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
C. Meet at one point and their lines of action also lie on the same plane
94.9 cm
99.4 cm
100 cm
101 cm
1/2
2/3
3/2
2/4
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
Balance each other
Constitute a moment
Constitute a couple
Constitute a moment of couple
ω
ωr
ω2r
ω/r
Equal to 50 %
Less than 50 %
Greater than 50 %
100 %
All the forces are equally inclined
Sum of all the forces is zero
Sum of resolved parts in the vertical direction is zero (i.e. ΣV = 0)
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
2mr2/3
2mr2/5
7mr2/3
7mr2/5
Directly
Inversely
Square root
None of these
L/2
L/3
3L/4
2L/3
Equal to
Less than
Greater than
None of these
Reversible machine
Non-reversible machine
Neither reversible nor non-reversible machine
Ideal machine
The periodic time of a particle moving with simple harmonic motion is the time taken by a particle for one complete oscillation.
The periodic time of a particle moving with simple harmonic motion is directly proportional to its angular velocity.
The velocity of the particle moving with simple harmonic motion is zero at the mean position.
The acceleration of the particle moving with simple harmonic motion is maximum at the mean position.
Angle of friction
Angle of repose
Angle of projection
None of these
Right angled triangle
Equilateral triangle
Square
Circle
u² sin²α/2g
u² cos²α/2g
u² sin²α/g
u² cos²α/g
Simple pendulum
Compound pendulum
Torsional pendulum
Second's pendulum
Arm of man
Pair of scissors
Pair of clinical tongs
All of the above
sinθ
cosθ
tanθ
cosecθ
Rolling friction
Dynamic friction
Limiting friction
Static friction
1 + m
1 - m
1 / m
m
Coplanar
Meet at one point
Both (A) and (B) above
All be equal
h/(kG² + h²)
(kG² + h²)/h
h²/(kG² + h²)
(kG² + h²)/h²
Less than
More than
Equal to
None of These
(v1 - v2)/(u1 - u2)
(v₂ - v₁)/(u1 - u2)
(u1 - u2)/(v1 - v2)
(u₂ + u₁)/(v₂ + v₁)
Friction
Limiting friction
Repose
Kinematic friction
Weight
Velocity
Acceleration
Force
Non-equilibrium
Partial equilibrium
Full equilibrium
Unpredictable
r/2
2r/3
r/A
3r/2