Mechanical advantage is greater than velocity ratio
Mechanical advantage is equal to velocity ratio
Mechanical advantage is less than velocity ratio
Mechanical advantage is unity
B. Mechanical advantage is equal to velocity ratio
4
8
16
20
g. cos² β/2u². sin (α + β). cos α
2u². sin (α + β). cos α/g. cos² β
g. cos² β/2u². sin (α - β). cos α
2u². sin (α - β). cos α/g. cos² β
bh3/4
bh3/8
bh3/12
bh3/36
Newton
erg
kg-m
joule
Inelastic bodies
Elastic bodies
Neither elastic nor inelastic bodies
None of these
v = u + a.t
s = u.t + ½ a.t2
v2 = u2 + 2a.s
All of these
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
Simple pendulum
Compound pendulum
Torsional pendulum
Second's pendulum
20 kg, -ve sense
20 kg, + ve sense
10 kg, + ve sense
10 kg, -ve sense
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
Horsepower
Joule
Watt
kg-m
h [(2a + b)/(a + b)]
(h/2) [(2a + b)/(a + b)]
(h/3) [(2a + b)/(a + b)]
(h/3) [(a + b)/(2a + b)]
g/2
g
√2.g
2g
(BD³/12) - (bd³/12)
(DB³/12) - (db³/12)
(BD³/36) - (bd³/36)
(DB³/36) - (db³/36)
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
N-m
m/s
m/s2
rad/s2
Purely translation
Purely rotational
Combined translation and rotational
None of these
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
P = W tanα
P = W tan (α + φ)
P = W (sinα + μcosα)
P = W (cosα + μsinα)
(2/3) Ml2
(1/3) Ml2
(3/4) Ml2
(1/12) Ml2
mr2/3
2mr2/3
2mr2/5
3mr2/5
Area of contact
Shape of surfaces
Strength of surfaces
Nature of surface
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
IP = IG + Ah2
IP = IG - Ah2
IP = IG / Ah2
IP = Ah2 / IG
h/2
J/3
h/6
h/4
Strain energy
Kinetic energy
Heat energy
Electrical energy
Less than
Equal to
More than
None of these
Equal to
Less than
Greater than
None of these
α = 45° + φ/2
α = 45° - φ/2
α = 90° + φ
α = 90° - φ
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