The stress and strain induced is compressive
The stress and strain induced is tensile
Both A and B is correct
None of these
A. The stress and strain induced is compressive
Equal to
Less than
Greater than
None of these
Plasticity
Ductility
Elasticity
Malleability
Kelvin
Joule
Clausis
Gay-Lussac
Temperature limits
Pressure ratio
Volume compression ratio
Cut-off ratio and compression ratio
Short columns
Long columns
Weak columns
Medium columns
Creeping
Yielding
Breaking
Plasticity
Chain riveted joint
Diamond riveted joint
Crisscross riveted joint
Zigzag riveted joint
d/4
d/8
d/12
d/16
Element
Compound
Atom
Molecule
1
1.4
1.67
1.87
First kind
Second kind
Third kind
None of these
τ²/ 2G × Volume of shaft
τ/ 2G × Volume of shaft
τ²/ 4G × Volume of shaft
τ/ 4G × Volume of shaft
Joint less section
Homogeneous section
Perfect section
Seamless section
Tensile stress
Compressive stress
Shear stress
Thermal stress
3 to 6
5 to 8
15 to 20
20 to 30
The stress and strain induced is compressive
The stress and strain induced is tensile
Both A and B is correct
None of these
Short columns
Long columns
Both short and long columns
Weak columns
There is no change in temperature
There is no change in enthalpy
There is no change in internal energy
All of these
δl = 4PE/ πl²
δl = 4πld²/PE
δl = 4Pl/πEd₁d₂
δl = 4PlE/ πd₁d₂
The indirect heat exchanger and cooler is avoided
Direct combustion system is used
A condenser is used
All of the above
l/8
l/4
l/2
l
Same
Twice
Four times
Eight times
Gauge pressure = Absolute pressure + Atmospheric pressure
Absolute pressure = Gauge pressure + Atmospheric pressure
Absolute pressure = Gauge pressure - Atmospheric pressure
Atmospheric pressure = Absolute pressure + Gauge pressure
Proportional limit, elastic limit, yielding, failure
Elastic limit, proportional limit, yielding, failure
Yielding, proportional limit, elastic limit, failure
None of the above
(p - 2d) t × σc
(p - d) t × τ
(p - d) t × σt
(2p - d) t × σt
π /4 × τ × D³
π /16 × τ × D³
π /32 × τ × D³
π /64 × τ × D³
Calorific value
Heat energy
Lower calorific value
Higher calorific value
Longitudinal stress to longitudinal strain
Volumetric stress to volumetric strain
Lateral stress to Lateral strain
Shear stress to shear strain
Carnot cycle
Stirling cycle
Ericsson cycle
Joule cycle
Gas engine
Petrol engine
Steam engine
Reversible engine