Concentration of the constituents only
Quantities of the constituents only
Temperature only
All (A), (B) and (C)
D. All (A), (B) and (C)
Increase the partial pressure of H2
Increase the partial pressure of I2
Increase the total pressure and hence shift the equilibrium towards the right
Not affect the equilibrium conditions
F = A + PV
F = E + A
F = A - TS
F = A + TS
High thermal conductivity
Low freezing point
Large latent heat of vaporisation
High viscosity
0
< 0
< 1
> 1
Third law of thermodynamics
Second law of thermodynamics
Nernst heat theorem
Maxwell's relations
Less than
Equal to
More than
Either (B) or (C); depends on the type of alloy
+ve
0
-ve
∞
Melting of ice
Condensation of alcohol vapor
Sudden bursting of a cycle tube
Evaporation of water
Enthalpies of all elements in their standard states are assumed to be zero
Combustion reactions are never endothermic in nature
Heat of reaction at constant volume is equal to the change in internal energy
Clausius-Clapeyron equation is not applicable to melting process
Not changed
Decreasing
Increasing
Data sufficient, can't be predicted
Expansion of a real gas
Reversible isothermal volume change
Heating of an ideal gas
Cooling of a real gas
Property of the system
Path function
Point function
State description of a system
0
∞
50
100
Solution
Formation
Dilution
Combustion
Zero
Positive
Negative
None of these
Less
More
Same
Dependent on climatic conditions
Temperature vs. enthalpy
Temperature vs. enthalpy
Entropy vs. enthalpy
Temperature vs. internal energy
Tds = dE - dW = 0
dE - dW - Tds = 0
Tds - dE + dW < 0
Tds - dT + dW < 0
2.73
28.3
273
283
Isolated
Open
Insulated
Closed
State functions
Path functions
Intensive properties
Extensive properties
Pressure
Volume
Temperature
All (A), (B) and (C)
0
1
2
3
270
327
300
540
Any
A perfect
An easily liquefiable
A real
Directly proportional
Inversely proportional
Equal
None of these
Polar
Non-polar
Both (A) & (B)
Neither (A) nor (B)
Less
More
Same
More or less depending upon the extent of work done
Helmholtz
Gibbs
Both a & b
Neither 'a' nor 'b'
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