1-3 m/s
3-15 m/s
15-30 m/s
30-50 m/s
B. 3-15 m/s
Simple pendulum
Compound pendulum
Torsional pendulum
Second's pendulum
Machine
Structure
Mechanism
Inversion
Equal to 1
Less than 2
Equal to 2
Greater than 2
Journal bearing
Ball and Socket joint
Leave screw and nut
None of the above
Is in phase
Leads by 90°
Leads by 180°
Lags by 90°
1
1/π
π
2 π
9/8
9/82
9/16
9/128
P = W tan(α - φ)
P = W tan(α + φ)
P = W tan(φ - α)
P = W cos(α + φ)
Cause withdrawing or throttling of steam
Reduce length of effective stroke of piston
Reduce maximum opening of port to steam
All of these
Can be used
Cannot be used
Unpredictable
None of these
Pitch circle to the bottom of a tooth
Pitch circle to the top of a tooth
Top of a tooth to the bottom of a tooth
Addendum circle to the clearance circle
Knife edge follower
Flat faced follower
Spherical faced follower
Roller follower
Inertia
Momentum
Moment of momentum
Torque
Slow speed
Moderate speed
Highs peed
Any one of these
(1/2) μ W R
(2/3) μ W R
(3/4) μ W R
μ W R
Slider crank mechanism
Four bar chain mechanism
Quick return motion mechanism
All of these
ω × AB
ω × (AB)²
ω² × AB
(ω × AB)²
In plane rotation with variable velocity
In plane translation with variable velocity
In plane motion which is a resultant of plane translation and rotation
Restrained to rotate while sliding over another body
μwr
¾μWR
(2/3) μWR
½μWR
π (r₁ + r₂) + [(r₁ + r₂)²/x] + 2x
π (r₁ + r₂) + [(r₁ - r₂)²/x] + 2x
π (r₁ - r₂) + [(r₁ - r₂)²/x] + 2x
π (r₁ - r₂) + [(r₁ + r₂)²/x] + 2x
0° and 90°
0° and 180°
90° and 180°
180° and 360°
Primary forces and couples must be balanced
Secondary forces and couples must be balanced
Both (A) and (B)
None of these
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
During which the follower returns to its initial position
Of rotation of the cam for a 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
Weak material of the belt
Weak material of the pulley
Uneven extensions and contractions of the belt when it passes from tight side to slack side
Expansion of the belt
A round bar in a round hole form a turning pair
A square bar in a square hole form a sliding pair
A vertical shaft in a foot step bearing forms a successful constraint
All of the above
The algebraic sum of the secondary forces must be equal to zero
The algebraic sum of the couples about any point in the plane of the secondary forces must be equal to zero
Both (A) and (B)
None of these
Lower pair
Higher pair
Self-closed pair
Force-closed pair
ω² r {(n + 1)/n}
ω² r {(n - 1)/n}
ω² r {n/(n + 1)}
ω² r {n/(n - 1)}
(1 - sinφ)/(1 + sinφ)
(1 + sinφ)/(1 - sinφ)
(1 - tanφ)/(1 + tanφ)
(1 + tanφ)/(1 - tanφ)