Kinetic friction
Limiting friction
Angle of repose
Coefficient of friction
D. Coefficient of friction
t = g cos β/2u sin (α - β)
t = 2u sin (α - β)/g cos β
t = g cos β/2u sin (α + β)
t = 2u sin (α + β)/g cos β
The kinetic energy of a body during impact remains constant.
The kinetic energy of a body before impact is equal to the kinetic energy of a body after impact.
The kinetic energy of a body before impact is less than the kinetic energy of a body after impact.
The kinetic energy of a body before impact is more than the kinetic energy of a body after impact.
kg-m2
kg-m-s2
kg/m2
m4
Change its motion
Balance the other forces acting on it
Retard its motion
All of the above
One fourth of the total height above base
One third of the total height above base
One-half of the total height above base
Three eighth of the total height above the base
h/(kG² + h²)
(kG² + h²)/h
h²/(kG² + h²)
(kG² + h²)/h²
Kinetic friction
Limiting friction
Angle of repose
Coefficient of friction
Magnitude
Direction
Point of application
All of the above
[√(4p² - q²)]/6
(4p² - q²)/6
(p² - q²)/4
(p² + q²)/4
Same
More
Less
May be less of more depending on nature of surfaces and velocity
Compression or tension
Buckling or shear
Shear or tension
All of the above
Output to the input
Work done by the machine to the work done on the machine
Mechanical advantage to the velocity ratio
All of the above
Newton's first law of motion
Newton's second law of motion
Newton's third law of motion
None of these
A force acting in the opposite direction to the motion of the body is called force of friction
The ratio of the limiting friction to the normal reaction is called coefficient of friction
A machine whose efficiency is 100% is known as an ideal machine
The velocity ratio of a machine is the ratio of load lifted to the effort applied
0°
30°
45°
60°
Meet
Do not meet
Either A or B
None of these
Upwards
Downwards
Horizontal
None of these
0.1 N-m
1 N-m
10 N-m
100 N-m
ω.√(y² - r²)
ω.√(r² - y²)
ω².√(y² - r²)
ω².√(r² - y²)
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
Newton's first law of motion
Newton's second law of motion
Principle of conservation of energy
Principle of conservation of momentum
a4/4
a4/8
a4/12
a4/36
g/2
g/3
g/4
None of these
If a system of coplanar forces is in equilibrium, then their algebraic sum is zero
If a system of coplanar forces is in equilibrium, then the algebraic sum of their moments about any point in their plane is zero
The algebraic sum of the moments of any two forces about any point is equal to moment of the resultant about the same point
Positive and negative couples can be balanced
Equal to
Less than
Greater than
None of these
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
πd3/16
πd3/32
πd4/32
πd4/64
Zero
Minimum
Maximum
None of these
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
Zero
One
Between zero and one
More than one