(l₁ + l₂ + l₃)/3
l = l₁ + l₂.(d₁/d₂)³ + l₂.(d₁/d₃)³
l = l₁ + l₂.(d₁/d₂)⁴ + l₃.(d₁/d₃)⁴
l₁ + l₂ + l₃
C. l = l₁ + l₂.(d₁/d₂)⁴ + l₃.(d₁/d₃)⁴
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
Constant
In arithmetic progression
In geometric progression
In logarithmic progression
ωR cosθ
ω(R - r₁) cosθ
ω(R - r₁) sinθ
ωr₁ sinθ
Parallel to OA
Perpendicular to OA
At 45° to OA
Along AO
(r₁² - r₂²)/(r₁ - r₂)
(r₁² - r₂²)/(r₁ + r₂)
(r₁³ - r₂³)/(r₁² - r₂²)
(r₁³ - r₂³)/(r₁ - r₂)
Below the critical speed
Near the critical speed
Above the critical speed
None of these
Crank has uniform angular velocity
Crank has nonuniform angular velocity
Crank has uniform angular acceleration
Crank has nonuniform angular acceleration
L + 1
L - 1
L
L + 2
Increases as the radius of rotation decreases
Increases as the radius of rotation increases
Decreases as the radius of rotation increases
Remain constant for all radii of rotation
Sliding pairs
Turning pairs
Rolling pairs
Higher pairs
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)
12
16
25
32
Turning pair
Rolling pair
Screw pair
Spherical pair
Inner edge
Outer edge
Corners
None of these
ω
ωr
ω²r
ω/r
Static friction
Dynamic friction
Limiting friction
Coefficient of friction
Dedendum
Addendum
Clearance
Working depth
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
Increases
Decreases
Remain unaffected
First increases and then decreases
Journal bearing
Ball and Socket joint
Leave screw and nut
None of the above
2πk/r. √(g/l)
r/2πk. √(l/g)
2πr/k. √(g/l)
r/2πk. √(g/l)
One lower pair and two additional links
Two lower pairs and one additional link
Two lower pairs and two additional links
Any one of these
(1/2). μ W cosecα (r₁ + r₂)
(2/3). μ W cosecα (r₁ + r₂)
(1/2). μ W cosecα [(r₁³ - r₂³)/(r₁² - r₂²)]
(2/3). μ W cosecα [(r₁³ - r₂³)/(r₁² - r₂²)]
60 to 80 r.p.m.
80 to 100 r.p.m.
100 to 200 r.p.m.
200 to 300 r.p.m.
Tractive force
Swaying couple
Hammer blow
None of these
The interference is inherently absent.
The variation in centre distance of shafts increases radial force.
A convex flank is always in contact with concave flank.
The pressure angle is constant throughout the teeth engagement.
Fluctuation of energy
Maximum fluctuation of energy
Coefficient of fluctuation of energy
None of these
Transverse vibrations
Torsional vibrations
Longitudinal vibrations
All of these
(1/2). μ W cosec α (r₁ + r₂)
(2/3).μ W cosec α (r₁ + r₂)
(1/2). μ W cosec α [(r₁³ - r₂³)/(r₁² - r₂²)]
(2/3). μ W cosec α [(r₁³ - r₂³)/(r₁² - r₂²)]
Inside admission valve
Outside admission valve
Piston slide valve
None of these