Simple train of wheels
Compound train of wheels
Reverted gear train
Epicyclic gear train
C. Reverted gear train
45° in the direction of rotation of the link containing the path
45° in the direction opposite to the rotation of the link containing the path
90° in the direction of rotation of the link containing the path
180° in the direction opposite to the rotation of the link containing the path
Small
Too small
Large
Too large
During which the follower returns to its initial position
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 highest position
Moved by the cam from the instant the follower begins to rise, till it reaches its highest position
The centre of the disc
The point of contact
An infinite distance on the plane surface
The point on the circumference situated vertically opposite to the contact point
Dependent on the size of teeth
Dependent on the size of gears
Always constant
Always variable
l - 2
l - 1
l
l + 1
Vector sum of radial component and coriolis component
Vector sum of tangential component and coriolis component
Vector sum of radial component and tangential component
Vector difference of radial component and tangential component
During which the follower returns to its initial position
Of rotation of the cam for 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
All four pairs are turning
Three pairs turning and one pair sliding
Two pairs turning and two pairs sliding
One pair turning and three pairs sliding
Parallel to AB
Perpendicular to AB
Along AB
At 45° to AB
The periodic time of a particle moving with simple harmonic motion is the time taken by a particle for one complete oscillation.
The periodic time of a particle moving with simple harmonic motion is directly proportional to its angular velocity.
The velocity of a particle moving with simple harmonic motion is zero at the mean position.
The acceleration of the particle moving with simple harmonic motion is maximum at the mean position.
Mass
Stiffness
Mass and stiffness
Stiffness and eccentricity
Pitch circle
Base circle
Pitch curve
Prime circle
Radial component only
Tangential component only
Coriolis component only
Radial and tangential components both
Uniform velocity
Simple harmonic motion
Uniform acceleration and retardation
Cycloidal motion
Steering
Pitching
Rolling
All of the above
Belt, rope and chain drives
Gears, cams
Ball and roller bearings
All of the above
Flat pivot bearing
Flat collar bearing
Conical pivot bearing
Truncated conical pivot bearing
Structure
Mechanism
Kinematic chain
Inversion
Fluctuation of speed
Maximum fluctuation of speed
Coefficient of fluctuation of speed
None of these
Number of cycles per hour
Number of cycles per minute
Number of cycles per second
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
Screw pair
Spherical pair
Turning pair
Sliding pair
Deep groove ball bearing
Double row self aligning ball bearing
Double row spherical roller bearing
Cylindrical roller bearing
(1/2) μ W R cosecα
(2/3) μ W R cosecα
(3/4) μ W R cosecα
μ W R cosecα
No acceleration
Linear acceleration
Angular acceleration
Both angular and linear accelerations
Base circle
Pitch circle
Prime circle
Outer circle
Is in phase
Leads by 90°
Leads by 180°
Lags by 90°
Slider crank mechanism
Four bar chain mechanism
Quick return motion mechanism
All of these
Turning pair
Rolling pair
Sliding pair
Spherical pair