Ice at the base contains impurities which lowers its melting point
Due to the high pressure at the base, its melting point reduces
The iceberg remains in a warmer condition at the base
All (A), (B) and (C)
B. Due to the high pressure at the base, its melting point reduces
Decreases
Decreases exponentially
Increases
Remain constant
Heat capacity
Molal heat capacity
Pressure
Concentration
Freezing
Triple
Boiling
Boyle
Fugacity
Partial pressure
Activity co-efficient
All (A), (B), and (C)
0
> 0
< 0
None of these
Polar
Non-polar
Both (A) & (B)
Neither (A) nor (B)
(atm)Δx, when Δx is negative
(atm)Δx, when Δx is positive
Dimensionless, when Δx = 0
(atm)Δx2, when Δx > 0
Solubility increases as temperature increases
Solubility increases as temperature decreases
Solubility is independent of temperature
Solubility increases or decreases with temperature depending on the Gibbs free energy change of solution
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
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Volume of the liquid phase is negligible compared to that of vapour phase
Vapour phase behaves as an ideal gas
Heat of vaporisation is independent of temperature
All (A), (B) & (C)
Entropy
Temperature
Internal energy
Enthalpy
Third law of thermodynamics
Second law of thermodynamics
Nernst heat theorem
Maxwell's relations
5 & 3
3.987 & 1.987
1.987 & 0.66
0.66 & 1.987
Closed
Open
Isolated
Non-thermodynamic
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
Less
More
Same
More or less depending upon the extent of work done
0
273
25
None of these
Zeroth
First
Second
Third
< 0
> 0
= 0
None of these
Equilibrium cannot be established
More ice will be formed
More water will be formed
Evaporation of water will take place
Isothermal
Adiabatic
Isobaric
Isochoric
Less than
More than
Equal to or higher than
Less than or equal to
T1/(T1-T2)
T2/(T1-T2)
T1/T2
T2/R1
dE = CpdT
dE = CvdT
dQ = dE + pdV
dW = pdV
Vapor pressure
Partial pressure
Chemical potential
None of these
Matter
Energy
Neither matter nor energy
Both matter and energy
The melting point of wax
The boiling point of a liquid
Both (A) and (B)
Neither (A) nor (B)
No heat and mass transfer
No mass transfer but heat transfer
Mass and energy transfer
None of these
Calorific value
Heat of reaction
Heat of combustion
Heat of formation