Kelvin
Joule
Clausis
Gay-Lussac
C. Clausis
(23/100) × Mass of excess carbon
(23/100) × Mass of excess oxygen
(100/23) × Mass of excess carbon
(100/23) × Mass of excess oxygen
cv/ cp =R
cp - cv = R
cv = R/ γ-1
Both (B) and (C)
Equal to
Directly proportional to
Inversely proportional to
Independent of
Reversible
Irreversible
Reversible or irreversible
None of these
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
Carnot cycle
Stirling cycle
Otto cycle
None of these
The stress is the pressure per unit area
The strain is expressed in mm
Hook's law holds good upto the breaking point
Stress is directly proportional to strain within elastic limit
Boyle's law
Charles' law
Gay-Lussac law
Avogadro's law
Change
Do not change
Both (A) and (B)
None of these
δl = 4PE/ πl²
δl = 4πld²/PE
δl = 4Pl/πEd₁d₂
δl = 4PlE/ πd₁d₂
Temperature limits
Pressure ratio
Compression ratio
Cut-off ratio and compression ratio
It is impossible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is possible to construct an engine working on a cyclic process, whose sole purpose is to convert heat energy into work
It is impossible to construct a device which operates in a cyclic process and produces no effect other than the transfer of heat from a cold body to a hot body
None of the above
p.t.σt
d.t.σc
π/4 × d² × σt
π/4 × d² × σc
(p1 v1 - p2 v2)/(γ - 1)
[m R (T1 - T2)] /(γ - 1)
[m R T1/(γ - 1)][1 - (p2 v2 /p1 v1)]
All of these
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
1.817
2512
4.187
None of these
More
Less
Equal
Depends on other factors
Boyle's law
Charle's law
Gay-Lussac law
Joule's law
Tensile stress
Compressive stress
Shear stress
Strain
Very low
Low
High
Very high
Carnot cycle
Bell-Coleman cycle
Rankine cycle
Stirling cycle
L = l/2
L = l/√2
L = l
L = 2l
9/7
11/7
7/4
1/4
Sum
Difference
Product
Ratio
-140 kJ
-80 kJ
-40 kJ
+60 kJ
Dual combustion cycle
Diesel cycle
Atkinson cycle
Rankine cycle
Breaking stress
Fracture stress
Yield point stress
Ultimate tensile stress
Decrease in cut-off
Increase in cut-off
Constant cut-off
None of these
Tensile in both the material
Tensile in steel and compressive in copper
Compressive in steel and tensile in copper
Compressive in both the materials
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