Disorder
Orderly behaviour
Temperature changes only
None of these
A. Disorder
Hour
Day
Minute
Second
At constant pressure
By throttling
By expansion in an engine
None of these
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
Isothermal
Adiabatic
Isobaric
Isometric
Superheated vapour
Partially condensed vapour with quality of 0.9
Saturated vapour
Partially condensed vapour with quality of 0.1
Slower than Y
Faster than Y
Three times slower than Y
Three times faster than Y
Work required to refrigeration obtained
Refrigeration obtained to the work required
Lower to higher temperature
Higher to lower temperature
Activity
Fugacity
Activity co-efficient
Fugacity co-efficient
(atm)Δx, when Δx is negative
(atm)Δx, when Δx is positive
Dimensionless, when Δx = 0
(atm)Δx2, when Δx > 0
Fugacity
Activity co-efficient
Free energy
None of these
Addition of inert gas favours the forward reaction, when Δx is positive
Pressure has no effect on equilibrium, when Δn = 0
Addition of inert gas has no effect on the equilibrium constant at constant volume for any value of Δx (+ ve, - ve) or zero)
All 'a', 'b' & 'c'
Less pronounced
More pronounced
Equal
Data insufficient, can't be predicted
Temperature
Mass
Volume
Pressure
Increases
Decreases
Remain constant
Increases linearly
More
Less
Same
Unpredictable; depends on the particular reaction
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
Temperature
Pressure
Volume
None of these
Mass
Energy
Momentum
None of these
Tds = dE + dW
dE - dW = Tds
dW - dE = Tds
Tds - dW + dE >0
72
92
142
192
Indeterminate
Zero
Negative
None of these
Shift the equilibrium towards right
Give higher yield of NH3
Both (B) and (C)
Neither (A) nor (B)
Entropy
Gibbs energy
Internal energy
Enthalpy
Volume
Density
Temperature
Pressure
(∂T/∂V)S = (∂p/∂S)V
(∂T/∂P)S = (∂V/∂S)P
(∂P/∂T)V = (∂S/∂V)T
(∂V/∂T)P = -(∂S/∂P)T
Activity co-efficient is dimensionless.
In case of an ideal gas, the fugacity is equal to its pressure.
In a mixture of ideal gases, the fugacity of a component is equal to the partial pressure of the component.
The fugacity co-efficient is zero for an ideal gas
T2/(T1 - T2)
T1/(T1 - T2)
(T1 - T2)/T1
(T1 - T2)/T2
He
N2
O2
H2
Below
At
Above
Either 'b' or 'c'
If an insoluble gas is passed through a volatile liquid placed in a perfectly insulated container, the temperature of the liquid will increase
A process is irreversible as long as Δ S for the system is greater than zero
The mechanical work done by a system is always equal to∫P.dV
The heat of formation of a compound is defined as the heat of reaction leading to the formation of the compound from its reactants