y = (gx²/2u² cos²α) + x. tanα
y = (gx²/2u² cos²α) - x. tanα
y = x. tanα - (gx²/2u² cos²α)
y = x. tanα + (gx²/2u² cos²α)
C. y = x. tanα - (gx²/2u² cos²α)
(1 - sinφ)/(1 + sinφ)
(1 + sinφ)/(1 - sinφ)
(1 - tanφ)/(1 + tanφ)
(1 + tanφ)/(1 - tanφ)
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
Increase
Decrease
Not be effected
None of these
h/(kG² + h²)
(kG² + h²)/h
h²/(kG² + h²)
(kG² + h²)/h²
Equal to
Less than
Greater than
None of these
kg/cm
Bar
Atmosphere
Newton
Resultant couple
Moment of the forces
Resulting couple
Moment of the couple
D/(D - d)
D/(D + d)
2D/(D - d)
2D/(D + d)
Concurrence of the medians
Intersection of its altitudes
Intersection of bisector of angles
Intersection of diagonals
Halved
Doubled
Quadrupled
None of these
Lie on the same line
Meet at one point
Meet on the same plane
None of these
0.1 joule/s
1 joule/s
10 joules/s
100 joules/s
u² sin²α/2g
u² cos²α/2g
u² sin²α/g
u² cos²α/g
Nine times
Six times
Four times
Two times
Towards the wall at its upper end
Away from the wall at its upper end
Upwards at its upper end
Downwards at its upper end
Force
Work
Power
Velocity
In the shaded area
In the hole
At O
None of these
0° and 180°
180° and 0°
90° and 180°
90° and 0°
Composition
Resolution
Decomposition
None of these
The C.G. of a circle is at its centre
The C.G. of a triangle is at the intersection of its medians
The C.G. of a rectangle is at the intersection of its diagonals
The C.G. of a semicircle is at a distance of r/2 from the centre
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
Angle of friction
Angle of repose
Angle of projection
None of these
W sinθ
W cosθ
W tanθ
W cotθ
Iω
Iω2
0.5 Iω
0.5 Iω2
Meet
Do not meet
Either A or B
None of these
ω/2π
2π/ω
2π × ω
π/ω
The algebraic sum of the forces, constituting the couple is zero
The algebraic sum of the forces, constituting the couple, about any point is the same
A couple cannot be balanced by a single force but can be balanced only by a couple of opposite sense
All of the above
Directly
Inversely
Square root
None of these
Friction
Limiting friction
Repose
Kinematic friction
Second moment of force
Second moment of area
Second moment of mass
All of these