Only ΔE = 0
Only ΔH =0
ΔE = ΔH = 0
dQ = dE
C. ΔE = ΔH = 0
Joule-Thomson co-efficient
Specific heat at constant pressure (Cp)
co-efficient of thermal expansion
Specific heat at constant volume (CV)
Compression ratio of an Otto engine is comparatively higher than a diesel engine
Efficiency of an Otto engine is higher than that of a diesel engine for the same compression ratio
Otto engine efficiency decreases with the rise in compression ratio, due to decrease in work produced per quantity of heat
Diesel engine normally operates at lower compression ratio than an Otto engine for an equal output of work
Unity
Zero
That of the heat of reaction
Infinity
Directly proportional
Inversely proportional
Equal
None of these
Always greater than one
Same at the same reduced temperature
Same at the same reduced pressure
Both (B) & (C)
Internal energy
Enthalpy
Gibbs free energy
Helmholtz free energy
Cp/Cv
Cp/(CP-R)
1 + (R/CV)
All (A), (B) and (C)
0
∞
+ ve
- ve
Δ H = 0 and ΔS = 0
Δ H ≠ 0 and ΔS = 0
Δ H ≠ 0 and ΔS ≠ 0
Δ H = 0 and ΔS ≠ 0
Infinity
Minus infinity
Zero
None of these
Enthalpies of all elements in their standard states are assumed to be zero
Combustion reactions are never endothermic in nature
Heat of reaction at constant volume is equal to the change in internal energy
Clausius-Clapeyron equation is not applicable to melting process
Pressure
Temperature
Both (A) & (B)
Neither (A) nor (B)
Surface tension
Free energy
Specific heat
Refractive index
At low temperature and high pressure
At standard state
Both (A) and (B)
In ideal state
Conduction
Convection
Radiation
Condensation
Decreases
Increases
Remain same
Decreases linearly
2.73
28.3
273
283
Sublimation
Vaporisation
Melting
Either (A), (B) or (C)
Reversible isothermal
Irreversible isothermal
Reversible adiabatic
None of these
Decreases in all spontaneous (or irreversible) processes
Change during a spontaneous process has a negative value
Remains unchanged in reversible processes carried at constant temperature and pressure
All (A), (B) and (C)
Isometric
Polytropic
Isentropic
Isobaric
300 × (32/7)
300 × (33/5)
300 × (333/7)
300 × (35/7)
Tds = dE - dW = 0
dE - dW - Tds = 0
Tds - dE + dW < 0
Tds - dT + dW < 0
1.987 cal/gm mole °K
1.987 BTU/lb. mole °R
Both (A) and (B)
Neither (A) nor (B)
Molar concentration
Temperature
Internal energy
None of these
dE = CpdT
dE = CvdT
dQ = dE + pdV
dW = pdV
0
1
2
3
Molecular size
Volume
Pressure
Temperature
Zero
+ve
-ve
Dependent on the path
4 J
∞
0
8 J