A child of mass 25 kg stands at the edge of a rotating platform of mass 150 kg and radius 4.0 m. The platform with the child on it rotates with an angular speed of 6.2 rad/s. The child jumps off in a radial direction (i.e. has no tangential velocity in the inertial frame of an outside observer). What happens to the angular speed of the platform? Treat the platform as a uniform disk. Give a quantitative explanation.

Solution:

- Concepts:

Conservation of angular momentum - Reasoning:

The angular momentum of two interacting objects is constant. - Details of the calculation:

(I_{platform}+ I_{child})ω_{i}= I_{platform}ω_{f}.

I_{platform}= ½ 150kg (4m)^{2}= 1200 kgm^{2}, I_{child}= 25kg (4m)^{2}= 400 kgm^{2}.

ω_{f}= 8.27 rad/s.

A 60 kg woman stands at the rim of a horizontal turntable having a moment of
inertia of 500 kgm^{2}, and a radius of 2 m. The turntable is
initially at rest and is free to rotate about a frictionless vertical axis
through its center. The woman then starts walking around the rim clockwise
(as viewed from above the system) at a constant speed of 1.5 m/s relative to the
Earth.

(a) In what direction and with what angular speed does the
turntable rotate?

(b) How much work does the woman do to set herself
and the turntable in motion?

Solution:

- Concepts:

Conservation of angular momentum - Reasoning:

The system consists of the woman and the turntable. No external torques act on the system, so the total angular momentum of the system is conserved. It is zero before the woman starts to walk, and it is zero afterwards. - Details of the calculation:

(a) When the women walks with angular velocity**ω**= -(v/r)**k**= -((1.5 m/s)/(2 m))**k**= -(0.75/s)**k**,

her angular momentum is

**L**= I**ω**= (-60 kg 4 m^{2 }0.75/s)**k**= -(180 kgm^{2}/s)**k**.

The angular momentum of the turntable will be**L**= (180 kgm^{2}/s)**k**,

its angular velocity**ω**= (180 kgm^{2}/s)k/(500 kgm^{2}) = (0.36/s)**k**. The turntable rotates counterclockwise.

(b) The kinetic energy of the women is ½Iω^{2 }= ½240 kgm^{2}(0.75 s)^{2 }= 67.5 J.

The kinetic energy of the turntable is ½Iω^{2 }= ½500 kgm^{2}(0.36 s)^{2 }= 32.4 J.

The work done by the women is W = (67.5 + 32.4) J = 99.9 J.

A mass M is attached to the end of a string which passes through a hole in a
frictionless horizontal plane. Initially the mass moves on a circle of radius R
with kinetic energy T_{0}. The string is then slowly pulled so that the
mass finally rotates on a circle of radius R/3. How much work was done?

Solution:

- Concepts:

Conservation of angular momentum - Reasoning:

We have a force directed towards the center of the orbit. Therefore the torque is zero. - Details of the calculation:

Initial angular momentum: L_{i}= mRv_{0}= mR(2T_{0}/m)^{½}.^{ }Final angular momentum: L_{f }= mRv_{f}/3 = m(R/3)(2T_{f}/m)^{½}.^{ }Conservation of angular momentum: L_{i}= L_{f},

mR(2T_{0}/m)^{½}= m(R/3)(2T_{f}/m)^{½}, T_{0}= T_{f}/9, T_{f}= 9 T_{0}._{ }Work done: T_{f}- T_{0}= 8 T_{0}.

A small ball swings in a
horizontal circle at the end of a cord of length L_{1} which forms an
angle θ_{1} with the vertical.
Gravity is acting downward. The cord is slowly shortened by pulling it through
a hole in its support until the free length is L_{2} and the ball is
moving at an angle θ_{2} from
the vertical.

(a) Derive a relation between
L_{1}, L_{2}, θ_{1}, and θ_{2}.

(b) If L_{1} = 50 cm, θ_{1} = 5^{o}, and L_{2}
= 30 cm, find θ_{2}.

Solution:

- Concepts:

Conservation of angular momentum - Reasoning:

The applied force produces no torque. - Details of the calculation:

Initial motion: T_{1}cosθ_{1}= mg, T_{1}sinθ_{1}= mv_{1}^{2}/r = mv_{1}^{2}/(L_{1}sinθ_{1}),

v_{1}^{2}= gL_{1}sin^{2}θ_{1}/cosθ_{1}.

Final motion : v_{2}^{2}= gL_{2}sin^{2}θ_{2}/cosθ_{2}.

Conservation of angular momentum: mL_{1}sinθ_{1}v_{1}= mL_{2}sinθ_{2}v_{2}, L_{1}^{2}sin^{2}θ_{1}v_{1}^{2}= L_{2}^{2}sin^{2}θ_{2}v_{2}^{2}.

Therefore L_{1}^{3}sin^{3}θ_{1}tanθ_{1}= L_{2}^{3}sin^{4}θ_{2}tanθ_{2}.

(b) Small angle approximation

L_{1}^{3}θ_{1}^{4}= L_{2}^{3}θ_{2}^{4}, θ_{2}^{4}= 2.68*10^{-4}, θ_{2}= 0.128 rad = 7.33^{o}.

A point mass m attached to the end of a string revolves in a circle of radius
R on a frictionless table at constant speed with initial kinetic energy E_{0}.
The string passes through a hole in the center of the table and the string is
pulled down until the radius of the circle is ½ of its initial value. Assuming
no external torque acts on the system, how much work is done?

Solution:

- Concepts:

Conservation of angular momentum - Reasoning:

A radial force does not exert a torque about the origin. - Details of the calculation:

E_{0}= ½mR^{2}ω^{2}, L = mR^{2}ω = (2mE_{0})^{½}R.

After the radius has been reduced to ½R, L = (2mE_{f})^{½}R/2.

(2mE_{0})^{½}R = (2mE_{f})^{½}R/2. 4E_{0}= E_{f}. The work done on the system is 3E_{0}.

(Or, E_{0}= ½mv^{2}, L = mvR = mv_{f}R/2. So v_{f}= 2v, E_{f}= ½mv_{f}^{2}= 4E_{0}. W = 4E_{0}- E_{0}= 3E_{0}.)

A solid sphere toy globe of mass M and radius R rotates freely without
friction with an initial angular velocity **ω**_{0}. A bug of
mass m starts at one pole N and travels with constant speed v to the other pole
S along a meridian in time T. The axis of rotation of the globe is held
fixed. Show that during the time the bug is traveling the globe rotates
through an angle

Δθ = (πω_{0}R/v) (2M/(2M + 5m))^{1/2}.

Useful integral: ∫_{0}^{2π}dx/(a + b cosx) = 2π/(a^{2}
- b^{2})^{1/2}, (a^{2} > b^{2}).

Solution:

- Concepts:

Conservation of a component of the angular momentum - Reasoning:

The axis of rotation is held fixed, so external forces cannot be excluded. But holding an axis fixed cannot exert a torque about this axis. So the component of angular momentum about the axis of rotation is conserved. - Details of the calculation:

L_{z}= Iω = I_{0}ω_{0}= constant.

I_{0}= (2/5)MR^{2}, I = I_{0}+ mR^{2}sin^{2}φ.

I(t)ω(t) = [(2/5)MR^{2}_{ }+ mR^{2}sin^{2}φ](dθ/dt) = (2/5)MR^{2}ω_{0}.

constant speed: φ = vt/R.

(dθ/dt) = (2/5)MR^{2}ω_{0}/[(2/5)MR^{2}_{ }+ mR^{2}sin^{2}(vt/R)].

Δθ = ∫_{0}^{T}dt (2/5)MR^{2}ω_{0}/[(2/5)MR^{2}_{ }+ mR^{2}sin^{2}(vt/R)].

Change variables: x = 2vt/R, sin^{2}(x/2) = ½(1 - cosx), since ∫dx/(a + b cosx) is an integral found in integral tables and is given here..

Use vT/R = π.

Δθ = (Rω_{0}/v)∫_{0}^{2π}dx/[2_{ }+ (5m/M) sin^{2}(x/2)]

= (Rω_{0}/v)∫_{0}^{2π}dx/[2_{ }+ (5m/(2M))(1 - cosx)]

= (πRω_{0}/v)(2M/(2M + 5m))^{1/2}.

As m --> 0, Δθ --> πω_{0}R/v = ω_{0}T, which corresponds to the free rotation of the globe with angular speed ω_{0}.

A uniform spherical planet of radius a revolves around the sun in
a circular orbit of radius r_{0 }and angular velocity
ω_{0}. It rotates about its axis with
angular velocity Ω_{0} (period T_{0})
normal to the plane of the orbit. Due to tides raised on the planet by the
sun, its angular velocity of rotation is decreasing. Find an expression
which gives the orbital radius r as a function of the angular
velocity Ω of rotation and the parameters r_{0} and T_{0 }at any later or earlier time.