ω sinθ/(n² - sin²θ)1/2
ω cosθ/(n² - cos²θ)1/2
ω sinθ/(n² - cos²θ)1/2
ω cosθ/(n² - sin²θ)1/2
D. ω cosθ/(n² - sin²θ)1/2
θ/2
θ
2θ
4θ
a is +ve and b = 0
a = 0 and b is +ve
a is +ve and b is -ve
a is +ve and b is also +ve
Zero
One
π/2
π
Same
Opposite
Perpendicular
None of these
Equal to sum of other two
Greater than sum of other two
Less than sum of other two
There is no such relationship
Pendulum type governor
Dead weight governor
Spring loaded governor
Inertia governor
Same
Different
Unpredictable
None of these
2 W CE / CS
W CE / 2CS
W CE / CS
W CS / 2CE
Crank
Connecting rod
Crank pin
Crosshead
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.
Ball and socket joint
Journal bearing
Lead screw and nut
Cam and follower
Compound gears
Worm and wheel method
Hooke's joint
Crown gear
Simple gear train
Compound gear train
Reverted gear train
Epicyclic gear train
2π. √(g/δ)
1/2π. √(g/δ)
2π. √(δ/g)
1/2π. √(δ/g)
Spur gear
Helical gear
Bevel gear
Spiral gear
m.ω².r sinθ
m.ω².r cosθ
m.ω².r (sin 2θ/n)
m.ω².r (cos 2θ/n)
At the instantaneous center of rotation, one rigid link rotates instantaneously relative to another for the configuration of mechanism considered
The two rigid links have no linear velocities relative to each other at the instantaneous centre
The two rigid links which have no linear velocity relative to each other at this center have the same linear velocity to the third rigid link
The double centre can be denoted either by O2 or O12, but proper selection should be made
Offset between centre lines of cam and follower
Lift of follower
Angle of ascent
All of the above
Velocity
Displacement
Rate of change of velocity
All of the above
Addendum circle
Dedendum circle
Pitch circle
Clearance circle
3 Hz
3π Hz
6 Hz
6π Hz
(1/2) μ W R cosec α
(2/3) μ W R cosec α
(3/4) μ W R cosec α
μ W R cosec α
Bulky
Wears rapidly
Difficult to manufacture
Both (A) and (B) above
Increases
Decreases
Remain unaffected
First increases and then decreases
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
Each of the four pairs is a turning pair
One is a turning pair and three are sliding pairs
Two are turning pairs and two are sliding pairs
Three are turning pairs and one is a sliding pair
15
28
30
8
The system is critically damped
There is no critical speed in the system
The system is also statically balanced
There will absolutely no wear of bearings
Intersecting and coplanar shafts
Nonintersecting and non-coplanar shafts
Parallel and coplanar shafts
Parallel and non-coplanar shafts
Sliding
Turning
Rolling
Screw