Equal to
Less than
More than
None of these
B. Less than
Mild steel
Cast iron
Concrete
Bone of these
Drying and crushing the coal to a fine powder
Moulding the finely ground coal under pressure with or without a binding material
Heating the wood with a limited supply of air to temperature not less than 280°C
None of the above
Inversely proportional to two times
Directly proportional to
Inversely proportional to
None of these
The stress and strain induced is compressive
The stress and strain induced is tensile
Both A and B is correct
None of these
Steel
Copper
Aluminium
None of the above
Area at the time of fracture
Original cross-sectional area
Average of (A) and (B)
Minimum area after fracture
1 kg of water
7 kg of water
8 kg of water
9 kg of water
Thermal stresses
Tensile stress
Bending
No stress
Isothermal expansion
Isentropic expansion
Isothermal compression
Isentropic compression
Brown coal
Peat
Coking bituminous coal
Non-coking bituminous coal
Zero
Minimum
Maximum
Infinity
Carnot cycle
Bell-Coleman cycle
Rankine cycle
Stirling cycle
Increase
Decrease
Remain unchanged
Increase/decrease depending on application
l/δl
δl/l
l.δl
l + δl
Plasticity
Elasticity
Ductility
Malleability
Maximum shear stress
No shear stress
Minimum shear stress
None of the above
400 MPa
500 MPa
900 MPa
1400 MPa
Boyle's law
Charles' law
Gay-Lussac law
All of these
Breaking stress
Fracture stress
Yield point stress
Ultimate tensile stress
A Joule cycle consists of two constant volume and two isentropic processes.
An Otto cycle consists of two constant volume and two isentropic processes.
An Ericsson cycle consists of two constant pressure and two isothermal processes.
All of the above
Sum of two specific heats
Difference of two specific heats
Product of two specific heats
Ratio of two specific heats
Elastic point of the material
Plastic point of the material
Breaking point of the material
Yielding point of the material
Partial combustion of coal, coke, anthracite coal or charcoal in a mixed air steam blast
Carbonisation of bituminous coal
Passing steam over incandescent coke
Passing air and a large amount of steam over waste coal at about 650°C
1 - rγ - 1
1 + rγ - 1
1 - (1/ rγ - 1)
1 + (1/ rγ - 1)
Two constant volume and two isentropic processes
Two constant pressure and two isentropic processes
Two constant volume and two isothermal processes
One constant pressure, one constant volume and two isentropic processes
Same
Half
Two times
Four times
Pitch
Back pitch
Diagonal pitch
Diametric pitch
Ideal materials
Uniform materials
Isotropic materials
Piratical materials
The increase in entropy is obtained from a given quantity of heat at a low temperature.
The change in entropy may be regarded as a measure of the rate of the availability or unavailability of heat for transformation into work.
The entropy represents the maximum amount of work obtainable per degree drop in temperature.
All of the above
L = l/2
L = l/√2
L = l
L = 2l