wl/4
wl/2
wl
wl²/2
D. wl²/2
Pressure exerted by the gas
Volume occupied by the gas
Temperature of the gas
All of these
No heat enters or leaves the gas
The temperature of the gas changes
The change in internal energy is equal to the mechanical workdone
All of the above
(p1 v1 - p2 v2)/(γ - 1)
[m R (T1 - T2)] /(γ - 1)
[m R T1/(γ - 1)][1 - (p2 v2 /p1 v1)]
All of these
Kh > Ks
Kh < Ks
Kh = Ks
None of these
Longitudinal stress to longitudinal strain
Volumetric stress to volumetric strain
Lateral stress to Lateral strain
Shear stress to shear strain
Acts at a point on a beam
Spreads non-uniformly over the whole length of a beam
Spreads uniformly over the whole length of a beam
Varies uniformly over the whole length of a beam
Heat
Work
Internal energy
Entropy
Thermodynamic law
Thermodynamic process
Thermodynamic cycle
None of these
Oxygen
Sulphur
Nitrogen
Carbon
Calorific value
Heat energy
Lower calorific value
Higher calorific value
Carbon and hydrogen
Oxygen and hydrogen
Sulphur and oxygen
Sulphur and hydrogen
Ideal materials
Uniform materials
Isotropic materials
Piratical materials
0.5 s.l.σt
s.l.σt
√2 s.l.σt
2.s.l.σt
3 to 6
5 to 8
10 to 20
15 to 30
(23/100) × Mass of excess carbon
(23/100) × Mass of excess oxygen
(100/23) × Mass of excess carbon
(100/23) × Mass of excess oxygen
Isothermal process
Adiabatic process
Hyperbolic process
Polytropic process
cv/ cp =R
cp - cv = R
cv = R/ γ-1
Both (B) and (C)
Area of cross-section of the column
Length and least radius of gyration of the column
Modulus of elasticity for the material of the column
All of the above
l/δl
δl/l
l.δl
l + δl
Temperature limits
Pressure ratio
Compression ratio
Cut-off ratio and compression ratio
2ε₁ - ε₂
2ε₁ + ε₂
2ε₂ - ε₁
2ε₂ + ε₁
Pitch
Back pitch
Diagonal pitch
Diametric pitch
(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)
(p - 2d) t × σc
(p - d) t × τ
(p - d) t × σt
(2p - d) t × σt
Energy stored in a body when strained within elastic limits
Energy stored in a body when strained up to the breaking of the specimen maximum strain
Energy which can be stored in a body
None of the above
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
For a given compression ratio, both Otto and Diesel cycles have the same efficiency.
For a given compression ratio, Otto cycle is more efficient than Diesel cycle.
For a given compression ratio, Diesel cycle is more efficient than Otto cycle.
The efficiency of Otto or Diesel cycle has nothing to do with compression ratio.
Increases the internal energy of the gas
Increases the temperature of the gas
Does some external work during expansion
Both (B) and (C)
The deformation of the bar per unit length in the direction of the force is called linear strain.
The Poisson's ratio is the ratio of lateral strain to the linear strain.
The ratio of change in volume to the original volume is called volumetric strain.
The bulk modulus is the ratio of linear stress to the linear strain.
Elements
Compounds
Atoms
Molecules