Rocket Trip Name __Key___
Anne, Bev, Chuck, and Dean have created a space
travel scenario involving a rocket that accelerates at 32 ft/s2 for
40 years of travel. The trip includes
ten years of acceleration and then ten years of deceleration that will bring
the rocket to a stop some distance from Earth.
One of the objects of this assignment is to find out how far the rocket
traveled during this 20 year odyssey.
As soon as the rocket comes to a stop far from Earth,
it begins its trip back which is the reverse of the trip away from Earth. Ten years of accelerating toward Earth
followed by ten years of decelerating so that the rocket reaches Earth with
zero speed.
As mentioned in class, you are going to analyze the
trip by breaking it into 3650 short trips each lasting one day of rocket time. Therefore the unit of time for this problem
is one day and the unit of distance is 1 light-day, the distance light travels
in one day. These definitions insure
that the speed of light is one, c = 1 light-day/day.
1.
How many seconds in a day? Seconds in a Day = 86,400
The rocket starts each day in a new reference
frame that is moving with the rocket. The
rocket’s velocity in this frame starts at zero but slowly increases because the
rocket is accelerating at 32 ft/s2.
2.
After one day of accelerating, how
fast is the rocket moving in the local reference frame? Speed of Rocket = _2,764,800 = 2.7648 x 106
ft/sec = _1,885,091 mph.
(This will be a large velocity compared to the everyday velocities we are used
to.)
The speed of light is 1 ft/ns or 1,000,000,000
ft/s = 109 ft/s.
3.
After one day of travel in the local
reference frame, what is the speed of the rocket, U, as a fraction of the
speed of light? U = Speed of
Rocket/c = __0.00276_
light-day/day
Note that once the speed is written as a fraction
of the speed of light, it doesn’t seem nearly so large! Also notice that the speed has the same
numerical value in ft/ns, light-days/day, or light-years/year. That is the beauty of using velocities as
fractions of light speed.
The U found in question 3 is the value that will
be used in the addition of velocity formula in the table that you will create
for this assignment.
4.
Suppose we did not know anything about
Special Relativity and used the answer in question 3 to find the speed of the
rocket after 3650 days of accelerating.
What would we calculate for the rocket’s velocity after those 3650 days
of constant acceleration?
5.
The Velocity of the Rocket Ignoring Special
Relativity = 10.3 times the speed of
light.
6.
Any comments about your answer to
question 5?
Wow. Too bad Special Relativity does not allow the
rocket to go that fast!!
7.
Create an Excel spreadsheet with the
following columns:
|
Trocket |
Tearth |
Xearth |
Vstart |
Vend |
Vaverage |
ΔTearth |
ΔXsam |
a.
Trocket
starts at 0 and increases 1 day per row.
The first row corresponds to the rocket’s trip during day one. The second row corresponds to the rocket’s trip
during day two, etc.
b.
Tearth
starts at zero and increases by ΔTearth
each row.
c.
Xearth
starts at zero and increases by ΔXearth
each row.
d.
Vstart
is the velocity of the rocket with respect to Earth at the start of each day’s
trip. It is equal to zero in the first
row. In each subsequent row, it is equal
to the Vend from the previous row.
e.
Vend =
is the velocity of the rocket with respect to
earth at the end of each day. We learned
earlier in the class that the reasonable and obvious way to add velocities, Vend
=
,
is incorrect for velocities that are large compared to the speed of light. The U in the equation is your answer to
question 3, the rocket’s speed in the local reference frame after accelerating
for 1 day.
f.
Vaverage
= ![]()
g.
ΔTearth
= ΔTrocket /
but since ΔTrocket
= 1 day, ΔTearth = 1 /
days
h.
ΔXearth
= Vaverage ΔTearth
8.
Each new row is found by using the values in
the previous row. The table gets built
one row at a time. Excel is very content
to do the same calculations over and over again, row by row, for as many rows
as you want!
The tables below are there to help you get your
table straight before having Excel do the calculation for 3650 rows.
|
Trocket |
Tearth |
Xearth |
Vstart |
Vend |
Vaverage |
ΔTearth |
ΔXearth |
|
0 |
0 |
0 |
0 |
0.0028 |
0.0014 |
1 |
0.0014 |
|
1 |
1 |
0.0014 |
0.0028 |
0.005599956 |
0.004199978 |
1.000004 |
0.0042 |
|
2 |
2.000004 |
0.0056 |
0.005599956 |
0.008399824 |
0.00699989 |
1.000016 |
0.007 |
|
3 |
3.00002 |
0.0126 |
0.008399824 |
0.011199561 |
0.009799693 |
1.000035 |
0.0098 |
|
Trocket |
Tearth |
Xearth |
Vstart |
Vend |
Vaverage |
ΔTearth |
ΔXearth |
|
0 |
0 |
0 |
0 |
=+(D2+0.0028)/(1+D2*0.0028) |
=0.5*(D2+E2) |
=+(1-D2^2)^(-0.5) |
=+F2*G2 |
|
=+A2+1 |
=+B2+G2 |
=+C2+H2 |
=+E2 |
=+(D3+0.0028)/(1+D3*0.0028) |
=0.5*(D3+E3) |
=+(1-D3^2)^(-0.5) |
=+F3*G3 |
|
=+A3+1 |
=+B3+G3 |
=+C3+H3 |
=+E3 |
=+(D4+0.0028)/(1+D4*0.0028) |
=0.5*(D4+E4) |
=+(1-D4^2)^(-0.5) |
=+F4*G4 |
|
=+A4+1 |
=+B4+G4 |
=+C4+H4 |
=+E4 |
=+(D5+0.0028)/(1+D5*0.0028) |
=0.5*(D5+E5) |
=+(1-D5^2)^(-0.5) |
=+F5*G5 |
|
=+A5+1 |
=+B5+G5 |
=+C5+H5 |
=+E5 |
=+(D6+0.0028)/(1+D6*0.0028) |
=0.5*(D6+E6) |
=+(1-D6^2)^(-0.5) |
=+F6*G6 |
9.
After ten years of travel, or 3650
days, the rocket’s distance from earth is _4,290,596_
light-days or 11,755_
light-years.
10. After
ten years of travel, the earth-frame observer next to the rocket has a clock
that reads _4,290,958_ days
or _11,756_ years.
11. Earth
observers, using your answers to questions 7 and 8 to calculate the rocket’s
average velocity during the first ten years, get the average velocity to be _0.99991 or effectively 1.000 _.
12. When
rocket returns to Earth, the maximum distance from Earth was 23,510 light-years.
13. Upon
the rocket’s triumphant return, the Earth clock that read zero at the start of
the trip now reads _47,010_ years.
14. How
much Earth time elapsed during the 3650th day of the rocket’s
trip? (The rocket’s speed is as big as
it ever will be at the end of this day.) _11,859_
days or _32.5_ years!
15. How
does the rocket’s maximum distance compare to size of the Milky Way, our home
galaxy? About ¼ of the diameter of the Milky Way.
16. What
does that say about the technological feasibility of visiting other galaxies?
Chances
run between none and slim but slim depends on finding some way to overcome the
limitations established by the nature of space and time.