Varies in magnitude but constant in direction
Varies in direction but constant in magnitude
Varies in magnitude and direction both
Constant in magnitude and direction both
B. Varies in direction but constant in magnitude
Mass and stiffness
Mass and damping coefficient
Mass and natural frequency
Damping coefficient and natural frequency
Of relative velocity vector for the two coincident points rotated by 90° in the direction of the angular velocity of the rotation of the link
Along the centripetal acceleration
Along tangential acceleration
Along perpendicular to angular velocity
Parallel to OA
Perpendicular to OA
At 45° to OA
Along AO
Upward
Downward
Forward
Backward
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
T/3
(T.g)/3
√(T/3m)
√(3m/T)
Simple gear train
Compound gear train
Reverted gear train
None of the above
To move the ship towards starboard
To move the ship towards port side
To raise the bow and lower the stern
To raise the stern and lower the bow
Parallel
Perpendicular
Both A and B
None of these
The algebraic sum of the secondary forces must be equal to zero
The algebraic sum of the couples about any point in the plane of the secondary forces must be equal to zero
Both (A) and (B)
None of these
Increases power transmitted
Decreases power transmitted
Have no effect on power transmitted
Increases power transmitted upto a certain speed and then decreases
Turning pairs
Sliding pairs
Spherical pairs
Self-closed pairs
A single mass in different planes
Two masses in any two planes
A single mass in one of the planes of the revolving masses
Two equal masses in any two planes
Sum
Difference
Product
Ratio
Steering
Pitching
Rolling
All of the above
Tip of the gear tooth and flank of pinion
Tip of the pinion and flank of gear
Flanks of both gear and pinion
Tip of both gear and pinion
All points of the disc have the same velocity
The centre of the disc has zero acceleration
The centre of the disc has centrifugal acceleration
The point on the disc making contact with the plane surface has zero acceleration
The sum of the two masses is equal to the total mass of body
The centre of gravity of the two masses coincides with that of the body
The sum of mass moment of inertia of the masses about their centre of gravity is equal to the mass moment of inertia of the body
All of the above
Velocity
Displacement
Rate of change of velocity
All of the above
Addendum circle
Dedendum circle
Pitch circle
Clearance circle
No acceleration
Linear acceleration
Angular acceleration
Both angular and linear accelerations
Open pair
Closed pair
Sliding pair
Point contact pair
Pendulum type governor
Dead weight governor
Spring loaded governor
Inertia governor
l = 2p - 2
l = 2p - 3
l = 2p - 4
l = 2p - 5
Leads by 90°
Lags by 90°
Leads by 180°
Are in phase
Worm and worm wheel
Spur gears
Bevel gears
Hooke's joint
Greater than
Less than
Equal to
None of these
Remain same as before
Become equal to 2R
Become equal to R/2
Become equal to R/4
Higher pair
Lower pair
Rolling pair
Sliding pair
Closed pair
Open pair
Mechanical pair
Rolling pair