Change its motion
Balance the forces, already acting on it
Give rise to the internal stresses in it
All of these
D. All of these
Angle between normal reaction and the resultant of normal reaction and the limiting friction
Ratio of limiting friction and normal reaction
The ratio of minimum friction force to the friction force acting when the body is just about to move
The ratio of minimum friction force to friction force acting when the body is in motion
ω/2π
2π/ω
2π × ω
π/ω
First
Second
Third
None of these
P + Q
P - Q
P / Q
Q / P
a = α/ r
a = α.r
a = r / α
None of these
h/kG
h2/kG
kG2/h
h × kG
Equal to 50 %
Less than 50 %
Greater than 50 %
100 %
Second moment of force
Second moment of area
Second moment of mass
All of these
Will
Will not
Either A or B
None of these
Lie
Do not lie
Either A or B
None of these
Bodies having relative motion
Two dry surfaces
Two lubricated surfaces
Solids and liquids
Equal to
Less than
Greater than
None of these
π/16 (D² - d²)
π/16 (D³ - d³)
π/32 (D⁴ - d⁴)
π/64 (D⁴ - d⁴)
β/2
30° + β/2
45° + β/2
60° + β/2
Between 60 and 70 %
Between 70 and 80 %
Between 80 and 90 %
100 %
Coplanar force
Non-coplanar forces
Moment
Couple
One point
Two points
Plane
Perpendicular planes
(1/2π). √(l/g)
(1/2π). √(g/l)
2π. √(l/g)
None of these
kg-m2
kg-m-s2
kg/m2
m4
3mr2/5
3mr2/10
2mr2/5
4mr2/5
The algebraic sum of the resolved parts of the forces in the given direction
The sum of the resolved parts of the forces in the given direction
The difference of the forces multiplied by the cosine of θ
The sum of the forces multiplied by the sine of θ
1/m
V.R./m
m/V.R.
1/(m × V.R.)
A force acting in the opposite direction to the motion of the body is called force of friction
The ratio of the limiting friction to the normal reaction is called coefficient of friction
A machine whose efficiency is 100% is known as an ideal machine
The velocity ratio of a machine is the ratio of load lifted to the effort applied
(v1 - v2)/(u1 - u2)
(v₂ - v₁)/(u1 - u2)
(u1 - u2)/(v1 - v2)
(u₂ + u₁)/(v₂ + v₁)
The algebraic sum of the forces, constituting the couple is zero
The algebraic sum of the forces, constituting the couple, about any point is the same
A couple cannot be balanced by a single force but can be balanced only by a couple of opposite sense
All of the above
Reversible machine
Non-reversible machine
Neither reversible nor non-reversible machine
Ideal machine
Downward at its upper end
Upward at its upper end
Zero at its upper end
Perpendicular to the wall at its upper end
Same
Half
Double
None of these
g (m1 - m2)/(m1 + m2)
2g (m1 - m2)/(m1 + m2)
g (m1 + m2)/(m1 - m2)
2g (m1 + m2)/(m1 - m2)
Potential energy
Kinetic energy
Power
None of these