Towards the wall at its upper end
Away from the wall at its upper end
Upwards at its upper end
Downwards at its upper end
C. Upwards at its upper end
√(P² + Q² + 2PQ sinθ)
√(P² + Q² + 2PQ cosθ)
√(P² + Q² - 2PQ cosθ)
√(P² + Q² - 2PQ tanθ)
kg m
kcal
Watt
Watt hours
Angle of friction
Angle of repose
Angle of projection
None of these
P/sin β = Q/sin α = R/sin
P/sin α = Q/sin β = R/sin
P/sin = Q/sin α = R/sin β
P/sin α = Q/sin = R/sin β
Same as
Twice
Thrice
Four times
W sinθ
W cosθ
W tanθ
None of these
Newton's first law of motion
Newton's second law of motion
Newton's third law of motion
None of these
Tangent of angle between normal reaction and the resultant of normal reaction and 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
m/min
rad/s
Revolutions/min
Both (B) and (C)
Increasing the length of the handle
Increasing the radius of the load drum
Increasing the number of teeth of the pinion
All 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
Will
Will not
Either A or B
None of these
(1/2π). √(l/g)
(1/2π). √(g/l)
2π. √(l/g)
None of these
Static friction
Dynamic friction
Limiting friction
Coefficient of friction
The same as centre of gravity
The point of suspension
The point of application of the resultant of all the forces tending to cause a body to rotate about a certain axis
None of the above
Translatory motion
Rotational motion
Combined translatory and rotational motion
None of the above
20 N
40 N
120 N
None of these
Remain horizontal
Slant up towards direction of pull
Slant down towards direction of pull
None of the above
Lie on the same line
Meet at one point
Meet on the same plane
None of these
db3/12
bd³/12
db³/36
bd³/36
Downward at its upper end
Upward at its upper end
Zero at its upper end
Perpendicular to the wall at its upper end
Equal to
Less than
Greater than
None of these
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
Less than
Equal to
More than
None of these
Equal to 50 %
Less than 50 %
Greater than 50 %
100 %
Newton
Pascal
Watt
Joule
Coplanar concurrent forces
Coplanar non-concurrent forces
Like parallel forces
Unlike parallel forces
(BD³/12) - (bd³/12)
(DB³/12) - (db³/12)
(BD³/36) - (bd³/36)
(DB³/36) - (db³/36)
Is constant at every instant
Varies from point to point
Is maximum in the start and minimum at the end
Is minimum in the start and maximum at the end
D + d
D - d
D × d
D / d