
Page 100 - 101
1. Package has same initial velocity as plane's
velocity; since it is horizontal, no need
to resolve into vertical and horizontal components.
(a) Use free fall equations to find time.
(b) use time from part a to find horizontal
distance.
2. Again a horizontal initial velocity, but
here we have the information to find the
time in the horizontal dimension. Use speed
and horizontal distance to find time. In
that time, how far will something fall?
3. Here we have a launch angle other than
horizontal. Find vertical and horizontal
components of initial velocity. Here they
are the same, but this won't always be the
case. Using the vertical component, find
the time for the flight. Now using the horizontal
component, figure how far it will go in that
much time.
4. Plug and chug
5. Here you have to calculate the speed of
the earth as it orbits the sun: v = d/t
6.(a & b) Straight-ahead calculation
of centripetal acceleration and force except
for the units of the speed and the weight
is given and not the mass. (c) To find the
frictional force, you must realize just what
it is that provides the centripetal force
for the car to turn.
8. Remember, at the bottom of the circle
the string must provide the centripetal force
to make the stopper go in a circle plus support
the weight of the stopper. At the top, the
weight helps by providing some of the centripetal
force.
10. First find radial distance from center of earth using earth's radius. Next, find value of g at this altitude. Now, plug into the equation for critical velocity because that's how fast satellites travel.
Page 108
1. 1 revolution = 2 pi radians; 1 radian
= 57.3 degrees
2. See #1
3. Two answers here, one for the somersault
dive and one for the twisting dive.
4. Look up the rotational inertia equation
for a uniform sphere on p 105. Be careful
with the units of the information given.
5. (a) Find change in angular velocity. (b)
Use angular constant acceleration equations
on page 103.
7. The force asked for is the force that
creates the torque that changes the speed.
Find the angular acceleration, then use 2nd
law for rotation to find torque. Assume the
merry-go-round is a disk for the rotational
inertia. The applied force must be enough
to create the torque plus overcome the frictional
force. (325 N)
Page 124
7. Rotary work problem: calculate torque,
multiply times angular displacement. Watch
the units!
11. Rotary work must equal linear work in
this case. Weight times height equals torque
times angular displacement. Convert to revolutions.
Page 130
5. Assume the wheel is a thin ring. Refer
to p. 105 for rotational inertia. Be sure
all quantities are in fundamental units.
9. (a) Assume the earth is a solid sphere.
Get the mass and radius from p. 66. Assume
1 day = 24 hours. Calculate angular speed
in fundamental units. (b) Use 1.50 x 1011 m as the radius of the earth's orbit.
10. (a) Ball has both rotary and linear kinetic
energy. To find the rotary energy, use the
rotational inertia for a solid sphere found
on page 105. Express angular velocity in
terms of linear velocity and radius. When
rotational inertia and angular velocity spuared
are multiplied together, the radius cancels
out and is therefore not necessary for the
problem. (b) Ball will roll up the incline
until all kinetic energy is converted to
potential energy. Set these quantities equal
and solve for h. Remember, this is the vertical height,
not the distance up the plane. Use trig to
find the distance.
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