Hookes law
Yield point
Plastic flow
Proof stress
C. Plastic flow
(Net work output)/(Workdone by the turbine)
(Net work output)/(Heat supplied)
(Actual temperature drop)/(Isentropic temperature drop)
(Isentropic increase in temperature)/(Actual increase in temperature)
Steel only
Concrete only
Steel and concrete both
None of these
Coal gas
Producer gas
Mond gas
Blast furnace gas
Ru × T
1.5 Ru × T
2 Ru × T
3 Ru × T
Reversible cycles
Irreversible cycles
Semi-reversible cycles
Quasi-static cycles
Increases power output
Improves thermal efficiency
Reduces exhaust temperature
Do not damage turbine blades
Increase
Decrease
Remain unchanged
Increase/decrease depending on application
√(KT/m)
√(2KT/m)
√(3KT/m)
√(5KT/m)
Becomes constant
Starts decreasing
Increases without any increase in load
None of the above
1 g
10 g
100 g
1000 g
Strains
Stress and strain
Shear stress and shear strain
Moduli and elasticity
Zero
Minimum
Maximum
Infinity
Its own length
Twice its length
Half its length
1/√2 × its length
A horizontal line
A vertical line
An inclined line
A parabolic curve
23.97 bar
25 bar
26.03 bar
34.81 bar
Isochoric process
Isobaric process
Hyperbolic process
All of these
(11/3) CO2 + (3/7) CO
(3/7) CO2 + (11/3) CO
(7/3) CO2 + (3/11) CO
(3/11) CO2 + (7/3) CO
1 × 102 N/m2
1 × 103 N/m2
1 × 104 N/m2
1 × 105 N/m2
Workdone
Entropy
Enthalpy
None of these
0.086
1.086
1.086
4.086
Carnot cycle
Rankine cycle
Brayton cycle
Bell Coleman cycle
Tensile strain increases more quickly
Tensile strain decreases more quickly
Tensile strain increases in proportion to the stress
Tensile strain decreases in proportion to the stress
Mono-atomic
Di-atomic
Tri-atomic
Poly-atomic
Constant volume
Constant temperature
Constant pressure
None of these
M/I = σ/y = E/R
T/J = τ/R = Cθ/l
M/R = T/J = Cθ/l
T/l= τ/J = R/Cθ
Change
Do not change
Both (A) and (B)
None of these
Equal to
Half
Double
Quadruple
L = l/2
L = l/√2
L = l
L = 2l
Short columns
Long columns
Weak columns
Medium columns
δl = 4PE/ πl²
δl = 4πld²/PE
δl = 4Pl/πEd₁d₂
δl = 4PlE/ πd₁d₂