Proportional limit, elastic limit, yielding, failure
Elastic limit, proportional limit, yielding, failure
Yielding, proportional limit, elastic limit, failure
None of the above
A. Proportional limit, elastic limit, yielding, failure
8/3
11/3
11/7
7/3
Isothermal process
Hyperbolic process
Adiabatic process
Polytropic process
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
M/I = σ/y = E/R
T/J = τ/R = Cθ/l
M/R = T/J = Cθ/l
T/l= τ/J = R/Cθ
(σx/2) + (1/2) × √(σx² + 4 τ²xy)
(σx/2) - (1/2) × √(σx² + 4 τ²xy)
(σx/2) + (1/2) × √(σx² - 4 τ²xy)
(1/2) × √(σx² + 4 τ²xy)
W1 - 2 = 0
Q1 - 2 = 0
dU = 0
All of these
pv = mRT
pv = RTm
pvm = C
pv = (RT)m
3p/E × (2/m - 1)
3p/E × (2 - m)
3p/E × (1 - 2/m)
E/3p × (2/m - 1)
Increasing the highest temperature
Decreasing the highest temperature
Increasing the lowest temperature
Keeping the lowest temperature constant
1 kg of water
7 kg of water
8 kg of water
9 kg of water
(11/3) CO2 + (3/7) CO
(3/7) CO2 + (11/3) CO
(7/3) CO2 + (3/11) CO
(3/11) CO2 + (7/3) CO
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Of same magnitude as that of bar and applied at the lower end
Half the weight of bar applied at lower end
Half of the square of weight of bar applied at lower end
One fourth of weight of bar applied at lower end
(p2/p1)γ - 1/ γ
(p1/p2)γ - 1/ γ
(v2/v1)γ - 1/ γ
(v1/v2)γ - 1/ γ
OC
OP
OQ
PQ
Equal to
Half
Double
Quadruple
Constant pressure cycle
Constant volume cycle
Constant temperature cycle
Constant temperature and pressure cycle
√(KT/m)
√(2KT/m)
√(3KT/m)
√(5KT/m)
1
0
-1
10
When coal is first dried and then crushed to a fine powder by pulverising machine
From the finely ground coal by moulding under pressure with or without a binding material
When coal is strongly heated continuously for 42 to 48 hours in the absence of air in a closed vessel
By heating wood with a limited supply of air to a temperature not less than 280°C
2
4
8
16
Greater than Carnot cycle
Less than Carnot cycle
Equal to Carnot cycle
None of these
Isothermal expansion
Isentropic expansion
Isothermal compression
Isentropic compression
Zero
Minimum
Maximum
Positive
Rankine
Stirling
Carnot
Brayton
Double
Half
Same
None of these
All the reversible engines have the same efficiency.
All the reversible and irreversible engines have the same efficiency.
Irreversible engines have maximum efficiency.
All engines are designed as reversible in order to obtain maximum efficiency.
Permanent
Temporary
Semi-permanent
None of these
1
1.4
1.67
1.87
It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is possible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is impossible to construct a device which operates in a cyclic process and produces no effect other than the transfer of heat from a cold body to a hot body
None of the above