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
D. All of the above
20 kg, -ve sense
20 kg, + ve sense
10 kg, + ve sense
10 kg, -ve sense
4
8
16
20
Bears a constant ratio to the normal reaction between the two surfaces
Is independent of the area of contact, between the two surfaces
Always acts in a direction, opposite to that in which the body tends to move
All of the above
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
25
50
100
250
Same as
Twice
Thrice
Four times
Meet at one point, but their lines of action do not lie on the same plane
Do not meet at one point and their lines of action do not lie on the same plane
Meet at one point and their lines of action also lie on the same plane
Do not meet at one point, but their lines of action lie on the same plane
a2/8
a3/12
a4/12
a4/16
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
P + Q
P - Q
P / Q
Q / P
These forces are equal
The lines of action of these forces meet in a point
The lines of action of these forces are parallel
Both (B) and (C) above
7.8 N
8.9 N
9.8 N
12 N
The C.G. of a circle is at its centre
The C.G. of a triangle is at the intersection of its medians
The C.G. of a rectangle is at the intersection of its diagonals
The C.G. of a semicircle is at a distance of r/2 from the centre
Simple pendulum
Compound pendulum
Torsional pendulum
Second's pendulum
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
π/16 (D² - d²)
π/16 (D³ - d³)
π/32 (D⁴ - d⁴)
π/64 (D⁴ - d⁴)
m1/m2
m1. g. sin α
m1.m2/m1 + m2
m1. m2.g (1 + sin α)/(m1 + m2)
Coplanar non-concurrent forces
Non-coplanar concurrent forces
Non-coplanar non-concurrent forces
Intersecting forces
Newton
erg
kg-m
joule
More inclined when moving
Less inclined when moving
More inclined when standing
Less inclined when standing
Static friction
Dynamic friction
Limiting friction
Coefficient of friction
Newton's first law of motion
Newton's second law of motion
Newton's third law of motion
None of these
g. cos² β/2u². sin (α + β). cos α
2u². sin (α + β). cos α/g. cos² β
g. cos² β/2u². sin (α - β). cos α
2u². sin (α - β). cos α/g. cos² β
db³/12
bd³/12
db³/36
bd³/36
h/2
J/3
h/6
h/4
Coplanar force
Non-coplanar forces
Moment
Couple
n
n²
2n
2n - 1
Rotate about itself without moving
Move in any one direction rotating about itself
Be completely at rest
All of these
15 N and 5 N
20 N and 5 N
15 N and 15 N
None of these
Newton's first law of motion
Newton's second law of motion
Newton's third law of motion
None of these