Loss of heat
No loss of heat
Gain of heat
No gain of heat
A. Loss of heat
Before point A
Beyond point A
Between points A and D
Between points D and E
Fixed at both ends
Fixed at one end and free at the other end
Supported at its ends
Supported on more than two supports
Very low
Low
High
Very high
Rankine
Stirling
Carnot
Brayton
Tensile stress
Compressive stress
Shear stress
Thermal stress
The stress and strain induced is compressive
The stress and strain induced is tensile
Both A and B is correct
None of these
Resilience
Proof resilience
Modulus of resilience
Toughness
Kh > Ks
Kh < Ks
Kh = Ks
None of these
Straight line formula
Eulers formula
Rankines formula
Secant formula
Carnot
Ericsson
Stirling
None of the above
Increases
Decreases
First increases and then decreases
First decreases and then increases
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
Fluids in motion
Breaking point
Plastic deformation of solids
Rupture stress
The first row
The second row
The central row
One rivet hole of the end row
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Permanent
Temporary
Semi-permanent
None of these
Zero
Minimum
Maximum
Infinity
Pulverised coal
Brown coal
Coking bituminous coal
Non-coking bituminous coal
Coke
Wood charcoal
Bituminous coal
Briquetted coal
0.287 J/kgK
2.87 J/kgK
28.7 J/kgK
287 J/kgK
Short column
Long column
Weak column
Medium column
1.817
2512
4.187
None of these
Equal to
Less than
More than
None of these
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
Cut-off is increased
Cut-off is decreased
Cut-off is zero
Cut-off is constant
Frequent heat treatment
Fatigue
Creep
Shock loading
δl = 4PE/ πl²
δl = 4πld²/PE
δl = 4Pl/πEd₁d₂
δl = 4PlE/ πd₁d₂
Increase
Decrease
Remain unchanged
Increase/decrease depending on application
Vapour
Perfect gas
Air
Steam
W1 - 2 = 0
Q1 - 2 = 0
dU = 0
All of these