Simple gear train
Compound gear train
Reverted gear train
Epicyclic gear train
D. Epicyclic gear train
Theory of machines
Applied mechanics
Mechanisms
Kinetics
Greater than
Less than
Equal to
None of these
cosθ = sinα
sinθ = ± tanα
tanθ = ± cosα
cotθ = cosα
Two forks
One fork
Three forks
Four forks
Rotating
Oscillating
Reciprocating
All of the above
Mass and stiffness
Mass and damping coefficient
Mass and natural frequency
Damping coefficient and natural frequency
Magnitude of the forces on journal
Angular velocity of journal
Clearance between journal and bearing
Radius of journal
Tension in the tight side of the belt
Tension in the slack side of the belt
Sum of the tensions on the tight side and slack side of the belt
Average tension of the tight side and slack side of the belt
Is in phase
Leads by 90°
Leads by 180°
Lags by 90°
Grasshopper mechanism
Watt mechanism
Peaucellier's mechanism
Tchebicheff mechanism
ω²r. (n + 1)/n
ω²r. (n - 1)/n
ω²r. n/(n + 1)
ω²r. n/(n - 1)
Maximum
Minimum
Zero
None of these
(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)]
Universal joint
Knuckle joint
Oldham's coupling
Flexible coupling
A small value of pressure angle
A large value of pressure angle
There is no such relation with pressure angle
Something else
1-3 m/s
3-15 m/s
15-30 m/s
30-50 m/s
The parts of a machine move relative to one another, whereas the members of a structure do not move relative to one another
The links of a machine may transmit both power and motion, whereas the members of a structure transmit forces only
A machine transforms the available energy into some useful work, whereas in a structure no energy is transformed into useful work
All of the above
Lower pair
Higher pair
Self-closed pair
Force-closed pair
Flat pivot bearing
Flat collar bearing
Conical pivot bearing
Truncated conical pivot bearing
Remain same as before
Become equal to 2R
Become equal to R/2
Become equal to R/4
Parallel
Perpendicular
Both A and B
None of these
The primary unbalanced force is less than the secondary unbalanced force.
The primary unbalanced force is maximum twice in one revolution of the crank.
The unbalanced force due to reciprocating masses varies in magnitude and direction both.
The magnitude of swaying couple in locomotives is inversely proportional to the distance between the two cylinder centre lines
Whitworth quick return mechanism
Hand pump
Oscillating cylinder engine
All of the above
Equal to
Less than
Greater than
None of these
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
Maximum and zero
Zero and maximum
Minimum and maximum
Zero and minimum
n₁ + n₂
n₁ + n₂ + 1
n₁ + n₂ - 1
n₁ + n₂ - 2
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
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
μ₁ = μ sinβ
μ₁ = μ cosβ
μ₁ = μ/sinβ
μ₁ = μ/cosβ