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Theory of Machine

Theory of Machine
V-belts are usually used for

Long drives
Long and short drives
Short drives
None of these

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Theory of Machine
A body of weight W is required to move up the rough inclined plane whose angle of inclination with the horizontal is α. The effort applied parallel to the plane is given by (where μ = tan φ = Coefficient of friction between the plane and the body)

P = W (cos α + μ sin α)
P = W tan (α + φ)
P = W tan α
P = W (sin α + μ cos α)

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Theory of Machine
The type of coupling used to join two shafts whose axes are neither in same straight line nor parallel, but intersect is

Chain coupling
Flexible coupling
Universal coupling
Oldham's coupling

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Theory of Machine
A disc is a spinning with an angular velocity ω rad/s about the axis of spin. The couple applied to the disc causing precession will be (where I = Mass moment of inertia of the disc, and ωP = Angular velocity of precession of the axis of spin)

Iω²
(1/2).Iω²
I ω ωP
(1/2). I ω ωP

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Theory of Machine
When one of the links of a kinematic chain is fixed, the chain is known as a

Structure
Machine
Mechanism
Inversion

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Theory of Machine
When two links are connected by a pin joint, their instantaneous center lies

At the pin joint
At the center of curvature
On their point of contact
At the center of circle

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