Expansion in an engine
Following a constant pressure cycle
Throttling
None of these
A. Expansion in an engine
More
Less
Same
Data insufficient to predict
Zeroth
First
Second
Third
Less than
More than
Equal to or higher than
Less than or equal to
Isobaric
Adiabatic
Isenthalpic
Both (B) & (C)
More than
Less than
Equal to
Not related to
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
Zero
Negative
More than zero
Indeterminate
Enthalpy does not remain constant
Entire apparatus is exposed to surroundings
Temperature remains constant
None of these
Zero
Unity
Infinity
None of these
The distribution law
Followed from Margules equation
A corollary of Henry's law
None of these
Straight line
Sine curve
Parabola
Hyperbola
Volume
Temperature
Pressure
None of these
Decrease on addition of Cl2
Increase on addition of an inert gas at constant pressure
Decrease on increasing the pressure of the system
None of these
Contracts
Expands
Has same volume
May contract or expand
n = y = 1.4
n = 0
n = 1
n = 1.66
Disorder
Orderly behaviour
Temperature changes only
None of these
Freon
Liquid sulphur dioxide
Methyl chloride
Ammonia
its internal energy (U) decreases and its entropy (S) increases
U and S both decreases
U decreases but S is constant
U is constant but S decreases
The expansion of a gas in vacuum is an irreversible process
An isometric process is a constant pressure process
Entropy change for a reversible adiabatic process is zero
Free energy change for a spontaneous process is negative
Tds = dE - dW = 0
dE - dW - Tds = 0
Tds - dE + dW < 0
Tds - dT + dW < 0
λb/Tb
Tb/λb
√(λb/Tb)
√(Tb/λb)
Saturated vapour
Solid
Gas
Liquid
-2 RT ln 0.5
-RT ln 0.5
0.5 RT
2 RT
Value of absolute entropy
Energy transfer
Direction of energy transfer
None of these
2
0
1
3
Initial concentration of the reactant
Pressure
Temperature
None of these
Phase rule variables are intensive properties
Heat and work are both state function
The work done by expansion of a gas in vacuum is zero
CP and CV are state function
No heat and mass transfer
No mass transfer but heat transfer
Mass and energy transfer
None of these
Is the most efficient of all refrigeration cycles
Has very low efficiency
Requires relatively large quantities of air to achieve a significant amount of refrigeration
Both (B) and (C)
Fugacity
Activity co-efficient
Free energy
None of these