Pressure
Volume
Temperature
Density
B. Volume
Increasing the internal energy of gas
Doing some external work
Increasing the internal energy of gas and also for doing some external work
None of the above
Zero
wl/4
wl/2
wl²/2
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
11/7
9/7
4/7
All of the above
It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work.
It is impossible to transfer heat from a body at a lower temperature to a higher temperature, without the aid of an external source.
There is a definite amount of mechanical energy, which can be obtained from a given quantity of heat energy.
All of the above
Pressure exerted by the gas
Volume occupied by the gas
Temperature of the gas
All of these
e (1 - 2m)
e (1 - 2/m)
e (m - 2)
e (2/m - 1)
πd²/4
πd²/16
πd3/16
πd3/32
Of same magnitude as that of bar and applied at the lower end
Half the weight of bar applied at lower end
Half of the square of weight of bar applied at lower end
One fourth of weight of bar applied at lower end
Extensive heat is transferred
Extensive work is done
Extensive energy is utilised
None of these
Greater than
Less than
Equal to
None of these
τ²/ 2G × Volume of shaft
τ/ 2G × Volume of shaft
τ²/ 4G × Volume of shaft
τ/ 4G × Volume of shaft
50 %
25 %
0 %
15 %
Short column
Long column
Weak column
Medium column
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
Ends are firmly fixed
Column is supported on all sides throughout the length
Length is equal to radius of gyration
Length is twice the radius of gyration
Oxygen
Nitrogen
Hydrogen
Methane
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
One right angled triangle
Two right angled triangles
One equilateral triangle
Two equilateral triangles
Same torque
Less torque
More torque
Unpredictable
Heat and work crosses the boundary of the system, but the mass of the working substance does not crosses the boundary of the system
Mass of the working substance crosses the boundary of the system but the heat and work does not crosses the boundary of the system
Both the heat and work as well as mass of the working substance crosses the boundary of the system
Neither the heat and work nor the mass of the working substance crosses the boundary of the system
W1 - 2 = 0
Q1 - 2 = 0
dU = 0
All of these
Equal to
Less than
Greater than
None of these
Linear stress to lateral strain
Lateral strain to linear strain
Linear stress to linear strain
Shear stress to shear strain
Wood charcoal
Bituminous coke
Pulverised coal
Coke
Greater than
Less than
Equal to
None of these
Element
Compound
Atom
Molecule
-273°C
73°C
237°C
-237°C
Isothermally
Isentropically
Polytropically
None of these
t
2t
4t
8t