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
D. Addendum circle to the clearance circle
Longitudinal vibrations
Transverse vibrations
Torsional vibrations
None of these
No node
One node
Two nodes
Three nodes
A very thin film of lubricant between the journal and the bearing such that there is contact between the journal and the bearing
A thick film of lubricant between the journal and the bearing
No lubricant between the journal and the bearing
A forced lubricant between the journal and the bearing
1
1/π
π
2 π
Straight line
Circle
Ellipse
Parabola
Fluctuation of energy
Maximum fluctuation of energy
Coefficient of fluctuation of energy
None of these
(1/2) μ W R
(2/3) μ W R
(3/4) μ W R
μ W R
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
P = W tan(α - φ)
P = W tan(α + φ)
P = W tan(φ - α)
P = W cos(α + φ)
ω² R cosθ
ω² (R - r₁) cosθ
ω² (R - r₁) sinθ
ω² r₁ sinθ
Thompson indicator
Richard indicator
Simplex indicator
Thomson indicator
(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)]
Point contact
Surface contact
No contact
None of the above
Beam engine
Rotary engine
Oldhams coupling
Elliptical trammel
Less sensitive
More sensitive
Unaffected of sensitivity
Isochronous
Structure
Machine
Inversion
Compound mechanism
P = W tan(α - φ)
P = W tan(α + φ)
P = W tan(φ - α)
P = W cos(α + φ)
Sliding pair
Rolling pair
Lower pair
Higher pair
Cylindrical pair
Turning pair
Rolling pair
Sliding pair
No acceleration
Linear acceleration
Angular acceleration
Both angular and linear accelerations
The sum of the two masses is equal to the total mass of body
The centre of gravity of the two masses coincides with that of the body
The sum of mass moment of inertia of the masses about their centre of gravity is equal to the mass moment of inertia of the body
All of the above
Spur gearing
Helical gearing
Bevel gearing
Spiral gearing
Varies in magnitude but constant in direction
Varies in direction but constant in magnitude
Varies in magnitude and direction both
Constant in magnitude and direction both
Be zero
Act in upward direction
Act in downward direction
None of these
Open pair
Closed pair
Sliding pair
Point contact pair
Simple
Compound
Binary
None of these
Displacement of various parts
Velocity of various parts
Acceleration of various parts
Angular acceleration of various parts
One direction only
Two directions only
More than one direction
None of these
Four times the first one
Same as the first one
One fourth of the first one
One and a half times the first one
(1/2) μ W R cosec α
(2/3) μ W R cosec α
(3/4) μ W R cosec α
μ W R cosec α