A perfectly uniform billiard ball at rest is struck by a cue at a height h.
This causes it to have an initial velocity v_{0} and an
initial angular velocity ω_{0}. How far will it go on
a surface with coefficient of friction μ before pure rolling sets in?

Solution:

- Concepts:

Sliding friction: F = mN, N = normal force. Friction opposes the relative motion.

Rolling: A definite relationship between linear and angular velocity is needed, and therefore a definite relationship between linear and angular momentum.

Newton's second law:**F**= d**P**/dt,**τ**= d**L**/dt. - Reasoning:

Friction acting at a point away from the CM results in a torque about the CM, thus changing linear as well as angular momentum.

Let**v**_{0}= v_{0}**i**and**ω**_{0}= ω_{0}**k**. The direction of the frictional force depends on v_{0}and ω_{0}. If they are both positive, then**F**= -mN**i**= -μmg**i**. Let us assume that this is the case. The friction results in Δ**p**= -Δp**i**, Δ**L**= -ΔL**k**. We need to find the time interval Δt after which the condition for rolling is satisfied and rolling sets in. The condition for rolling is

v(t) = -aω(t), or p(t)/m = -aL(t)/I, with**v**= v**i**and**ω**= ω**k**and**p**= p**i**and**L**= L**k**. - Details of the calculation:

**F**= -μmg**i**= m(dv/dt)**i**. dv/dt = -μg, v(t) = v_{0}- μgt.

**τ**= d**L**/dt = I(dω/dt)**k**= -μmga**k**. dω/dt = -μmga/I, ω(t) = ω_{0}- μmgat/I.

Now find the time t when v(t) = -aω(t).

v_{0}- μgt = -aω_{0}+ μmga^{2}t/I.

For a sphere I = (2/5)ma^{2}. Therefore v_{0}- μgt = -aω_{0}+ (5/2)μgt, (7/2)μgt = v_{0}+ aω_{0}.

t = (v_{0}+ aω_{0})/((7/2)μg) is the time when rolling sets in.

d = v_{0}t - ½μgt^{2}is the distance the ball has traveled before this time.Think about:

What is the relationship between h, v_{0}and ω_{0}?

mv_{0}= FΔt, Iω_{0}= (2/5)ma^{2}ω_{0}= aF sinaΔt, ω_{0 }= (5/2)v_{0}sina/a = (5/2)v_{0}(a-h)/a^{2}.

Therefore t = (v_{0}+ (5/2)v_{0}(a-h)/a)/((7/2)μg) is the time when rolling sets in.

What happens for different values of h?

A homogeneous thin rod of mass m and length 2a slides on a smooth, horizontal
table, one end being constrained to slide without friction in a fixed straight
line. It is initially at rest, with its extension normal to the line, when it
is struck at the free end with an impulse Q parallel to the line.

(a) Determine the initial motion of the rod.

(b) Show that the force exerted by the line on the rod is given by

Q^{2}sinθ/[ma((4/3) - sin^{2}θ)^{2}], where θ is the
angle between the rod and the line.

Solution:

- Concepts:

Newton's second law:**F**= d**P**/dt,**τ**= d**L**/dt. The linear and the angular motion are coupled by a constraint. - Reasoning:

The force delivering the impulse acts at a point away from the CM. This results in a torque about the CM. The force of constraint also acts away from the CM and therefore can produce a torque.

The impulse is in the x-direction. It will result in momentum**P**of the CM and angular momentum**L**about the CM. The force of constraint is in the y-direction. It can change the y-component of**P**and it can change**L**.

The y coordinate of the CM and the angular coordinate θ are linked by constraints. - Details of the calculation:

(a) initial motion of CM:= Q

P**i**,**V**= (Q/m)**i**, initial motion about CM:**L**= -Qa**k**,**ω**= -(Qa/I)**k**.

moment of inertia of the rod about the CM: I = 2(m/2a)∫_{0}^{a}r^{2}dr = ma^{2}/3.

(b) subsequent motion: There is no force in the x-direction, V_{x}= Q/m = constant.

There is a force in the y-direction which produces linear acceleration of the CM and angular acceleration about the CM.

d^{2}y/dt^{2}= -F/m, d**L**/dt = F cosθ a**k**= I(d^{2}θ/dt^{2})**k**.

Therefore d^{2}y/dt^{2}= -I(d^{2}θ/dt^{2})/(m cosθ a). (y is the y-coordinate of the CM.)

But y and θ are linked by constraints.

y = a sinθ, d^{2}y/dt^{2}= - a sinθ (dθ/dt)^{2}+ a cosθ (d^{2}θ/dt^{2}).

Therefore - a sinθ (dθ/dt)^{2}+ a cosθ (d^{2}θ/dt^{2}) = -I(d^{2}θ/dt^{2})/(m cosθ a),

d^{2}θ/dt^{2}= cosθ sinθ (dθ/dt)^{2}/[(4/3) - sin^{2}θ]

We are supposed to show that F = Q^{2}sinθ/[ma((4/3) - sin^{2}θ)^{2}].

Using F cosθ a**k**= I(d^{2}θ/dt^{2})**k**, we are supposed to show that d^{2}θ/dt^{2}= (Q^{2}/I)cosθ sinθ/[ma((4/3) - sin^{2}θ)^{2}].

[To solve this differential equation guess (dθ/dt) = A/((4/3) - sin^{2}θ)^{½}and verify the solution. This is an obvious guess, since the solution for F^{ }is given. A is determined from the initial conditions.

At θ = 90^{o}, dθ/dt = Qa/I = 3Q/ma = 3^{½}A. A = 3^{½}Q/ma.]

F = I(d^{2}θ/dt^{2})/[cosθ a] = [ma/(3cosθ)][A^{2}sinθ cosθ/((4/3) -sin^{2}θ)^{2}] = Q^{2}sinθ/[ma((4/3) - sin^{2}θ)^{2}]

A sphere of radius R, mass M, and radius of gyration k = (I/M)^{½ }
about any axis through its center rolls with linear velocity **v** on a
horizontal plane. The direction of motion is perpendicular to a vertical step
of height h, where h < R. The sphere and step are perfectly rough and
inelastic. Show that the sphere will surmount the step upon collision if v^{2}
> 2ghR^{2}(R^{2} + k^{2})/(R^{2} - hR + k^{2})^{2}.

Solution:

- Concepts:

Δ**P**=**F**Δt, Δ**L**=**τ**Δt, relationship between linear and angular momentum for rolling motion - Reasoning:

The sphere makes an inelastic collision with the step. It starts rotating about the pivot point. Its momentum and angular momentum change. The change in momentum and angular momentum are not independent of each other but are connected by the fact that the pivot point is fixed. - Details of the calculation:

Just after the sphere has contacted the pivot point it is rotating about the pivot point. Its kinetic energy is

T = ½MR^{2}(dα/dt)^{2}+ ½Mk^{2}(dα/dt)^{2}.^{ KE of motion of CM + KE of motion about CM }For the sphere to surmount the step we need T > Mgh just after the sphere has contacted the pivot point.

Right after contacting the step the magnitude of the momentum of the sphere is

MR(dα/dt) = Mv sinα - FΔt = Mv(R - h)/R - FΔt.

Here Mv sinα is the momentum component perpendicular to the direction from the pivot point to the center of the sphere from before the collision and FΔt is the impulse due to the tangential force F.

At the same time the magnitude of the angular momentum about the CM is

I(dα/dt) = Iv/R + FRΔt.

Here Iv/R is the angular momentum before the collision and FRΔt is the change in angular momentum because of the impulse.

We therefore can write FΔt = Mv(R - h)/R - MR(dα/dt) = (I/R)(dα/dt) - Iv/R^{2}.

Solving for (dα/dt) we have:

MR(dα/dt) = Mv(R - h)/R - (I/R)(dα/dt) + Iv/R^{2}.

(R^{2}+ k^{2})(dα/dt) = v(R - h + k^{2}/R), (dα/dt) = v(R^{2}- hR + k^{2})/[(R^{2}+ k^{2})R].

T = ½M(R^{2}+ k^{2})(dα/dt)^{2}> Mgh yields

½v^{2}(R^{2}- hR + k^{2})^{2}/[(R^{2}+ k^{2})R^{2}] > gh,

v^{2}> 2ghR^{2}(R^{2}+ k^{2})/(R^{2}- hR + k^{2})^{2}.

A man wishes to break a long rod of length l by hitting it on a rock. The end of the rod which is in his hand rotates without displacement as shown in the figure below.

The man wishes to avoid having a large force act on his hand at the time the rod hits the rock. Which point on the rod should hit the rock? (Ignore gravity).

Solution:

- Concepts:

Center of percussion - Reasoning:

When the rod hits the rock a distance x > l/2 from the point O, the rock exerts a force of magnitude F on the rod. This force causes the CM to accelerate backward with acceleration of magnitude dv/dt = F/m. (This causes the point O to accelerate backward with a = dv/dt.) The force also exerts a torque about the CM, which causes a ccw angular acceleration about the CM of magnitude dω/dt = F(x - l/2)/I. (This causes the point O to accelerate forward with a = (l/2)dω/dt.)

If x denotes the center of percussion, then the backward and forward accelerations exactly cancel. - Details of the calculation:

We want (l/2)dω/dt = dv/dt, or (l/2)F(x - l/2)/I = F/m, (l/2)(x - l/2) = I/m.

The moment of inertia of a rod about its CM is I = ml^{2}/12.

We want (l/2)(x - l/2)= l^{2}/12. x = 2l/3.

The rod should contact the rock a distance x = 2l/3 from the point O.

A uniform disk of radius R and mass M is spinning about its diameter with
angular velocity **ω**, as shown below. Located on the rim of the disk,
at an angle θ from the spin axis, is point P, and P is moving with speed v_{p}.
Point P is now suddenly fixed. Show that the subsequent linear speed v_{c}
of the center of the disk is v_{c }= v_{p}/5.

Solution:

- Concepts:

Newton's second law: Δ**P**=**F**Δt, Δ**L**=**τ**Δt - Reasoning:

To reduce the velocity of point P to zero, an impulse must be delivered. The force acts at a point away from the CM. This results in a torque and an angular impulse about the CM.

The impulse changes the momentum of the CM and the angular momentum about the CM in such a way that point P is at rest. This determines the magnitude of Δ**P**. The velocity of the CM is given by**v**_{c}= Δ**P**/M. - Details of the calculation:

The disk rotates about the z-axis. Assume that when it is aligned with the yz-plane the impulse is delivered to the point P on the rim, a distance y = Rsinθ from the z-axis and z = Rcosθ from the y-axis.

Δ**P**= FΔt**i**, Δ**L**=**r**× Δ**P**= -F R sinθ Δt**k**+ F R cosθ Δt**j**.

Just after the impulse, the momentum of the CM is Δ**P**and the angular momentum about the CM is= I

L_{z}ω**k**- F R sinθ Δt**k**+ F R cosθ Δt**j**.

The velocity of the point P after the impulse is v = (FΔt/M)**i**+ ω**r**= 0.

(FΔt/M)**i**- (1/I_{z})(I_{z}ω - F R sinθ Δt)R sinθ**i**+ (1/I_{y})(F R cosθ Δt)R cosθ**i**= 0.

For a disk of radius R we have:

I_{z}= I_{y}= 2∫_{0}^{R}∫_{0}^{π}rdrdφ(r sinφ)^{2}ρ = MR^{2}/4.

Therefore:

FΔt/M - ωR sinθ - FR^{2}sin^{2}θ Δt/(MR^{2}/4) + FR^{2}cos^{2}θ Δt/(MR^{2}/4) = 0.

FΔt = (M/5)ωR sinθ .

The speed of point P before the impulse is v_{p}= ωR sinθ.

Therefore FΔt = (M/5)v_{p}, v_{c}= FΔt/M = v_{p}/5.