Double slider crank chain
Elliptical trammel
Scotch yoke mechanism
All of these
D. All of these
A small value of pressure angle
A large value of pressure angle
There is no such relation with pressure angle
Something else
Leads by 90°
Lags by 90°
Leads by 180°
Are in phase
One direction only
Two directions only
More than one direction
None of these
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
Cylinder and piston
Piston rod and connecting rod
Crankshaft and flywheel
Flywheel and engine frame
Purely turning
Purely sliding
Purely rotary
Combination of sliding and turning
Four
Five
Six
Seven
10°
14°
20°
30°
More than
Less than
Same as
None of these
Flat pivot bearing
Flat collar bearing
Conical pivot bearing
Truncated conical pivot bearing
2
3
4
5
Theory of machines
Applied mechanics
Mechanisms
Kinetics
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.
Difference of minimum fluctuation of speed and the mean speed
Difference of the maximum and minimum speeds
Sum of maximum and minimum speeds
Variations of speed above and below the mean resisting torque line
0.2
0.4
0.6
0.8
Second inversion of double slider crank chain
Third inversion of double slider crank chain
Second inversion of single slider crank chain
Third inversion of slider crank chain
Is directly proportional to
Is inversely proportional to
Is equal to cos φ multiplied by
Does not depend upon
Sliding pairs
Turning pairs
Rolling pairs
Higher pairs
Vector sum of radial component and coriolis component
Vector sum of tangential component and coriolis component
Vector sum of radial component and tangential component
Vector difference of radial component and tangential component
fn/2
2 fn
4 fn
8 fn
ω₁.ω₂.r
(ω₁ - ω₂)r
(ω₁ + ω₂)r
(ω₁ - ω₂)2r
Bevel gear
Universal joint
Hooke's joint
Knuckle joint
ωv
2ωv
ω²v
2ωv²
No acceleration
Only linear acceleration
Only angular acceleration
Both linear and angular acceleration
Is based on acceleration diagram
Is a simplified form of instantaneous center method
Utilises a quadrilateral similar to the diagram of mechanism for reciprocating engine
Enables determination of Carioles component
m.ω².r cosθ
c.m.ω².r sinθ
(1 - c).m.ω².r (cosθ - sinθ)
m.ω².r (cosθ - sinθ)
Inner dead centre
Outer dead centre
Right angles to the link of the stroke
All of the above
There is a reduction in amplitude after every cycle of vibration
No external force acts on a body, after giving it an initial displacement
A body vibrates under the influence of external force
None of the above
Angular acceleration of the body
Moment of inertia of the body
Periodic time of the body
Frequency of vibration of the body
One-half
Two-third
Three-fourth
Whole