__Describing trajectories__

A circle of radius a rolls on a straight line in the positive x-direction. The trajectory y(x) of a given point P on this circle is a cycloid.

(a) Find the parametric representation x(y) of this cycloid.

(b) Find the length of the path of the point P, when the circle has completed
one revolution, i.e. when the center of the circle has traveled a distance 2πa.

Solution:

- Concepts:

Describing trajectories - Reasoning:

We are asked for the the parametric representation of the trajectore of a piont on a rolling circle. - Details of the calculation:

(a) Let X be the x-coordinate of the center of the circle and x and y the coordinates of the point P.X = aθ, x = X – a sinθ = a θ – a sinθ,

y = a – a cosθ.

θ = cos^{-1}((a - y)/a),

sinθ = (1 - cos^{2}θ)^{½}= ((2ay – y^{2})/a^{2})^{½}.

x = a cos^{-1}((a - y)/a) - (2ay – y^{2})^{½}.

(b) Let s denote the length of the path.

ds/dθ = [(dx/dθ)^{2}+ (dy/dθ)^{2}]^{½}.

(dx/dθ)^{2}= a^{2}(1 - cosθ)^{2}= a^{2}(1 + cos^{2}θ – 2cosθ),

(dy/dθ)^{2}= a^{2}sin^{2}θ.

ds = a(2 – 2cosθ)^{½}dθ.

cos2x = cos^{2}x – sin^{2}x = 1 - 2sin^{2}x , 1 – cosθ = 2sin^{2}(θ/2)

s = ∫_{0}^{2π }(a√2)(1 – cosθ)^{½}dθ = ∫_{0}^{2π }(2a) sin(θ/2)dθ = (4a) ∫_{0}^{π }sinx dx = 8a.

The length of the path is 8a.

__Kinematics (1D)__

A chipmunk is taking a sunbath 5.0 m^{ }away from its burrow. It
then decides to go jogging. ^{ }The chipmunk takes off and runs directly
away from the^{ }burrow, so that its velocity is inversely proportional
to the^{ }distance from the burrow. If the initial speed of the^{
}chipmunk is 2.0 m/s, how long would it take it^{ }to run 15.0 m?

Solution:

- Concepts

Kinematics - Reasoning:

The chipmunk moves along a straight line. We are given dx/dt = f(x). dt = dx/f(x). Integrate to find ∆t. - Details of the calculations

The chipmunk's velocity is v = a/(x + 5), with x measured in meters.

v(x = 0) = 2 m/s, so a = 10 m^{2}/s.

dx/dt = a/(x + 5), (1/a)(x + 5)dx = dt, (1/a)∫_{0}^{15}(x + 5)dx = ∆t.

∆t = (1/10)(225/2 + 75) s = 18.75 s

Laurel running at 10 m/s is 40 m behind Hardy when Hardy
starts from rest on his moped with an acceleration 1.0 m/s^{2}. How
long does it take for Laurel to catch up with Hardy?

Solution:

- Concepts:

Kinematics - Reasoning:

One person is moving with constant speed and the other with constant acceleration. - Details of the calculation:

For Hardy: x = ½at^{2}= (0.5 m/s^{2})t^{2}.

For Laurel: x = -40 m + vt = -40 m + (10 m/s)t.

Laurel catches up when (0.5 m/s^{2})t^{2}= -40 m + (10 m/s)t.

t^{2}- 20t + 80 = 0, t = (10 – √20) s = 5.53 s

At t = (10 + √20) s = 14.47 s Hardy catches up with Laurel.

You are traveling east at 30 miles per hour. You see a ball rolling onto the road and you break hard, because you are afraid that a child will come running after the ball. You come to a stop in 0.8 seconds. What is the direction of your average velocity in this short time interval? What is your average acceleration?

Solution:

- Concepts:

Kinematics - Reasoning:

Average acceleration:**a**= ∆**v**/∆t - Details of the calculation:

The direction of your average velocity is east. You are traveling east with decreasing speed until you come to a stop.

The change in your velocity is ∆**v**= v_{2}- v_{1 }= 0 - 30 mph east = -30 mph east = 30 mph west. Let us convert to SI units.

30 mph * 1609 m/mile *s 1 h/(3600 s) = 13.4 m/s.

Your average acceleration is ∆**v**/∆t = (13.4 m/s)/(0.8 s) west = 16.8 m/s^{2}west.

A mass m starting from rest slides without friction in the field of gravity from the top of a vertical diameter d of a circle, A, along a straight wire connecting A and a point on the circumference, B. The wire makes an angle θ with the diameter, as shown in the figure. Does the time it takes to slide from A to B depend on θ? Justify your answer.

Solution:

- Concepts:

Kinematics - Reasoning:

We are asked for the time it takes for an object to travel a given distance when it starts from rest and the acceleration is constant.

The distance x the mass m travels is found from x/2 = (d/2)cosθ.

The acceleration of the mass is a_{x}= g cosθ.

Kinematics: x = ½a_{x}t^{2}. - Details of the calculation:

The time t it takes for the mass to reach point B is

t = (2x/a_{x})^{½}= (2dcosθ/(gcosθ))^{½}= (2d/g)^{½}, independent of θ.

Two cars approach an^{ }intersection of two perpendicular roads as
shown. The velocities of^{ }the cars are v_{1} and v_{2}.

At the moment when^{ }car 1 reaches the intersection, the separation
between the cars^{ }is d.

What is the minimum separation between the
cars^{ }during this motion?^{ }

Solution:

- Concepts:

Kinematics - Reasoning:

Both cars move with constant velocity. - Details of the calculation:

Let t = 0 denote the time car 1 arrives at the intersection.

Then for the position of car 1 as a function of time we have x_{1}(t) = v_{1}t, y_{1}= 0.

For car 2 we have x_{2}= 0, y_{2}(t) = d + v_{2}t = d + (v_{2}/v_{1})x_{1}. In the problem it is not specified if d is positive or negative.

The separation between the cars is s = (x_{1}^{2}+ y_{2}^{2})^{½}.

s^{2}= (1 + (v_{2}/v_{1})^{2})x_{1}^{2}+ d^{2}+ 2d(v_{2}/v_{1})x_{1}._{ }ds^{2}/dx_{1}= 2(1 + (v_{2}/v_{1}))x_{1}+ 2d(v_{2}/v_{1}) = 0 --> x_{1}= -d(v_{2}/v_{1}) /(1 + (v_{2}/v_{1})^{2}),

s_{min}^{2}= (1 + (v_{2}/v_{1})^{2})x_{1}^{2}+ d^{2}+ 2d(v_{2}/v_{1})x_{1}= d^{2}/(1 + (v_{2}/v_{1})^{2}). s_{min}= |d|/(1 + (v_{2}/v_{1})^{2})^{½}.

A prankster drops a water-filled balloon out of a window. The balloon is released from rest at a height of 10 m above the ears of an innocent man who is the target. Then, because of a guilty conscience, the prankster shouts a warning after the balloon is released. The warning will do no good, however, if shouted after the balloon reaches a certain point, even if the man could react infinitely quickly. Ignoring the effect of air resistance on the balloon, determine how far above the innocent man's ears this point is. The speed of sound is 340 m/s.

Solution:

- Concepts:

Kinematics - Reasoning:

The sound has to reach the man before the balloon does. - Details of the calculation:

It takes sound t_{s}= (10/340) s to travel 10 m.

The balloon reaches the man in t_{b}= (2*10/9.8)^{½}s = 1.43 s.

If the warning is shouted later than a time t_{b}- t_{s}= 1.4 s after the balloon is dropped, the warning will reach the man after he is hit by the balloon. In time t_{b}- t_{s}the balloon has dropped a distance d = ½g (t_{b}- t_{s})^{2}= 9.6 m and is therefore a distance 40 cm above the man.

A boy wants to throw a can straight up and then hits it with a second can. He wants the collision to occur 4 m above the throwing point. In addition, he knows that the time he needs between throws is 3.0 second. Assuming that he throws the second can 3.0 seconds after he throws the first can and that he throws both cans with the same speed, what must the initial speed be? What are the speeds of both cans when they collide?

Solution:

- Concepts:

Kinematics, energy conservation - Reasoning:

The only force acting on a can after it leaves the boy's hand is gravity. The gravitational force is a conservative force. - Details of the calculation:

Energy conservation requires that the cans have the same speed when they collide.

The first can must be coming down, and the second can must be going up.

– (v_{0}– gt) = v_{0}– g(t – 3s), t = v_{0}/g + 1.5 s.

The cans collide after t = v_{0}/g + 1.5 s.

Their speed when they collide is v = –v_{0}+ gt = g(1.5 s) = 14.7 m/s.

If the collision occurs at a height of 4 m we need

½mv_{0}^{2}= ½mv^{2}+ mg(4 m), v_{0}^{2}= v^{2}+ g(8 m) = 294.49 m^{2}/s^{2}, v_{0}= 17.16 m/s.

A ball that is thrown upward near the surface of the earth with a velocity of 50 m/s will come to rest about 5 second later. If the ball were thrown up with the same initial velocity on Planet X, after 5 seconds it would still be moving upwards at nearly 31 m/s. The magnitude of the gravitational field near the surface of Planet X is what fraction of the gravitational field near the surface of the earth?

Solution:

- Concepts:

One-dimensional motion with constant acceleration - Reasoning:

We are given the velocity at t = 0 and t = 5 s and are asked to find the acceleration. - Details of the calculation:

v(t) = v_{0}+ at = v_{0}- g't. 31 m/s = 5 0 m/s - g'(5 s).

g' = 3.8 m/s^{2}. g'/g = 0.388.

A projectile launched from the ground explodes into three fragments of equal mass at the top point of the trajectory. One of the fragments lands t seconds after the explosion; two other fragments land simultaneously 2t seconds after the explosion. How high above the ground does the projectile explode?

Solution:

- Concepts:

Momentum conservation, kinematics - Reasoning:

Let h be the height above the ground at which the projectile explodes and v_{jy}(j = 1, 2, 3) the y-component of the velocity at the moment of the explosion for the three fragments. Label with 1 the fragment which lands after t seconds.

Since the landing time depends only on the y-component of the velocity at the moment of the explosion, we have v_{3y}= v_{2y}.

We then need only the equations for fragments 1 and 2, stating that at the landing time the y-coordinate will be zero.

h + v_{1y}t – ½gt^{2}= 0, h + 2v_{2y}t – 2gt^{2}= 0. - Details of the calculation:

Since the masses of the three fragments are equal, and the y-component of the projectile momentum at the moment of the explosion is equal to 0, momentum conservation requires

v_{1y }+ v_{2y}+ v_{3y}= v_{1y }+ 2v_{2y}= 0, v_{2y}= -½v_{1y}.

We have 3 equations for 3 unknowns, v_{1y}, v_{2y}, and h.

h + v_{1y}t – ½ gt^{2}= 0, h - v_{1y}t – 2gt^{2}= 0.

v_{1y}t – ½ gt^{2}= -v_{1y}t – 2gt^{2}, v_{1y}= -¾gt.

h = ¾gt^{2}+ ½gt^{2}= (5/4)gt^{2}.

A student in a boat wants to cross the river from point K to point L (see the diagram). The current of the river is v = 2.0 km/h; the speed of the boat in still water is u = 5.0 km/h. The river is a = 0.25 km wide; distance LM is b = 0.5 km (see the diagram). How long would the trip take?

Solution:

- Concepts:

Kinematics, frame transformations - Reasoning:

In the rest frame of the water, the student has to travel a distance b + vΔt into the –x direction and a distance a in the y direction in time Δt to move on a straight line path and to arrive in the minimum time.

We have: -v_{x}Δt = b + vΔt, v_{y}Δt = a, v_{x}^{2}+ v_{y}^{2}= u^{2}. - Details of the calculation:

These are 3 equations for 3 unknowns. Solve for Δt.

v_{y}= a/Δt. v_{x}^{2}= u^{2}- a^{2}/Δt^{2}.

v_{x}^{2}Δt^{2}= b^{2}+ v^{2}Δt^{2}+ 2bvΔt. (u^{2 }- v^{2})Δt^{2}- 2bvΔt - (a^{2 }+ b^{2}) = 0.

21Δt^{2}- 2Δt - 0.3125 = 0, with Δt in hours. Δt = 0.17858 h.

Two ferries leave from opposite sides of a river. They move with different speeds and meet 400 m from the left bank. Each continues to its destination, take 5 minutes to unload and load, and then starts the return trip. The ferries meet again 200 m from the right bank. How wide is the river?

Solution:

- Concepts:

Kinematics - Reasoning:

Kinematics gives us two expression for the ratio v_{B}/v_{A}, one for the initial and one for the return trip. Setting these equal to each other allows us to solve for the width W of the river. - Details of the calculation:

Let ferry B start from the left bank and ferry A start from the right bank.

v_{B}t_{1}= W – 400 m, v_{A}t_{1}= 400 m

v_{B}(t_{2}- 5 min) = 2W – 200 m, v_{B}(t_{2}– 5 min) = W + 200 m

v_{B}/v_{A}= (2W – 200 m)/(W + 200 m) = (W – 400 m)/(400 m)

Solve for W: W^{2}– (1000 m)W = 0, W = 1000 m