One right angled triangle
Two right angled triangles
One equilateral triangle
Two equilateral triangles
B. Two right angled triangles
There is no change in temperature
There is no change in enthalpy
There is no change in internal energy
All of these
pv = C
pv = m R T
pvn = C
pvγ = C
Petrol engine
Diesel engine
Reversible engine
Irreversible engine
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
Bearing stresses
Fatigue stresses
Crushing stresses
Resultant stresses
Same
More
Less
Unpredictable
The deformation of the bar per unit length in the direction of the force is called linear strain.
The Poisson's ratio is the ratio of lateral strain to the linear strain.
The ratio of change in volume to the original volume is called volumetric strain.
The bulk modulus is the ratio of linear stress to the linear strain.
Long
Medium
Short
None of these
50 %
25 %
0 %
15 %
Fixed at both ends
Fixed at one end and free at the other end
Supported on more than two supports
Extending beyond the supports
Malleability
Ductility
Plasticity
Elasticity
√(KT/m)
√(2KT/m)
√(3KT/m)
√(5KT/m)
Strains
Stress and strain
Shear stress and shear strain
Moduli and elasticity
65° to 220°C
220° to 345°C
345° to 470°C
470° to 550°C
(11/3) CO2 + (3/7) CO
(3/7) CO2 + (11/3) CO
(7/3) CO2 + (3/11) CO
(3/11) CO2 + (7/3) CO
Two constant volume and two isentropic processes
Two isothermal and two isentropic processes
Two constant pressure and two isentropic processes
One constant volume, one constant pressure and two isentropic processes
Zero
1/5
4/5
1
p v = constant, if T is kept constant
v/T = constant, if p is kept constant
p/T = constant, if v is kept constant
T/p = constant, if v is kept constant
Total internal energy of a system during a process remains constant
Total energy of a system remains constant
Workdone by a system is equal to the heat transferred by the system
Internal energy, enthalpy and entropy during a process remain constant
Smaller end
Larger end
Middle
Anywhere
From maximum at the centre to zero at the circumference
From zero at the centre to maximum at the circumference
From maximum at the centre to minimum at the circumference
From minimum at the centre to maximum at the circumference
Breaking stress
Fracture stress
Yield point stress
Ultimate tensile stress
Combustion is at constant volume
Expansion and compression are isentropic
Maximum temperature is higher
Heat rejection is lower
Heat transfer is constant
Work transfer is constant
Mass flow at inlet and outlet is same
All of these
Half
Same amount
Double
One-fourth
Increase in availability of energy
Increase in temperature
Decrease in pressure
Degradation of energy
δQ = T.ds
δQ = T/ds
dQ = ds/T
None of these
0.01 to 0.1
0.23 to 0.27
0.25 to 0.33
0.4 to 0.6
Zeroth law of thermodynamics
First law of thermodynamics
Second law of thermodynamics
Kinetic theory of gases
Isothermal
Isentropic
Polytropic
None of these