressure
Very low temperature
All of the above
Path
Point
State
None of these
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Increases
Decreases
Remains unchanged
May increase or decrease; depends on the gas
580
640
1160
Data insufficient; can't be computed
By throttling
By expansion in an engine
At constant pressure
None of these
Isothermal
Isobaric
Polytropic
Adiabatic