Between 60 and 70 %
Between 70 and 80 %
Between 80 and 90 %
100 %
D. 100 %
Coefficient of friction
Angle of friction
Angle of repose
Sliding friction
(v1 - v2)/(u1 - u2)
(v₂ - v₁)/(u1 - u2)
(u1 - u2)/(v1 - v2)
(u₂ + u₁)/(v₂ + v₁)
Halved
Doubled
Quadrupled
None of these
Maximum
Minimum
Zero
Infinity
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
kg m
kcal
Watt
Watt hours
IP = IG + Ah2
IP = IG - Ah2
IP = IG / Ah2
IP = Ah2 / IG
3r/ 8
4r/ 3π
8r/3
3r/4π
Arm of man
Pair of scissors
Pair of clinical tongs
All of the above
Stable
Unstable
Neutral
None of these
g sinθ
g cosθ
g tanθ
None of these
7.8 N
8.9 N
9.8 N
12 N
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.
Equal to
Less than
Greater than
Either (B) or (C)
Zero
Minimum
Maximum
None of these
Non-equilibrium
Partial equilibrium
Full equilibrium
Unpredictable
r/2
2r/3
r/A
3r/2
Lie
Do not lie
Either A or B
None 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
g (m1 - m2)/(m1 + m2)
2g (m1 - m2)/(m1 + m2)
g (m1 + m2)/(m1 - m2)
2g (m1 + m2)/(m1 - m2)
v
2v
4v
8v
P = mW - C
P = m/W + C
P = mW + C
P = C - mW
Translatory motion
Rotational motion
Combined translatory and rotational motion
None of the above
0.5 cm
1.0 cm
1.5 cm
2.5 cm
Distance moved by effort to the distance moved by load
Load lifted to the effort applied
Output to the input
All of the above
W sinθ
W cosθ
W tanθ
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
Kinetic friction
Limiting friction
Angle of repose
Coefficient of friction
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
1/m
V.R./m
m/V.R.
1/(m × V.R.)