(r₁ - r₂) (1 - cosθ)
(r₁ + r₂) (1 + cosθ)
(r₁ - r₂) [(1 - cosθ)/cos θ]
(r₁ + r₂) [(1 - cosθ)/cos θ]
D. (r₁ + r₂) [(1 - cosθ)/cos θ]
Theory of machines
Applied mechanics
Mechanisms
Kinetics
Because of difficulty in manufacturing cam profile
Because of loose contact of follower with cam surface
In order to have acceleration in beginning and retardation at the end of stroke within the finite limits
Because the uniform velocity motion is a partial parabolic motion
The power absorbed in operating the piston valve is less than D-slide valve
The wear of the piston valve is less than the wear of the D-slide valve
The D-slide valve is also called outside admission valve.
All of the above
Changing of a higher pair to a lower pair
Turning its upside down
Obtained by fixing different links in a kinematic chain
Obtained by reversing the input and output motion
vBA × AB
vBA /AB
v²BA
v²BA /AB
Pitch circle dia. × cosφ
Addendum circle dia. × cosφ
Clearance circle dia. × cosφ
Pitch circle dia. × sinφ
Yes
No
It is a marginal case
Data are insufficient to determine it
Theory of machines
Applied mechanics
Mechanisms
Kinetics
Base circle
Pitch circle
Prime circle
Pitch curve
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.
Shoe brake
Band brake
Band and block brake
Internal expanding brake
Vertically and parallel
Vertically and perpendicular
Horizontally and parallel
Horizontally and perpendicular
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
Any point on pitch curve
The point on cam pitch curve having the maximum pressure angle
Any point on pitch circle
The point on cam pitch curve having the minimum pressure angle
Halved
Doubled
Quadrupled
None of these
At the origin
Below the origin
Above the origin
Any one of these
Fluctuation of speed
Maximum fluctuation of speed
Coefficient of fluctuation of speed
None of these
1
1/π
π
2 π
Pitch circle
Base circle
Pitch curve
Prime circle
(r₁ - r₂) (1 - cosθ)
(r₁ + r₂) (1 + cosθ)
(r₁ - r₂) [(1 - cosθ)/cos θ]
(r₁ + r₂) [(1 - cosθ)/cos θ]
45 mm
Slightly less than 45 mm
Slightly more than 45 mm
95 mm
45°
90°
135°
180°
On their point of contact
At the centre of curvature
At the centre of circle
At the pin joint
Fc = ar + b
Fc = ar - b
Fc = ar
Fc = a/r + b
Total lift, total angle of lift, minimum radius of cam and cam speed
Radius of circular arc, cam speed, location of centre of circular arc and roller diameter
Mass of cam follower linkage, spring stiffness and cam speed
Total lift, centre of gravity of the cam and cam speed
Equal to
Less than
Greater than
None of these
Material of the pulley
Material of the belt
Larger size of the driver pulley
Uneven extensions and contractions due to varying tension
6 times more
6 times less
2.44 times more
2.44 times less
(1/2) μ W (r₁ + r₂)
(2/3) μ W (r₁ + r₂)
(1/2) μ W [(r₁³ - r₂³)/(r₁² - r₂²)]
(2/3) μ W [(r₁³ - r₂³)/(r₁² - r₂²)]
Simple train of wheels
Compound train of wheels
Reverted gear train
Epicyclic gear train