Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
Kinetic theory of gases
B. First law of thermodynamics
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
Thermodynamic law
Thermodynamic process
Thermodynamic cycle
None of these
Short columns
Long columns
Weak columns
Medium columns
π /4 × τ × D³
π /16 × τ × D³
π /32 × τ × D³
π /64 × τ × D³
Homogeneous
Inelastic
Isotropic
Isentropic
Carbon and hydrogen
Oxygen and hydrogen
Sulphur and oxygen
Sulphur and hydrogen
Two constant volume and two isentropic processes
Two isothermal and two isentropic processes
Two constant pressure and two isentropic processes
One constant volume, one constant pressure and two isentropic processes
Kelvin
Joule
Clausis
Gay-Lussac
0°
30°
45°
90°
Atomisation
Carbonisation
Combustion
None of these
No stress
Shear stress
Tensile stress
Compressive stress
1.333 N/m2
13.33 N/m2
133.3 N/m2
1333 N/m2
Wl3 / 48EI
5Wl3 / 384EI
Wl3 / 392EI
Wl3 / 384EI
Change in volume to original volume
Change in length to original length
Change in cross-sectional area to original cross-sectional area
Any one of the above
Linear stress to linear strain
Linear stress to lateral strain
Volumetric strain to linear strain
Shear stress to shear strain
Cracking
Carbonisation
Fractional distillation
Full distillation
0
1
γ
∝
Short column
Long column
Weak column
Medium column
Pressure
Volume
Temperature
Density
Inversely proportional to strain
Directly proportional to strain
Square root of strain
Equal to strain
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
Load/original cross-sectional area and change in length/original length
Load/ instantaneous cross-sectional area and loge (original area/ instantaneous area)
Load/ instantaneous cross-sectional area and change in length/ original length
Load/ instantaneous area and instantaneous area/original area
Equal to
More than
Less than
None of these
Proportional limit, elastic limit, yielding, failure
Elastic limit, proportional limit, yielding, failure
Yielding, proportional limit, elastic limit, failure
None of the above
Becomes constant
Starts decreasing
Increases without any increase in load
None of the above
Heat transfer is constant
Work transfer is constant
Mass flow at inlet and outlet is same
All of these
WD3n/Cd⁴
2WD3n/Cd⁴
4WD3n/Cd⁴
8WD3n/Cd⁴
Yield point stress
Breaking stress
Ultimate stress
Elastic limit
Middle of bar
Supported end
Bottom end
None of these
(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)