cosθ = sinα
sinθ = ± tanα
tanθ = ± cosα
cotθ = cosα
C. tanθ = ± cosα
Turning pair
Screw pair
Belt and pulley
None of the above
Longitudinal vibration
Torsional vibration
Transverse vibration
Damped free vibration
Deep groove ball bearing
Double row self aligning ball bearing
Double row spherical roller bearing
Cylindrical roller bearing
Stable
Unstable
Isochronous
Hunt
Enhance the load carrying capacity of the jack
Reduce the effort needed for lifting the working load
Reduce the value of frictional torque required to be countered for lifting the load
Prevent the rotation of load being lifted
Is in motion
Is at rest
Just begins to slide over the surface of the other body
None of the above
ω/2π
2π/ω
ω × 2π
π/ω
Kinematically sound
Not sound
Soundness would depend upon which link is kept fixed
Data is not sufficient to determine same
Structure
Mechanism
Inversion
Machine
Wear is less
Power absorbed is less
Both wear and power absorbed are low
The pressure developed being high provides tight sealing
(1/2) μ W R cosecα
(2/3) μ W R cosecα
(3/4) μ W R cosecα
μ W R cosecα
Velocity of various parts
Acceleration of various parts
Displacement of various parts
Angular acceleration of various parts
Greater than
Less than
Equal to
None of these
Four bar linkage
6 bar linkage
8 bar linkage
3 bar linkage
Mass
Stiffness
Mass and stiffness
Stiffness and eccentricity
Will remain same
Will change
Could change or remain unaltered depending on which link is fixed
Will not occur
10°-15°
15°-25°
25°-30°
30°-40°
Toothed gearing
Belt and rope drive
Ball and roller bearing
All of these
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
Below the critical speed
Near the critical speed
Above the critical speed
None of these
On their point of contact
At the centre of curvature
At the centre of circle
At the pin joint
Balanced completely
Balanced partially
Balanced by secondary forces
Not balanced
Universal joint
Knuckle joint
Oldham's coupling
Flexible coupling
Bolt and nut
Lead screw of a lathe
Ball and socket joint
Ball bearing and roller bearing
Return to equilibrium position without oscillation
Oscillate with increasing time period
Oscillate with decreasing amplitude
Oscillate with constant amplitude
Increases
Decreases
Remain same
None of these
Velocity
Displacement
Rate of change of velocity
All of the above
Dynamically balanced
Statically balanced
Statically and dynamically balanced
Not balanced
0.2
0.4
0.6
0.8
Tension in the tight side of the belt
Tension in the slack side of the belt
Sum of the tensions on the tight side and slack side of the belt
Average tension of the tight side and slack side of the belt