Along the plane
Horizontally
Vertically
At an angle equal to the angle of friction to the inclined plane
D. At an angle equal to the angle of friction to the inclined plane
Limiting friction
Kinematic friction
Frictional resistance
Dynamic friction
Impulsive force
Mass
Weight
Momentum
One point
One plane
Different planes
Perpendicular planes
0° and 180°
180° and 0°
90° and 180°
90° and 0°
Magnitude
Direction
Point of application
All of the above
1 m
2 m
3 m
4 m
Meet
Do not meet
Either A or B
None of these
3mr2/5
3mr2/10
2mr2/5
4mr2/5
Translatory
Rotary
Circular
Translatory as well as rotary
n
n²
2n
2n - 1
Inward
Outward
Towards front
Towards back
Downwards at its upper end
Upwards at its upper end
Perpendicular to the wall at its upper end
Zero at its upper end
Stable
Unstable
Neutral
None of these
Equal to
Less than
Greater than
None of these
Equal to
Less than
Greater than
None of these
IP = IG + Ah2
IP = IG - Ah2
IP = IG / Ah2
IP = Ah2 / IG
Two members with unknown forces of the frame
Three members with unknown forces of the frame
Four members with unknown forces of the frame
Three members with known forces of the frame
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
Balance each other
Produce a couple and an unbalanced force
Are equivalent
Cannot balance each other
Everybody continues in its state of rest or of uniform motion, in a straight line, unless it is acted upon by some external force
The rate of change of momentum is directly proportional to the impressed force, and takes place in the same direction, in which the force acts
To every action, there is always an equal and opposite reaction
None of the above
If any number of forces acting at a point can be represented by the sides of a polygon taken in order, then the forces are in equilibrium
If any number of forces acting at a point can be represented in direction and magnitude by the sides of a polygon, then the forces are in equilibrium
If a polygon representing forces acting at a point is closed then forces are in equilibrium
If any number of forces acting at a point can be represented in direction and magnitude by the sides of a polygon taken in order, then the forces are in equilibrium
In the shaded area
In the hole
At O
None of these
Iω
Iω2
0.5 Iω
0.5 Iω2
Increase
Decrease
Remain the same
None of these
6t² - 8t
3t² + 2t
6f - 8
6f - 4
Is the turning effect produced by a force, on the body, on which it acts
Is equal to the product of force acting on the body and the perpendicular distance of a point and the line of action of the force
Is equal to twice the area of the triangle, whose base is the line representing the force and whose vertex is the point, about which the moment is taken
All of the above
(1/2π). √(l/g)
(1/2π). √(g/l)
2π. √(l/g)
None of these
94.9 cm
99.4 cm
100 cm
101 cm
Newton's first law of motion
Newton's second law of motion
Newton's third law of motion
None of these
The point of C.G.
The point of metacenter
The point of application of the resultant of all the forces tending to cause a body to rotate about a certain axis
Point of suspension