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Transcript
CT9-4.A rock is released from rest at a point in space far from Earth, beyond the orbit of the Moon.
The rock falls toward the Earth and crosses the orbit of the Moon. When the rock is the same distance
from the Earth as the Moon, the magnitude of the acceleration of the rock is .. (Ignore the gravitational
force between the rock and the Moon.)
Pink: greater
Yellow: smaller Blue: the same as the acceleration of the Moon.
Moon
Earth
rock
Answer: The acceleration of the rock and the moon have the same magnitude. If the they are the same
distance from the center of Earth, they experience the same acceleration since the acceleration is
a
F 1 GM E m GM E

 2
m m r2
r
and this depends only on the distance r from the Earth's center.
As the rock falls toward the Earth, its acceleration is..
Pink: constant.
Green: not constant.
Answer: Not constant. As the rock falls, r decreases, and g increases.
CT9-5. Two satellites, A and B, are in circular orbit around the earth. The distance of
satellite B from the center of the Earth is twice that of satellite A. What is the ratio of the
magnitudes of the accelerations of A to B?
aA
 ....
aB
Pink: 1
Blue: 1/2
Green: 2
Purple: 1/4
Yellow: 4
B
A
a
Answer: A
aB
F
GM I
G
J
r Kr
H


F
GM I r
G
Hr J
K
2
A
2
B
2
A
 22  4
Qualitatively, the closer satellite will feel a larger
2
B
force of gravity and will thus have a larger acceleration. Both the force (F) and the
acceleration (F/m) of gravity vary as "one-over-r-squared" 1/r2. So if r doubles, the
acceleration changes by a factor of 4.
CT9-6. A planet in elliptical orbit around a star moves from the point in its orbit furthest
from the star to the closest point. The work done by the force of gravity during this
movement is:
Pink: zero
Green: Positive
Yellow: Negative.
The work is positive. The force of gravity from the Sun is centripetal (toward the center).
The force
 has a component along the direction of displacement.
W  F  r  F r cos  0
r
FSun
Also, the work-energy theorem saysWnet = KE. The work must be positive, since by
Kepler's second law, the planet moves faster (has higher KE) when it is nearer the Sun, so
KE>0.
The planet executes one complete orbit starting from point A and returning to A. The
work done by the force of gravity during this orbit is:
Pink: zero
Green: Positive
Yellow: Negative.
Answer: zero. The positive work done in the first half of the orbit is cancelled by the
negative work in the second half.
CT9-7 Kepler's third law states that the ratio
T2
r3
is a constant for all the planets. The
period T of the Earth is 1 year. An astronomical unit (1 A.U.) is defined as the mean
distance from the Earth to the Sun, therefore the mean Earth-Sun distance is 1A.U.
Consider an asteroid in circular orbit around the Sun with radius r = 2A.U. The period of
the asteroid is..
Pink: 2 years. Green: 3 years
Yellow: 22/3  1.59 years
Blue: 23/2  2.83 years.
Purple: None of these.
Answer: The constant (T2/r3) = (1yr)2/(1 AU)3= 1 yr2 AU-3 .
T2
 1, T2  r 3 , T  r 3/ 2  2 3/ 2 yr
r3
The point is that since T2/r3 is the same for all planets (says Kepler III), if we know the
value of T2/r3 for any planet, then we know it for all the planets. For the Earth, T2/r3 = 1,
so T2/r3 must equal 1 for all the planets.
CT9-8.
At time t=0, a satellite in circular orbit about the Earth is directly over Denver, 300 miles
above the city, and traveling eastward at 16,000 mph. At the same time, a rock is
released from rest 300 miles above the city, very near the satellite.
rock
satellite
Denver
True or False: at t=0+, the accelerations of the rock and the satellite are identical in
magnitude and direction.
Green: true
Pink: False
Answer: True! Remember: acceleration is not velocity; velocity is not acceleration. The
satellite and the rock have very different velocities, but that has NOTHING to do with the
acceleration. The acceleration of gravity = g = Fgrav/m = GME/r2 is the same for both the
rock and the satellite because they at the same location, and g only depends on the
location.