Transverse vibrations
Torsional vibrations
Longitudinal vibrations
All of these
A. Transverse vibrations
Motion of a piston in the cylinder of a steam engine
Motion of a square bar in a square hole
Motion of a shaft with collars at each end in a circular hole
All of the above
Ball and socket joint
Journal bearing
Lead screw and nut
Cam and follower
In increasing velocity ratio
In decreasing the slip of the belt
For automatic adjustment of belt position so that belt runs centrally
Increase belt and pulley life
ω². (r₁ r₂). (1 - cos² θ)
ω². (r₁ + r₂). (1 + cos² θ)
ω². (r₁ + r₂). [(2 - cos² θ)/cos³ θ]
ω². (r₁ - r₂). (1 - sin² θ)
Flat pivot bearing
Flat collar bearing
Conical pivot bearing
Truncated conical pivot bearing
ω
ωr
ω²r
ω/r
Flexible coupling
Universal coupling
Chain coupling
Oldham's coupling
Shaft revolving in a bearing
Straight line motion mechanisms
Automobile steering gear
All of the above
4, 4
4, 5
5, 4
4, 6
Diameter of disc
Span of shaft
Eccentricity
All of these
Radial component only
Tangential component only
Coriolis component only
Radial and tangential components both
Piston and cylinder of a reciprocating steam engine
Shaft with collars at both ends fitted into a circular hole
Lead screw of a lathe with nut
Ball and a socket joint
2
4
3
None of the above
Increases
Decreases
Remain unaffected
First increases and then decreases
θ/2
θ
2θ
4θ
Because of difficulty in manufacturing cam profile
Because of loose contact of follower with cam surface
In order to have acceleration in beginning and retardation at the end of stroke within the finite limits
Because the uniform velocity motion is a partial parabolic motion
Small
Too small
Large
Too large
The interference is inherently absent.
The variation in centre distance of shafts increases radial force.
A convex flank is always in contact with concave flank.
The pressure angle is constant throughout the teeth engagement.
Turning pair
Rolling pair
Screw pair
Spherical pair
l - 2
l - 1
l
l + 1
Incompletely constrained motion
Partially constrained motion
Completely constrained motion
Successfully constrained motion
A single plane
Two planes
Three planes
Four planes
Depends upon
Is independent of
Either A or B
None of these
Angle of friction
Angle of repose
Angle of projection
None of these
Directly proportional to speed
Directly proportional to (speed)²
Inversely proportional to speed
Inversely proportional to (speed)²
Greater than
Less than
Equal to
None of these
At the instantaneous center of rotation, one rigid link rotates instantaneously relative to another for the configuration of mechanism considered
The two rigid links have no linear velocities relative to each other at the instantaneous centre
The two rigid links which have no linear velocity relative to each other at this center have the same linear velocity to the third rigid link
The double centre can be denoted either by O2 or O12, but proper selection should be made
Base circle
Pitch circle
Root circle
Prime circle
Shear stress
Bending stress
Tensile stress
Compressive stress
Of rotation of the cam for a definite displacement of the follower
Through which the cam rotates during the period in which the follower remains in the highest position
Moved by the cam from the instant the follower begins to rise, till it reaches its highest position
Moved by the cam from beginning of ascent to the termination of descent