When coal is first dried and then crushed to a fine powder by pulverising machine
From the finely ground coal by moulding under pressure with or without a binding material
When coal is strongly heated continuously for 42 to 48 hours in the absence of air in a closed vessel
By heating wood with a limited supply of air to a temperature not less than 280°C
C. When coal is strongly heated continuously for 42 to 48 hours in the absence of air in a closed vessel
1 N-m/s
100 N-m
1000 N-m/s
1 × 106 N-m/s
2/3
3/4
1
9/8
Change the shape of the beam
Effect the saving in material
Equalise the strength in tension and compression
Increase the cross-section of the beam
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
Bending moment (i.e. M)
Bending moment² (i.e. M²)
Bending moment³ (i.e. M³)
Bending moment⁴ (i.e. M⁴)
kJ
kJ/kg
kJ/m2
kJ/m3
E = 3K.C/(3K + C)
E = 6K.C/(3K + C)
E = 9K.C/(3K + C)
E = 12K.C/(3K + C)
OC
OP
OQ
PQ
Carnot cycle can't work with saturated steam
Heat is supplied to water at temperature below the maximum temperature of the cycle
A Rankine cycle receives heat at two places
Rankine cycle is hypothetical
d/4
d/8
d/12
d/16
Equal to
Less than
Greater than
None of these
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Zero
Minimum
Maximum
Infinity
(σx + σy)/2 + (1/2) × √[(σx - σy)² + 4 τ²xy]
(σx + σy)/2 - (1/2) × √[(σx - σy)² + 4 τ²xy]
(σx - σy)/2 + (1/2) × √[(σx + σy)² + 4 τ²xy]
(σx - σy)/2 - (1/2) × √[(σx + σy)² + 4 τ²xy]
Malleability
Ductility
Plasticity
Elasticity
t
2t
4t
8t
Boyle's law
Charles' law
Gay-Lussac law
All of these
Same
More
Less
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
Mono-atomic
Di-atomic
Tri-atomic
Poly-atomic
Flow processes
Non-flow processes
Adiabatic processes
None of these
Less than
Equal to
More than
None of these
Thermodynamic law
Thermodynamic process
Thermodynamic cycle
None of these
Reversible process
Irreversible process
Reversible or irreversible process
None of these
12
14
16
32
(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)
(11/3) CO2 + (3/7) CO
(3/7) CO2 + (11/3) CO
(7/3) CO2 + (3/11) CO
(3/11) CO2 + (7/3) CO
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
10 MPa
30 MPa
50 MPa
100 MPa
External energy
Internal energy
Kinetic energy
Molecular energy