Q. 46. A solid body rotates about a stationary axis according to the law φ = at  bt^{3}, where a = 6.0 rad/s and b = 2.0 rad/s^{3}. Find:
(a) the mean values of the angular velocity and angular acceleration averaged over the time interval between t = 0 and the complete stop;
(b) the angular acceleration at the moment when the body stops.
Ans. Let us take the rotation axis as zaxis whose positive direction is associated with the positive direction o f the cordinate <p, the rotation angle, in accordance w ith the righthand screw rule (Fig.)
(a) Defferentiating φ (t) with respect to time.
From (1) the solid comes to stop at
The angular velocity
Sim ilarly for all values of t.
So,
So,
Hence
Q. 47. A solid body starts rotating about a stationary axis with an angular acceleration β = at, where a = 2.0.10^{2} rad/s^{3}. How soon after the beginning of rotation will the total acceleration vector of an arbitrary point of the body form an angle α = 60° with its velocity vector?
Ans. Angle a is related with wt and wn by means of the fomula :
(1)
where R is die radius of die circle which an arbitrary point of the body circumscribes. From die given equation is positive for all values of t)
Integrating within the limit
So,
and
Putting the values of w_{t} and w_{n} in Eq. (1), we get,
Q. 48. A solid body rotates with deceleration about a stationary axis with an angular deceleration where ω is its angular velocity. Find the mean angular velocity of the body averaged over the whole time of rotation if at the initial moment of time its angular velocity was equal to ω_{0}.
Ans. In accordance with the problem, β_{z} < 0
Thus where A: is proportionality constant
or, (1)
When ω = 0 , total time o f rotation
Average angular velocity
Q.49. A solid body rotates about a stationary axis so that its angular velocity depends on the rotation angle φ as ω = ω_{0} — aφ, where ω_{0} and a are positive constants. At the moment t = 0 the angle = 0. Find the time dependence of
(a) the rotation angle;
(b) the angular velocity.
Ans. We have
Integratin this Eq. within its limit for (φ) f
Hence (1)
(b) From the or by differentiating Eq. (1)
Q.50. A solid body starts rotating about a stationary axis with an angular acceleration β = β_{0} cos φ, where β_{0} is a constant vector and φ is an angle of rotation from the initial position. Find the angular velocity of the body as a function of the angle φ. Draw the plot of this dependence.
Ans. Let us choose the positive direction of zaxis (stationary rotation axis) along the vector
In accordance with the equation
Integrating this Eq. within its limit for
The plot is shown in the Fig. It can be seen that as the angle qp grows, the vector increases, coinciding with the direction of the vector reaches the maximum at then starts decreasing and finally turns into zero at φ = π. After that the body starts rotating in the opposite direction in a similar fashion (ω_{z} < 0). As a result, the body will oscillate about the position with an amplitude equal to π/2.
Q. 51. A rotating disc (Fig. 1.6) moves in the positive direction of the x axis. Find the equation y (x) describing the position of the instantaneous axis of rotation, if at the initial moment the axis C of the disc was located at the point O after which it moved
(a) with a constant velocity v, while the disc started rotating counterclockwise with a constant angular acceleration β (the initial angular velocity is equal to zero);
(b) with a constant acceleration w (and the zero initial velocity), while the disc rotates counterclockwise with a constant angular velo city ω.
Ans. Rotating disc moves along the xaxis, in plane motion in x  y plane. Plane motion of a solid can be imagined to be in pure rotation about a point (say 7) at a certain instant known as instantaneous centre of rotation. The instantaneous axis whose positive sense is directed along the solid and which passes through the point/, is known as instantaneous axis of rotation.
Therefore the velocity vector of an aibitrary point (P) of the solid can be represented as :
(1)
On the basis of Eq. (1) for the C. M. (C) of the disc
(2)
According to the problem and plane, so to satisy the Hence point l is at a distance above the centre of the disc along y  axis. Using all these facts in Eq. (2), we get
(3)
(a) From the angular kinematical equation
(4)
On the other hand x = v t, (where x is the x coordinate of the C.M.)
or, t = x/y (5)
From Eqs. (4) and (5),
Using this value o f co in Eq. (3) w e get
(b) As centre C moves with constant acceleration w, with zero initial velocity
So,
Therefore,
Hence
Q. 52. A point A is located on the rim of a wheel of radius R = 0.50 m which rolls without slipping along a horizontal surface with velocity v = 1.00 m/s. Find:
(a) the modulus and the direction of the acceleration vector of the point A;
(b) the total distance s traversed by the point A between the two successive moments at which it touches the surface.
Ans. The plane motion of a solid can be imagined as the combination of translation of the C.M . and rotation about C.M.
is the position o f vector o f A with respect to C.
In the problem constant, and the rolling is without slipping
Using these conditions in Eq. (2)
Here, is the unit vector directed along
Hence or directed toward the centre of the wheel.
(b) Let the centre o f the wheel m ove toward right (positive jcaxis) then for pure tolling on the rigid horizontal surface, wheel will have to rotate in clockwise sense. If co be the angular velocity o f the wheel then
Let the point A touches the horizontal surface at t = 0, further let us locate the point A at t = ty
When it makes θ = ω t at the centre of the wheel.
H ence distance covered b y the point A during
Q. 53. A ball of radius R = 10.0 cm rolls without slipping down an inclined plane so that its centre moves with constant acceleration w = 2.50 cm/s^{2}; t = 2.00 s after the beginning of motion its position corresponds to that shown in Fig. 1.7. Find:
(a) the velocities of the points A, B, and 0;
(b) the accelerations of these points.
Ans. Let us fix the coordinate axis xyz as shown in the fig. As the ball rolls without slipping along the rigid surface so, on the basis o f the solution o f problem Q.52 :
At the position corresponding to that of Fig., in accordance with the problem,
and
(a) Let us fix the coordinate system with the frame attached with the rigid surface as shown in the Fig.
As point O is the instantaneous centre of rotation of the ball at the moment shown in Fig.
so,
Now,
So,
So,
Similarly
So,
Q. 54. A cylinder rolls without slipping over a horizontal plane. The radius of the cylinder is equal to r. Find the curvature radii of trajectories traced out by the points A and B (see Fig. 1.7).
Ans. Let us draw the kinematical diagram of the rolling cylinder on the basis of the solutioi of problem Q.53.
As, an arbitrary point of the cylinder follows a curve, its normal acceleration and radius of curvature are related by the well known equation
so, for point A,
or,
Similarly for point B,
or,
Q. 55. Two solid bodies rotate about stationary mutually perpendicular intersecting axes with constant angular velocities ω_{1} = 3.0 rad/s and ω_{2} = 4.0 rad/s. Find the angular velocity and angular acceleration of one body relative to the other.
Ans. The angular velocity is a vector as infinitesimal rotation commute. Then file relative angular velocity of the body 1 with respect to the body 2 is dearly.
as fo r relative lin ear velocity. The relative acceleration of 1 w.r.t 2 is
where S ' is a fram e corotating with the second body and S is a space fixed frame with origin coinciding with the point of intersection of the two axes,
but
Since S ' rotates with angular velocity as the first b ody rotates with constant angular velocity in space, thus
Note that for any vector relation in space forced frame (k) and a frame (Jd) rotating with angular velocity
Q. 56. A solid body rotates with angular velocity ω = ati + bt^{2}j, where a = 0.50 rad/s^{2}, b = 0.060 rad/s^{3}, and i and j are the unit vectors of the x and y axes. Find:
(a) the moduli of the angular velocity and the angular acceleration at the moment t = 10.0 s;
(b) the angle between the vectors of the angular velocity and the angular acceleration at that moment.
Ans. We have (1)
So,
D ifferen tia tin g E q. (1) with respect to time
(2)
So,
and
(b)
Putting the values of (a) and (b) and ' taking t =10s, we get
α = 17°
Q. 57. A round cone with halfangle α = 30° and the radius of the base R = 5.0 cm rolls uniformly and without slipping over a horizontal plane as shown in Fig. 1.8. The cone apex is hinged at the point O which is on the same level with the point C, the cone base centre. The velocity of point C is v = 10.0 cm/s. Find the moduli of
(a) the vector of the angular velocity of the cone and the angle it forms with the vertical;
(b) the vector of the angular acceleration of the cone.
Ans. Let the axis of the cone (OC) rotates in an ticlockw ise sense w ith constant angular velocity and the cone itself about it’s own axis (OC) in clockwise sense with angular velocity Then the resultant angular velocity of the cone.
(1)
As the rolling is pure the magnitudes of the vectors
can be easily found from Fig.
(2)
(b) Vector of angular acceleration
The vector which rotates about the OO' axis with the angular velocity retains i magnitude. This increment in the time interval dt is equal to
Thus
The magnitude of the vector
So,
Q. 58. A solid body rotates with a constant angular velocity ω_{0} = 0.50 rad/s about a horizontal axis AB. At the moment t = 0 the axis AB starts turning about the vertical with a constant angular acceleration β_{0} = 0.10 rad/s^{2}. Find the angular velocity and angular acceleration of the body after t = 3.5 s.
Ans. The axis AB acquired the angular velocity
(1)
Using the facts of the solution of 1.57, the angular velocity of the body
And the angular acceleration.
But
So,
1. What is kinematics? 
2. How is kinematics different from dynamics? 
3. What are the basic quantities in kinematics? 
4. How is average velocity calculated in kinematics? 
5. What is the difference between speed and velocity in kinematics? 

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