Straight line
Parabolic curve
Triangle
Rectangle
A. Straight line
ω (r₁ r₂) sinθ
ω (r₁ + r₂) sinθ sec2θ
ω (r₁ r₂) cosθ
ω (r₁ + r₂) cosθ cosec2θ
(1/2). μ W cosec α (r₁ + r₂)
(2/3).μ W cosec α (r₁ + r₂)
(1/2). μ W cosec α [(r₁³ - r₂³)/(r₁² - r₂²)]
(2/3). μ W cosec α [(r₁³ - r₂³)/(r₁² - r₂²)]
Be zero
Act in upward direction
Act in downward direction
None of these
Incompletely constrained motion
Partially constrained motion
Completely constrained motion
Successfully constrained motion
(S₁ + S₂)/h
(S₁ - S₂)/h
(S₁ + S₂)/2h
(S₁ - S₂)/2h
Radial component only
Tangential component only
Coriolis component only
Radial and tangential components both
Will remain same
Will change
Could change or remain unaltered depending on which link is fixed
Will not occur
Simple gear train
Compound gear train
Reverted gear train
Epicyclic gear train
Decreases linearly with time
Increases linearly with time
Decreases exponentially with time
Increases exponentially with time
Increases as the radius of rotation decreases
Increases as the radius of rotation increases
Decreases as the radius of rotation increases
Remain constant for all radii of rotation
Number of cycles per hour
Number of cycles per minute
Number of cycles per second
None of these
Sliding pair
Rolling pair
Lower pair
Higher pair
Weak material of the belt
Weak material of the pulley
Uneven extensions and contractions of the belt when it passes from tight side to slack side
Expansion of the belt
2
3
4
5
15
28
30
8
Self-closed
Force-closed
Friction closed
None of these
9/8
9/82
9/16
9/128
Rack and pinion
Worm and wheel
Spiral gears
None of the above
Radial component
Tangential component
Coriolis component
None of these
No node
One node
Two nodes
Three nodes
(Length of the path of approach)/(Circular pitch)
(Length of path of recess)/(Circular pitch)
(Length of the arc of contact)/(Circular pitch)
(Length of the arc of approach)/cosφ
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.
Screw pair
Spherical pair
Turning pair
Sliding pair
Changing of a higher pair to a lower pair
Turning its upside down
Obtained by fixing different links in a kinematic chain
Obtained by reversing the input and output motion
x₁/x₂
log(x₁/x₂)
loge(x₁/x₂)
log(x₁.x₂)
10°-15°
15°-25°
25°-30°
30°-40°
Base circle
Pitch circle
Prime circle
Pitch curve
One
Two
Four
Six
Is directly proportional to
Is inversely proportional to
Is equal to cos φ multiplied by
Does not depend upon
Single slider crank chain
Whitworth quick return motion mechanism
Crank and slotted lever quick return motion mechanism
All of the above