Otto cycle
Ericsson cycle
Joule cycle
Stirling cycle
C. Joule cycle
T.ω watts
2π. T.ω watts
2π. T.ω/75 watts
2π. T.ω/4500 watts
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
300° to 500°C
500° to 700°C
700° to 900°C
900° to 1100°C
πd²/4
πd²/16
πd3/16
πd3/32
Zero
1/5
4/5
1
Isothermal
Isentropic
Polytropic
None of these
Carnot
Stirling
Ericsson
None of the above
Oxygen
Sulphur
Nitrogen
Carbon
Maximum shear stress
No shear stress
Minimum shear stress
None of the above
Fluids in motion
Breaking point
Plastic deformation of solids
Rupture stress
Th > Ts
Th < Ts
Th = Ts
None of these
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
A Joule cycle consists of two constant volume and two isentropic processes.
An Otto cycle consists of two constant volume and two isentropic processes.
An Ericsson cycle consists of two constant pressure and two isothermal processes.
All of the above
Greater than
Less than
Equal to
None of these
The material A is more ductile than material B
The material B is more ductile than material A
The ductility of material A and B is equal
The material A is brittle and material B is ductile
Butt joint
Lap joint
Double riveted lap joints
All types of joints
Area of cross-section of the column
Length and least radius of gyration of the column
Modulus of elasticity for the material of the column
All of the above
(11/3) CO2 + (3/7) CO
(3/7) CO2 + (11/3) CO
(7/3) CO2 + (3/11) CO
(3/11) CO2 + (7/3) CO
Boyle
Charles
Joule
None of these
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
(Net work output)/(Workdone by the turbine)
(Net work output)/(Heat supplied)
(Actual temperature drop)/(Isentropic temperature drop)
(Isentropic increase in temperature)/(Actual increase in temperature)
Isothermal expansion
Isentropic expansion
Isothermal compression
Isentropic compression
Tensile strain increases more quickly
Tensile strain decreases more quickly
Tensile strain increases in proportion to the stress
Tensile strain decreases in proportion to the stress
l/δl
δl/l
l.δl
l + δl
-140 kJ
-80 kJ
-40 kJ
+60 kJ
Energy stored in a body when strained within elastic limits
Energy stored in a body when strained up to the breaking of the specimen maximum strain
Energy which can be stored in a body
None of the above
1
0
-1
10
Tension
Compression
Bearing
Any one of the above
Shear force changes sign
Shear force is maximum
Bending moment changes sign
Bending moment is maximum
Zero
Minimum
Maximum
Infinity