0.287 J/kgK
2.87 J/kgK
28.7 J/kgK
287 J/kgK
D. 287 J/kgK
Ideal materials
Uniform materials
Isotropic materials
Piratical materials
The axis of load
An oblique plane
At right angles to the axis of specimen
Would not occur
pv = C
pv = m R T
pvn = C
pvγ = C
Peat
Lignite
Bituminous coal
Anthracite coal
Homogeneous
Inelastic
Isotropic
Isentropic
Proportional limit, elastic limit, yielding, failure
Elastic limit, proportional limit, yielding, failure
Yielding, proportional limit, elastic limit, failure
None of the above
3 to 6
5 to 8
10 to 20
15 to 30
Atomisation
Carbonisation
Combustion
None of these
Increase key length
Increase key depth
Increase key width
Double all the dimensions
l/δl
δl/l
l.δl
l + δl
Equal to
One-half
Twice
Four times
Butt joint
Lap joint
Double riveted lap joints
All types of joints
Sum of two principal stresses
Difference of two principal stresses
Half the sum of two principal stresses
Half the difference of two principal stresses
Malleability
Ductility
Plasticity
Elasticity
Increases
Decreases
First increases and then decreases
First decreases and then increases
A horizontal line
A vertical line
An inclined line
A parabolic curve
Mechanical and fluid friction
Unrestricted expansion
Heat transfer with a finite temperature difference
All of the above
It is possible to transfer heat from a body at a lower temperature to a body at a higher temperature.
It is impossible to transfer heat from a body at a lower temperature to a body at a higher temperature, without the aid of an external source.
It is possible to transfer heat from a body at a lower temperature to a body at a higher temperature by using refrigeration cycle.
None of the above
Kelvin
Joule
Clausis
Gay-Lussac
Low
Very low
High
Very high
Tensile in both the material
Tensile in steel and compressive in copper
Compressive in steel and tensile in copper
Compressive in both the materials
Same
More
Less
Unpredictable
Two isothermal and two isentropic
Two isentropic and two constant volumes
Two isentropic, one constant volume and one constant pressure
Two isentropic and two constant pressures
Wl3/48 EI
Wa²b²/3EIl
[Wa/(a√3) x EIl] x (l² - a²)3/2
5Wl3/384 EI
50 %
25 %
20 %
30 %
Inversely proportional to two times
Directly proportional to
Inversely proportional to
None of these
First kind
Second kind
Third kind
None of these
65° to 220°C
220° to 345°C
345° to 470°C
470° to 550°C
Extensive heat is transferred
Extensive work is done
Extensive energy is utilised
None of these
Pressure exerted by the gas
Volume occupied by the gas
Temperature of the gas
All of these