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Theory of Machine

Theory of Machine
Carnot cycle is

a quasi static cycle
a semi-reversible cycle
an irreversible cycle
a reversible cycle

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Theory of Machine
Klein's construction can be used to determine acceleration of various parts when the crank is at

Inner dead centre
All of the listed here
Outer dead centre
Right angles to the link of the stroke

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Theory of Machine
The example of higher pair is

Ball and roller bearings
All of these
Gears, cams
Belt, rope and chain drives

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Theory of Machine
In a screw jack, the effort required to lower the load W is given by

P = W tan(α + φ)
P = W tan(φ - α)
P = W tan(α - φ)
P = W cos(α + φ)

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Theory of Machine
The periodic time is given by (where ω = Angular velocity of the particle in rad/s)

ω × 2π
ω/2π
2π/ω
π/ω

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Theory of Machine
A torsional system with discs of moment of inertia I₁ and I₂ as shown in the below figure, is gear driven such that the ratio of speed of shaft B to shaft A is 'G'. Neglecting the inertia of gears, the equivalent inertia of disc on shaft B at the speed of shaft A is equal to

I₂/G²
G.I₂
G².I₂
I₂/G

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MORE MCQ ON Theory of Machine

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