Directly proportional
Inversely proportional
Cube root
None of these
A. Directly proportional
Coefficient of friction
Angle of friction
Angle of repose
Sliding friction
sinθ
cosθ
tanθ
cosecθ
Reducing the problem of kinetics to equivalent statics problem
Determining stresses in the truss
Stability of floating bodies
Designing safe structures
P + m.a = 0
P - m.a = 0
P × m.a = 0
P/m.a = 0
Algebraic sum of the horizontal components of all the forces should be zero
Algebraic sum of the vertical components of all the forces should be zero
Algebraic sum of moments of all the forces about any point should be zero
All of the above
0.5r
0.6 r
0.7 r
0.8 r
ω/2π
2π/ω
2π × ω
π/ω
Downwards at its upper end
Upwards at its upper end
Perpendicular to the wall at its upper end
Zero at its upper end
Their algebraic sum is zero
Their lines of action are at equal distances
The algebraic sum of their moments about any point in their plane is zero
The algebraic sum of their moments about any point is equal to the moment of their resultant force about the same point.
Newton
Pascal
Watt
Joule
Energy
Mass
Momentum
Angle
mv2
mgv2
0.5 mv2
0.5 mgv2
Equal to
Less than
Greater than
None of these
Strain energy
Kinetic energy
Heat energy
Electrical energy
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
Do not meet at one point but their lines of action lie on the same plane
None of the above
94.9 cm
99.4 cm
100 cm
101 cm
Maximum
Minimum
Zero
Infinity
Bodies having relative motion
Two dry surfaces
Two lubricated surfaces
Solids and liquids
√(P² + Q² + 2PQ sinθ)
√(P² + Q² + 2PQ cosθ)
√(P² + Q² - 2PQ cosθ)
√(P² + Q² - 2PQ tanθ)
Three forces acting at a point will be in equilibrium
Three forces acting at a point can be represented by a triangle, each side being proportional to force
If three forces acting upon a particle are represented in magnitude and direction by the sides of a triangle, taken in order, they will be in equilibrium
If three forces acting at a point are in equilibrium, each force is proportional to the sine of the angle between the other two
20 kg, -ve sense
20 kg, + ve sense
10 kg, + ve sense
10 kg, -ve sense
Angle of projection
Angle of inclination of the plane
Both (A) and (B)
None of these
Direction of the axis of rotation
Magnitude of angular displacement
Sense of angular displacement
All of these
Force
Work
Power
Velocity
Arm of man
Pair of scissors
Pair of clinical tongs
All of the above
The tangent of the angle of friction is equal to coefficient of friction
The angle of repose is equal to angle of friction
The tangent of the angle of repose is equal to coefficient of friction
The sine of the angle of repose is equal to coefficient to friction
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
Angle of friction
Angle of repose
Angle of banking
None of these
Angular displacement
Angular velocity
Angular acceleration
All of these
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