ω
ωr
ω2r
ω/r
B. ωr
Towards the wall at its upper end
Away from the wall at its upper end
Downward at its upper end
Upward at its upper end
Three forces acting at a point will be in equilibrium
Three forces acting at a point can be represented by a triangle, each side being proportional to force
If three forces acting upon a particle are represented in magnitude and direction by the sides of a triangle, taken in order, they will be in equilibrium
If three forces acting at a point are in equilibrium, each force is proportional to the sine of the angle between the other two
15 N and 5 N
20 N and 5 N
15 N and 15 N
None of these
Proportional to normal load between the surfaces
Dependent on the materials of contact surface
Proportional to velocity of sliding
Independent of the area of contact surfaces
Increase
Decrease
Remain the same
None of these
Mechanical advantage is greater than velocity ratio
Mechanical advantage is equal to velocity ratio
Mechanical advantage is less than velocity ratio
Mechanical advantage is unity
P/2
2P
√2 × P
P/√2
D/(d₁ + d₂)
D/(d₁ - d₂)
2D/(d₁ + d₂)
2D/(d₁ - d₂)
kg-m²
m²/kg.
kg/m²
kg/m
W/√3 (compression)
W/√3 (tension)
2W/√3 (compression)
2W/√3 (tension)
Potential energy only
Kinetic energy of translation only
Kinetic energy of rotation only
Kinetic energy of translation and rotation both
Translatory motion
Rotational motion
Combined translatory and rotational motion
None of the above
Coplanar non-concurrent forces
Non-coplanar concurrent forces
Non-coplanar non-concurrent forces
Intersecting forces
a4/4
a4/8
a4/12
a4/36
Purely translation
Purely rotational
Combined translation and rotational
None of these
20 N
40 N
120 N
None of these
g (m1 - m2)/(m1 + m2)
2g (m1 - m2)/(m1 + m2)
g (m1 + m2)/(m1 - m2)
2g (m1 + m2)/(m1 - m2)
(1 - sinφ)/(1 + sinφ)
(1 + sinφ)/(1 - sinφ)
(1 - tanφ)/(1 + tanφ)
(1 + tanφ)/(1 - tanφ)
Less than
Equal to
More than
None of these
Work is done by a force of 1 N when it displaces a body through 1 m
Work is done by a force of 1 kg when it displaces a body through 1 m
Work is done by a force of 1 dyne when it displaces a body through 1 cm
Work is done by a force of 1 g when it displaces a body through 1 cm
ω/r
ω.r
ω2/r
ω2.r
More inclined when moving
Less inclined when moving
More inclined when standing
Less inclined when standing
mr2/3
2mr2/3
2mr2/5
3mr2/5
0.5r
0.6 r
0.7 r
0.8 r
Tangent of angle between normal reaction and the resultant of normal reaction and the limiting friction
Ratio of limiting friction and normal reaction
The friction force acting when the body is just about to move
The friction force acting when the body is in motion
Potential energy
Kinetic energy
Power
None of these
30°
60°
90°
120°
Mechanical advantage is greater than velocity ratio
Mechanical advantage is equal to velocity ratio
Mechanical advantage is less than velocity ratio
Mechanical advantage is unity
The tangent of the angle of friction is equal to coefficient of friction
The angle of repose is equal to angle of friction
The tangent of the angle of repose is equal to coefficient of friction
The sine of the angle of repose is equal to coefficient to friction
Dyne
Kilogram
Newton
Watt