A rigid link rotates instantaneously relative to another link at the instantaneous centre for the configuration of the mechanism considered.
The two rigid links have no linear velocity relative to each other at the instantaneous centre.
The velocity of the instantaneous centre relative to any third rigid link is same whether the instantaneous centre is regarded as a point on the first rigid link or on the second rigid link.
All of the above
D. All of the above
Equal to
Less than
Greater than
None of these
(l₁ + l₂ + l₃)/3
l = l₁ + l₂.(d₁/d₂)³ + l₂.(d₁/d₃)³
l = l₁ + l₂.(d₁/d₂)⁴ + l₃.(d₁/d₃)⁴
l₁ + l₂ + l₃
Base circle
Pitch circle
Prime circle
Outer circle
The former is mathematically accurate
The former is having turning pair
The former is most economical
The former is most rigid
Higher pair
Lower pair
Rolling pair
Sliding pair
Turning pair
Rolling pair
Screw pair
Spherical pair
Structure
Machine
Inversion
Compound mechanism
Pitch circle
Base circle
Prime circle
Outer circle
Stable
Unstable
Isochronous
None of these
Balanced completely
Balanced partially
Balanced by secondary forces
Not balanced
The mass of two are same
C.G. of two coincides
M.I. of two about an axis through e.g. is equal
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
Angle of friction
Angle of repose
Angle of projection
None of these
0°
90°
180°
270°
Length of pair of contact to the circular pitch
Length of arc of contact to the circular pitch
Length of arc of approach to the circular pitch
Length of arc of recess to the circular pitch
One-half
Two-third
Three-fourth
Whole
Beam engine
Rotary engine
Oldhams coupling
Elliptical trammel
Equal to
Less than
Greater than
None of these
Flexible coupling
Universal coupling
Chain coupling
Oldham's coupling
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.
Along PO
Perpendicular to PO
At 45° to PO
None of the above
Incompletely constrained motion
Partially constrained motion
Completely constrained motion
Successfully constrained motion
l = (1/2).(j + 2)
l = (2/3).(j + 2)
l = (3/4).(j + 3)
l = j + 4
[c²/(1 + 2c)] (m + M) g.h
[2c²/(1 + 2c)] (m + M) g.h
[3c²/(1 + 2c)] (m + M) g.h
[4c²/(1 + 2c)] (m + M) g.h
Shoe brake
Band brake
Band and block brake
Internal expanding brake
Equal to 1
Equal to 2
Less than 2
Greater than 2
Increases as the radius of rotation decreases
Increases as the radius of rotation increases
Decreases as the radius of rotation increases
Remains constant for all radii of rotation
Open pair
Closed pair
Sliding pair
Point contact pair
The reaction on me inner wheels increases and on the outer wheels decreases
The reaction on the outer wheels increases and on the inner wheels decreases
The reaction on the front wheels increases and on the rear wheels decreases
The reaction on the rear wheels increases and on the front wheels decreases
The broken belt only
All the belts
The broken belt and the belts on either side of it
None of the above