Lectures on Physics has been derived from Benjamin Crowell's Light and Matter series of free introductory textbooks on physics. See the editorial for more information....

When you're done using an electric mixer, you can get most of
the batter off of the beaters by lifting them out of the batter with
the motor running at a high enough speed. Let's imagine, to make
things easier to visualize, that we instead have a piece of tape stuck
to one of the beaters.

(a) Explain why static friction has no effect on whether or not the
tape flies off.

(b) Suppose you find that the tape doesn't fly off when the motor
is on a low speed, but at a greater speed, the tape won't stay on.
Why would the greater speed change things?

2

Show that the expression |v|^{2}/r has the units of acceleration.

3

A plane is flown in a loop-the-loop of radius 1.00 km. The
plane starts out flying upside-down, straight and level, then begins
curving up along the circular loop, and is right-side up when it
reaches the top . (The plane may slow down somewhat on the way
up.) How fast must the plane be going at the top if the pilot is to
experience no force from the seat or the seatbelt while at the top of
the loop?

√

4

In this problem, you'll derive the equation |a| = |v|^{2}/r using
calculus. Instead of comparing velocities at two points in the particle's
motion and then taking a limit where the points are close
together, you'll just take derivatives. The particle's position vector
is

where and are the unit vectors along
the x and y axes. By the definition of radians, the distance traveled
since t = 0 is rθ, so if the particle is traveling at constant speed
v = |v|, we have v = rθ/t.

(a) Eliminate θ to get the particle's position vector as a function of
time.

(b) Find the particle's acceleration vector.

(c) Show that the magnitude of the acceleration vector equals v^{2}/r.

∫

5

Three cyclists in a race are rounding a semicircular curve.
At the moment depicted, cyclist A is using her brakes to apply a
force of 375 N to her bike. Cyclist B is coasting. Cyclist C is
pedaling, resulting in a force of 375 N on her bike Each cyclist,
with her bike, has a mass of 75 kg. At the instant shown, the
instantaneous speed of all three cyclists is 10 m/s. On the diagram,
draw each cyclist's acceleration vector with its tail on top of her
present position, indicating the directions and lengths reasonably
accurately. Indicate approximately the consistent scale you are using
for all three acceleration vectors. Extreme precision is not necessary
as long as the directions are approximately right, and lengths of
vectors that should be equal appear roughly equal, etc. Assume all
three cyclists are traveling along the road all the time, not wandering
across their lane or wiping out and going off the road.

Solution, p. 283

6

The amusement park ride shown in the figure consists of a
cylindrical room that rotates about its vertical axis. When the rotation
is fast enough, a person against the wall can pick his or her
feet up off the floor and remain "stuck" to the wall without falling.
(a) Suppose the rotation results in the person having a speed v. The
radius of the cylinder is r, the person's mass is m, the downward
acceleration of gravity is g, and the coefficient of static friction between
the person and the wall is µs. Find an equation for the speed,
v, required, in terms of the other variables. (You will find that one
of the variables cancels out.)

(b) Now suppose two people are riding the ride. Huy is wearing
denim, and Gina is wearing polyester, so Huy's coefficient of static
friction is three times greater. The ride starts from rest, and as it
begins rotating faster and faster, Gina must wait longer before being
able to lift her feet without sliding to the floor. Based on your equation
from part a, how many times greater must the speed be before
Gina can lift her feet without sliding down?

* Solution, p. 283

7

An engineer is designing a curved off-ramp for a freeway. Since
the off-ramp is curved, she wants to bank it to make it less likely that
motorists going too fast will wipe out. If the radius of the curve is r,
how great should the banking angle, θ, be so that for a car going at
a speed v, no static friction force whatsoever is required to allow the
car to make the curve? State your answer in terms of v, r, and g, and
show that the mass of the car is irrelevant.

Solution, p. 283

8

Lionel brand toy trains come with sections of track in standard
lengths and shapes. For circular arcs, the most commonly used
sections have diameters of 662 and 1067 mm at the inside of the outer
rail. The maximum speed at which a train can take the broader
curve without flying off the tracks is 0.95 m/s. At what speed must
the train be operated to avoid derailing on the tighter curve?

√

9

The figure shows a ball on the end of a string of length L
attached to a vertical rod which is spun about its vertical axis by a
motor. The period (time for one rotation) is P.

(a) Analyze the forces in which the ball participates.

(b) Find how the angle θ depends on P, g, and L. [Hints: (1)
Write down Newton's second law for the vertical and horizontal
components of force and acceleration. This gives two equations,
which can be solved for the two unknowns, θ and the tension in
the string. (2) If you introduce variables like v and r, relate them
to the variables your solution is supposed to contain, and eliminate
them.]

(c) What happens mathematically to your solution if the motor is
run very slowly (very large values of P)? Physically, what do you
think would actually happen in this case?

√

10

Psychology professor R.O. Dent requests funding for an experiment
on compulsive thrill-seeking behavior in hamsters, in which
the subject is to be attached to the end of a spring and whirled
around in a horizontal circle. The spring has equilibrium length b,
and obeys Hooke's law with spring constant k. It is stiff enough to
keep from bending significantly under the hamster's weight.

(a) Calculate the length of the spring when it is undergoing steady
circular motion in which one rotation takes a time T. Express your
result in terms of k, b, and T.

(b) The ethics committee somehow fails to veto the experiment, but
the safety committee expresses concern. Why? Does your equation
do anything unusual, or even spectacular, for any particular
value of T? What do you think is the physical significance of this
mathematical behavior?

√

11

The figure shows an old-fashioned device called a flyball governor,
used for keeping an engine running at the correct speed. The
whole thing rotates about the vertical shaft, and the mass M is
free to slide up and down. This mass would have a connection (not
shown) to a valve that controlled the engine. If, for instance, the
engine ran too fast, the mass would rise, causing the engine to slow
back down.

(a) Show that in the special case of a = 0, the angle θ is given by

where P is the period of rotation (time required for one complete
rotation).

(b) There is no closed-form solution for θ in the general case where
a is not zero. However, explain how the undesirable low-speed behavior
of the a = 0 device would be improved by making a nonzero.

*

12

The figure shows two blocks of masses m_{1} and m_{2} sliding
in circles on a frictionless table. Find the tension in the strings if
the period of rotation (time required for one complete rotation) is
P.

√

13

The acceleration of an object in uniform circular motion can
be given either by |a| = |v|^{2}/r or, equivalently, by |a| =
4π^{2}r/T^{2},
where T is the time required for one cycle. (The latter expression
comes simply from substituting |v| = circumference/T = 2πr/T
into the first expression.) Person A says based on the first equation
that the acceleration in circular motion is greater when the circle
is smaller. Person B, arguing from the second equation, says that
the acceleration is smaller when the circle is smaller. Rewrite the
two statements so that they are less misleading, eliminating the
supposed paradox. [Based on a problem by Arnold Arons.]