Freon
Liquid sulphur dioxide
Methyl chloride
Ammonia
A. Freon
0°C and 760 mm Hg
15°C and 760 mm Hg
20°C and 760 mm Hg
0°C and 1 kgf/cm2
d ln p/dt = Hvap/RT2
d ln p/dt = RT2/Hvap
dp/dt = RT2/Hvap
dp/dt = Hvap/RT2
Increase the partial pressure of I2
Decrease the partial pressure of HI
Diminish the degree of dissociation of HI
None of these
Zero
Positive
Negative
None of these
Escaping tendencies of the same substance in different phases of a system
Relative volatility of a mixture of two miscible liquids
Behaviour of ideal gases
None of these
Pressure
Volume
Mass
None of these
More than
Less than
Equal to
Data insufficient, can't be predicted
x
x + 1
x + 2
x + 3
Zero
Unity
Infinity
An indeterminate value
Always greater than one
Same at the same reduced temperature
Same at the same reduced pressure
Both (B) & (C)
Isothermal
Adiabatic
Isobaric
Isochoric
Direction of energy transfer
Reversible processes only
Irreversible processes only
None of these
No
Any real
Only ideal
Both (B) and (C)
Isothermally
Isobarically
Adiabatically
None of these
In which there is a temperature drop
Which is exemplified by a non-steady flow expansion
Which can be performed in a pipe with a constriction
In which there is an increase in temperature
Expansion valve
Condenser
Refrigerator
Compressor
The amount of work needed is path dependent
Work alone cannot bring out such a change of state
The amount of work needed is independent of path
More information is needed to conclude anything about the path dependence or otherwise of the work needed
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
12 P1V1
6 P1 V1
3 P1V1
P1 V1
Turbine
Heat engine
Reversed heat engine
None of these
R loge 4
R log10 4
Cv log10 4
Cv loge 4
Ideal
Real
Isotonic
None of these
Zero
50%
Almost 100%
unpredictable
Lewis-Randall
Margules
Van Laar
Both (B) & (C)
Molar concentration
Temperature
Internal energy
None of these
Only enthalpy change (ΔH) is negative
Only internal energy change (ΔE) is negative
Both ΔH and ΔE are negative
Enthalpy change is zero
Trouton's ratio of non-polar liquids is calculated using Kistyakowsky equation
Thermal efficiency of a Carnot engine is always less than 1
An equation relating pressure, volume and temperature of a gas is called ideal gas equation
None of these
At constant pressure
By throttling
By expansion in an engine
None of these
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)
Mass
Momentum
Energy
None of these