Steam to ethylene ratio
Temperature
Pressure
None of these
D. None of these
Heating takes place
Cooling takes place
Pressure is constant
Temperature is constant
Less than
Equal to
More than
Either (B) or (C); depends on the type of alloy
States that n1dμ1 + n2dμ2 + ....njdμj = 0, for a system of definite composition at constant temperature and pressure
Applies only to binary systems
Finds no application in gas-liquid equilibria involved in distillation
None of these
Maxwell's equation
Clausius-Clapeyron Equation
Van Laar equation
Nernst Heat Theorem
Pressure to critical pressure
Critical pressure to pressure
Pressure to pseudocritical pressure
Pseudocritical pressure to pressure
Temperature
Mass
Volume
Pressure
Solution
Formation
Dilution
Combustion
Independent of pressure
Independent of temperature
Zero at absolute zero temperature for a perfect crystalline substance
All (A), (B) & (C)
State function
Macroscopic property
Extensive property
None of these
Is increasing
Is decreasing
Remain constant
Data insufficient, can't be predicted
Kelvin's
Antoines
Kirchoffs
None of these
Both the processes are adiabatic
Both the processes are isothermal
Process A is isothermal while B is adiabatic
Process A is adiabatic while B is isothermal
Pressure
Composition
Temperature
All (A), (B) and (C)
Not liquify (barring exceptions)
Immediately liquify
Never liquify however high the pressure may be
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
Increases with rise in pressure
Decreases with rise in pressure
Is independent of pressure
Is a path function
Expansion of an ideal gas against constant pressure
Atmospheric pressure vaporisation of water at 100°C
Solution of NaCl in water at 50°C
None of these
0
1
2
3
Vapor compression cycle using expansion valve
Air refrigeration cycle
Vapor compression cycle using expansion engine
Carnot refrigeration cycle
Solid-vapor
Solid-liquid
Liquid-vapor
All (A), (B) and (C)
-94 kcal
+94 kcal
> 94 kcal
< -94 kcal
He
N2
O2
H2
1
< 1
> 1
>> 1
High thermal conductivity
Low freezing point
Large latent heat of vaporisation
High viscosity
dP/dT = ΔH/TΔV
ln P = - (ΔH/RT) + constant
ΔF = ΔH + T [∂(ΔF)/∂T]P
None of these
Only ΔE = 0
Only ΔH =0
ΔE = ΔH = 0
dQ = dE
0
∞
+ve
-ve
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
Work required to refrigeration obtained
Refrigeration obtained to the work required
Lower to higher temperature
Higher to lower temperature
Heating occurs
Cooling occurs
Pressure is constant
Temperature is constant