h/(kG² + h²)
(kG² + h²)/h
h²/(kG² + h²)
(kG² + h²)/h²
B. (kG² + h²)/h
2.√(gh)
√(gh)
√(2gh)
2g.√h
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.
Ellipse
Hyperbola
Parabola
Circle
The tangent of the angle of friction is equal to coefficient of friction
The angle of repose is equal to angle of friction
The tangent of the angle of repose is equal to coefficient of friction
The sine of the angle of repose is equal to coefficient to friction
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
v
2v
4v
8v
W sinθ
W cosθ
W tanθ
None of these
Static friction
Dynamic friction
Limiting friction
Coefficient of friction
Translatory
Rotary
Circular
Translatory as well as rotary
Translatory motion
Rotational motion
Combined translatory and rotational motion
None of the above
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
Equal to
Less than
Greater than
None of these
Potential energy
Kinetic energy
Power
None of these
20 N
40 N
120 N
None of these
(1 - sinφ)/(1 + sinφ)
(1 + sinφ)/(1 - sinφ)
(1 - tanφ)/(1 + tanφ)
(1 + tanφ)/(1 - tanφ)
Straight line
Parabola
Hyperbola
Elliptical
P = W tan (α - φ)
P = W tan (α + φ)
P = W tan (φ - α)
P = W cos (α + φ)
0.5r
0.6 r
0.7 r
0.8 r
Halved
Doubled
Quadrupled
None of these
W sinθ
W cosθ
W secθ
W cosecθ
These forces are equal
The lines of action of these forces meet in a point
The lines of action of these forces are parallel
Both (B) and (C) above
Reversible machine
Non-reversible machine
Neither reversible nor non-reversible machine
Ideal machine
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
25
50
100
250
tan(α + φ)/tanα
tanα/tan (α + φ)
tan(α - φ)/tanα
None of these
Rolling friction
Dynamic friction
Limiting friction
Static friction
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
g/2
g/3
g/4
None of these
Compression or tension
Buckling or shear
Shear or tension
All of the above
+8.9 m/s2
-8.9 m/s2
+9.8 m/s2
-9.8 m/s2