ωx
ω²x
ω²/x
ω³/x
B. ω²x
A rigid link rotates instantaneously relative to another link at the instantaneous centre for the configuration of the mechanism considered.
The two rigid links have no linear velocity relative to each other at the instantaneous centre.
The velocity of the instantaneous centre relative to any third rigid link is same whether the instantaneous centre is regarded as a point on the first rigid link or on the second rigid link.
All of the above
Damping factor
Damping coefficient
Logarithmic decrement
Magnification factor
Along the angular velocity
Opposite to angular velocity
May be any one of these
Perpendicular to angular velocity
(1/2) μ W R
(2/3) μ W R
(3/4) μ W R
μ W R
Open pair
Kinematic pair
Sliding pair
None of these
n = 3(l - 1) - 2j - h
n = 2(l - 1) -2j - h
n = 3(l - 1) - 3j - h
n = 2(l - 1) - 3j - h
Same
Opposite
Perpendicular
None of these
m/(m + M)
M/(m + M)
(m + M)/m
(m + M)/M
Each of the four pairs is a turning pair
One is a turning pair and three are sliding pairs
Two are turning pairs and two are sliding pairs
Three are turning pairs and one is a sliding pair
90° and 180°
45° and 225°
180° and 270°
270° and 360°
(ω₁ + ω₂)y
(ω₁/ω₂)y
(ω₁ × ω₂)y
(ω₁ + ω₂)/y
1/24
1/8
4/15
12
2π. √(g/l)
(1/2π). √(g/l)
2π. √(l/g)
(1/2π). √(l/g)
Equal to 1
Equal to 2
Less than 2
Greater than 2
Inner edge
Outer edge
Corners
None of these
ω² r {(n + 1)/n}
ω² r {(n - 1)/n}
ω² r {n/(n + 1)}
ω² r {n/(n - 1)}
Balancing partially revolving masses
Balancing partially reciprocating masses
Best balancing of engines
All of these
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
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
Scott-Russell's mechanism
Hart's mechanism
Peaucellier's mechanism
All of these
ω √(x² - r²)
ω √(r² - x²)
ω² √(x² - r²)
ω² √(r² - x²)
Steering
Pitching
Rolling
All of the above
Dependent on the size of teeth
Dependent on the size of gears
Always constant
Always variable
kG + l₁
kG² + l₁
(kG² + l₁²)/ l₁
(kG + l₁²)/ l₁
ω²r. (n + 1)/n
ω²r. (n - 1)/n
ω²r. n/(n + 1)
ω²r. n/(n - 1)
Angular acceleration of the body
Moment of inertia of the body
Periodic time of the body
Frequency of vibration of the body
Over-damped
Under damped
Critically damped
Without vibrations
Crank
Connecting rod
Crank pin
Crosshead
Increases as the radius of rotation decreases
Increases as the radius of rotation increases
Decreases as the radius of rotation increases
Remains constant for all radii of rotation
Minimise the effect of primary forces
Minimise the effect of secondary forces
Have perfect balancing
To start the locomotive quickly