Melting of ice
Condensation of alcohol vapor
Sudden bursting of a cycle tube
Evaporation of water
C. Sudden bursting of a cycle tube
Mass
Energy
Momentum
None of these
(∂P/∂V)T
(∂V/∂T)P
(∂P/∂V)V
All (A), (B) & (C)
Positive
Negative
Zero
May be positive or negative
Molar heat capacity
Internal energy
Viscosity
None of these
Van Laar equation
Margules equation
Wilson's equation
All (A), (B) and (C)
Molecular size
Volume
Pressure
Temperature
0
1
2
3
A heating effect
No change in temperature
A cooling effect
Either (A) or (C)
In an isothermal system, irreversible work is more than reversible work
Under reversible conditions, the adiabatic work is less than isothermal work
Heat, work, enthalpy and entropy are all 'state functions'
Matter and energy cannot be exchanged with the surroundings in a closed system
Increases
Decreases
Remains unchanged
Decreases linearly
Critical properties
Specific gravity
Specific volume
Thermal conductivity
A = H - TS
A = E - TS
A = H + TS
None of these
0
1
2
3
Heating takes place
Cooling takes place
Pressure is constant
Temperature is constant
RT d ln P
RT d ln f
R d ln f
None of these
Low temperature
High pressure
Both (A) and (B)
Neither (A) nor (B)
0
1
2
3
Increased COP
Same COP
Decreased COP
Increased or decreased COP; depending upon the type of refrigerant
d ln p/dt = Hvap/RT2
d ln p/dt = RT2/Hvap
dp/dt = RT2/Hvap
dp/dt = Hvap/RT2
Cold reservoir approaches zero
Hot reservoir approaches infinity
Either (A) or (B)
Neither (A) nor (B)
Air compressor
Liquid cooling system of an automobile
Boiler
None of these
System (of partially miscible liquid pairs), in which the mutual solubility increases with rise in temperature, are said to possess an upper consolute temperature
Systems, in which the mutual solubility increases with decrease in temperature, are said to possess lower consolute temperature
Nicotine-water system shows both an upper as well as a lower consolute temperature, implying that they are partially miscible between these two limiting temperatures
None of these
2.73
28.3
273
283
Enthalpy
Volume
Both 'a' & 'b'
Neither 'a' nor 'b'
Zero
Positive
Negative
Indeterminate
Stirling
Brayton
Rankine
None of these
State functions
Path functions
Intensive properties
Extensive properties
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
Binary solutions
Ternary solutions
Azeotropic mixture only
None of these
Volume
Mass
Critical temperature
None of these