This homework set shouldn't require any use of a calculator. Homework solutions should be neatly typed, and be sure to fully explain your answers.
Kepler's third law applies here, since it's the one which includes orbital period and mass. We use the second (longer) form of the 3rd law, because Dactyl is orbiting Ida, rather than directly orbiting the Sun. Since we know the orbital period P, and we could measure the distance R between the two bodies, we could plug the numbers into Kepler's 3rd law and get the mass M1 out. From the pictures, it looks like Dactyl is a lot smaller in mass than Ida, so we can just ignore its mass (M2) entirely in the equation.
b) Let's assume Ida's mass suddenly doubled -- for instance, if it collided and merged with another asteroid. Would Dactyl suddenly begin to orbit with a longer period, or a shorter one?P2 = 4 pi2 A3 / (G (M1 + M2))
If M1 were to go up, P would have to go down to keep the equation balanced. P is the orbital period in seconds: smaller orbital period means that it orbits faster. You can also think of this intuituvely: if Ida's mass were to increase, its gravity could then pull stronger on Dactyl and accelerate it in a faster circle, just like turning a tighter corner in your car if you tug on the wheel a bit harder.
You might want to use a moon ball like we did in the planetarium - just stand in the right place, and the solution will pop out.
We did this exact problem in the planetarium: hold the moon in front of you, with the moon behind you, and you see a full moon. Spin your head around, and you'll see that when the moon just goes out of view, the sun is just coming into view: in other words, one sets when the other rises. If the sun rises at 6 AM and sets at 6 PM, the moon rises at 6 PM and sets at 6 AM. They're essentially never in the sky together. (In reality, in the summer the sun & moon are up for more than 12 hours as we saw in the planetarium, so they might be in the sky together for a couple of hours. Either way, they don't share the sky for 12 or 24 hours - more like 2 or 3 at most, and 0 hours is just fine too.)
If you move your head around in this configuration, you'll block the moon - lunar eclipse! Usually this doesn't happen every month because in the `real' solar system your head would be much smaller, and it's hard to get the Sun, Earth, & Moon to line up perfectly. You could not get a solar eclipse in the configuration - you'd have to wait two weeks for the Moon to move around the Earth until it could block the sun out.
Ptolemy's model had several problems:
However, it was held onto as a good model for over a millennium, in part because:
Although Copernicus didn't have Physics at his disposal, he did have Tycho Brahe's extremely accurate naked-eye observations of the planets' positions, and he critically analyzed whether these data could fit the Ptolemaic model or not. He concluded that, unfortunately, they could not, and then proposed - largely unprompted by earlier work - that many of the problems of the geocentric model could be solved with a sun-centered one.
You may find it helpful to get a globe (or some fruit), and think this one out. Once you're set up right, it's easy.
Just like if you stood on our North pole day after day and saw the same stars and Sun in the sky, standing on Uranus would give you the same view of the sky day after day as the planet rotates and you stand in place. Slowly, as Uranus moves through its orbit around the Sun, the Sun would appear lower & lower in the sky, until dipping below the horizon and staying there for a half an orbit: 42 years. You'd have a 42 earth-year long summer, followed by a 42 earth-year long winter. (Or, 21 years each of summer, fall, winter, spring.) Moreover, the sun would be up in the sky continually during the summer, and never rise once during the winter.
If you were standing on the equator, the stars would rise & set similar to how they do on Earth. Every day throughout Uranus' orbit, the Sun would rise and set - sometimes high in the sky and sometimes low, depending on the time of year.
See also figure 2.11 in the text.
Last modified 14-Jun-2000