The broken belt only
All the belts
The broken belt and the belts on either side of it
None of the above
B. All the belts
On their point of contact
At the centre of curvature
At the centre of circle
At the pin joint
Mean speed to the maximum equilibrium speed
Mean speed to the minimum equilibrium speed
Difference of the maximum and minimum equilibrium speeds to the mean speed
Sum of the maximum and minimum equilibrium speeds to the mean speed
Angle of friction
Angle of repose
Angle of projection
None of these
Perpendicular to sliding surfaces
Along sliding surfaces
Somewhere in between above two
None of the above
Parallel to the link joining the points
Perpendicular to the link joining the points
At 45° to the link joining the points
None of the above
The control of speed fluctuations
Balancing of forces and couples
Kinematic analysis
Vibration analysis
Leads by 90°
Lags by 90°
Leads by 180°
Are in phase
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)
Broken belt
Broken belt and its adjacent belts
All the belts
There is no need of changing any one as remaining belts can take care of transmission of load
Over damped
Under damped
Critically damped
Without vibrations
Free vibration
Forced vibration
Damped vibration
Under damped vibration
T₁/T₂ = μ. θ. n
T₁/T₂ = [(1 - μ tanθ)/(1 + μ tanθ)]n
T₁/T₂ = (μ θ)n
T₁/T₂ = [(1 + μ tanθ)/(1 - μ tanθ)]n
Vertically and parallel
Vertically and perpendicular
Horizontally and parallel
Horizontally and perpendicular
Two links should be fixed
One link should be fixed
None of the links should be fixed
There is no such criterion
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
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.
Decreases linearly with time
Increases linearly with time
Decreases exponentially with time
Increases exponentially with time
Same
Opposite
Perpendicular
None of these
ωv
2ωv
ω²v
2ωv²
Equal to 1
Less than 2
Equal to 2
Greater than 2
Smaller
Larger
Either A or B
None of these
The algebraic sum of the primary forces must be equal to zero
The algebraic sum of the couples about any point in the plane of the primary forces must be equal to zero
Both (A) and (B)
None of these
P = 2L - 4
P = 2L + 4
P = 2L + 2
P = 2L - 2
Sliding pair
Rolling pair
Lower pair
Higher pair
5,367 r.p.m.
6,000 r.p.m.
9,360 r.p.m.
12,000 r.p.m.
Eight links
Six links
Four links
Twelve links
2ECS
ECS/2
2ECS²
2E²CS
Zero
Less than one
Greater than one
Infinity
Radius of rotation of balls increases as the equilibrium speed decreases
Radius of rotation of balls decreases as the equilibrium speed decreases
Radius of rotation of balls increases as the equilibrium speed increases
Radius of rotation of balls decreases as the equilibrium speed increases
Two times
Four times
Eight times
Sixteen times