Slenderness ratio and area of cross-section
Poisson's ratio and modulus of elasticity
Slenderness ratio and modulus of elasticity
Slenderness ratio, area of cross-section and modulus of elasticity
D. Slenderness ratio, area of cross-section and modulus of elasticity
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
Boyle
Charles
Joule
None of these
Same
More
Less
Unpredictable
3/7
7/3
11/3
3/11
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
Same
Double
Half
Four times
0.5 s.l.σt
s.l.σt
√2 s.l.σt
2.s.l.σt
Tensile stress
Compressive stress
Shear stress
Strain
1.333 N/m2
13.33 N/m2
133.3 N/m2
1333 N/m2
Same torque
Less torque
More torque
Unpredictable
Doubled
Halved
Becomes four times
None of the above
Cracking
Carbonisation
Fractional distillation
Full distillation
1 × 102 N/m2
1 × 103 N/m2
1 × 104 N/m2
1 × 105 N/m2
The axis of load
An oblique plane
At right angles to the axis of specimen
Would not occur
Dual cycle, Diesel cycle, Otto cycle
Otto cycle, Diesel cycle, Dual cycle
Dual cycle, Otto cycle, Diesel cycle
Diesel cycle, Otto cycle, Dual cycle
wl/6
wl/3
wl
2wl/3
Isothermal expansion
Isentropic expansion
Isothermal compression
Isentropic compression
1
0
-1
10
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
Kinetic theory of gases
d/4
d/8
d/12
d/16
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
None of these
Carbon and hydrogen
Oxygen and hydrogen
Sulphur and oxygen
Sulphur and hydrogen
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
Area at the time of fracture
Original cross-sectional area
Average of (A) and (B)
Minimum area after fracture
Fixed at both ends
Fixed at one end and free at the other end
Supported on more than two supports
Extending beyond the supports
In tension
In compression
Neither in tension nor in compression
None 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
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Increases the internal energy of the gas
Increases the temperature of the gas
Does some external work during expansion
Both (B) and (C)
Equal to
Less than
Greater than
None of these