It should be non-explosive
It should have a sub-atmospheric vapor pressure at the temperature in refrigerator coils
Its vapor pressure at the condenser temperature should be very high
None of these
B. It should have a sub-atmospheric vapor pressure at the temperature in refrigerator coils
Calorific value
Heat of reaction
Heat of combustion
Heat of formation
Infinity
Unity
Constant
Negative
-94 kcal
+94 kcal
> 94 kcal
< -94 kcal
Surface tension of a substance vanishes at critical point, as there is no distinction between liquid and vapour phases at its critical point
Entropy of a system decreases with the evolution of heat
Change of internal energy is negative for exothermic reactions
The eccentric factor for all materials is always more than one
Adiabatic process
Endothermic reaction
Exothermic reaction
Process involving a chemical reaction
1
< 1
> 1
>> 1
Critical temperature
Melting point
Freezing point
Both (B) and (C)
Decreases
Increases
Remains constant
Decreases logarithmically
(∂T/∂V)S = (∂p/∂S)V
(∂T/∂P)S = (∂V/∂S)P
(∂P/∂T)V = (∂S/∂V)T
(∂V/∂T)P = -(∂S/∂P)T
RT d ln P
R d ln P
R d ln f
None of these
∞
+ve
0
-ve
-273
0
-78
5
dP/dT = ΔH/TΔV
ln P = - (ΔH/RT) + constant
ΔF = ΔH + T [∂(ΔF)/∂T]P
None of these
(∂T/∂V)S, ni = -(∂P/∂S)V, ni
(∂S/∂P)T, ni = (∂V/∂T)P, ni
(∂S/∂V)T, ni = (∂P/∂T)V, ni
(∂T/∂P)S, ni = (∂V/∂S)P, ni
1.572
1.9398
3.389
4.238
Like internal energy and enthalpy, the absolute value of standard entropy for elementary substances is zero
Melting of ice involves increase in enthalpy and a decrease in randomness
The internal energy of an ideal gas depends only on its pressure
Maximum work is done under reversible conditions
Increase
Decrease
Remain unchanged
First fall and then rise
Expansion valve
Condenser
Refrigerator
Compressor
Adiabatic
Isometric
Isentropic
Isothermal
Property of the system
Path function
Point function
State description of a system
Isothermal
Adiabatic
Isentropic
Polytropic
Below
At
Above
Either 'b' or 'c'
Reversible isothermal volume change
Heating of a substance
Cooling of a substance
Simultaneous heating and expansion of an ideal gas
5 & 3
3.987 & 1.987
1.987 & 0.66
0.66 & 1.987
Solution
Vaporisation
Formation
Sublimation
Zero
Unity
Infinity
An indeterminate value
Zero
Negative
Very large compared to that for endothermic reaction
Not possible to predict
Chemical potential
Fugacity
Both (A) and (B)
Neither (A) nor (B)
Ideal compression of air
Free expansion of an ideal gas
Adiabatic expansion of steam in a turbine
Adiabatic compression of a perfect gas
Extensive property
Intensive property
Force which drives the chemical system to equilibrium
Both (B) and (C)