Arm of man
Pair of scissors
Pair of clinical tongs
All of the above
D. All of the above
kW (kilowatt)
hp (horse power)
kcal/sec
kcal/kg sec
Bodies having relative motion
Two dry surfaces
Two lubricated surfaces
Solids and liquids
Reversible machine
Non-reversible machine
Neither reversible nor non-reversible machine
Ideal machine
Kinetic friction
Limiting friction
Angle of repose
Coefficient of friction
Same
Half
Double
None of these
Downwards at its upper end
Upwards at its upper end
Perpendicular to the wall at its upper end
Zero at its upper end
Iω
Iω2
0.5 Iω
0.5 Iω2
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
0.1 N-m
1 N-m
10 N-m
100 N-m
a2/8
a3/12
a4/12
a4/16
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
y = (gx²/2u² cos²α) + x. tanα
y = (gx²/2u² cos²α) - x. tanα
y = x. tanα - (gx²/2u² cos²α)
y = x. tanα + (gx²/2u² cos²α)
[m₁ m₂/2(m₁ + m₂)] (u₁ - u₂)²
[2(m₁ + m₂)/m₁ m₂] (u₁ - u₂)²
[m₁ m₂/2(m₁ + m₂)] (u₁² - u₂²)
[2(m₁ + m₂)/m₁ m₂] (u₁² - u₂²)
mv2
mgv2
0.5 mv2
0.5 mgv2
P × OA
P × OB
P × OC
P × AC
sinθ
cosθ
tanθ
cosecθ
1 + m
1 - m
1 / m
m
g sinθ
g cosθ
g tanθ
None of these
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
A path, traced by a projectile in the space, is known as trajectory.
The velocity, with which a projectile is projected, is known as the velocity of projection.
The angle, with the horizontal, at which a projectile is projected, is known as angle of projection.
All of the above
The three forces must be equal
The three forces must be at 120° to each other
The three forces must be in equilibrium
If the three forces acting at a point are in equilibrium, then each force is proportional to the sine of the angle between the other two
(1/2π). √(l/g)
(1/2π). √(g/l)
2π. √(l/g)
None of these
D/(d₁ + d₂)
D/(d₁ - d₂)
2D/(d₁ + d₂)
2D/(d₁ - d₂)
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
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
ω.√(y² - r²)
ω.√(r² - y²)
ω².√(y² - r²)
ω².√(r² - y²)
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
Momentum and impulse
Torque and energy
Torque and work
Moment of a force and angular momentum.
Angle of friction
Angle of repose
Angle of banking
None of these
P = Q
Q = R
Q = 2R
None of these