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Physics 307 simulate the Earth going around the Sun

创建日期：2024-07-15 18:11:19

所属分类：物理Physical

标签： Physics 307

simulate the Earth going around the Sun

Hello, dear friend, you can consult us at any time if you have any questions, add WeChat: THEend8_

you will simulate the Earth going around the Sun, and then generalize your work to other orbits. There is a hints section at the end.

To review the discussion in class: For an orbit in the x-y plane, you have four dynamical variables x, y, vx, and vy. The four differential equations that govern them arewhere M is the mass of the Sun.

Firstwe will pretend that the Earth is in an exactly circular orbit; this is approximately the case. If we measure distance in astronomical units and time in years,
- what initial conditions for the Earth’s position and velocity vectors will give a circularorbit with the correct radius, and
- what is the numerical value ofGM?
Write code that simulates the Earth’s orbit around the Sun using the leapfrog algo- rithm.(If you like, you can code Euler-Cromer-Aspel ) Animate your simulation.
Now,let’s check to see if the simulation is Since you put in initial conditions that are explicitly designed to simulate a planet orbiting in a circular orbit with a period of one year

(a)Doesyour planet stay at a fixed distance from the origin?

(b)Doesyour planet complete an orbit in one year?

(c)Does your planet’s orbit conserveenergy?

Remember, you will see some deviation from these ideals because of “finite timestep error”. That’s okay, as long as those errors get small as dt → 0.

I’ll let you test these things in any way you want.

The total energy per unit mass (“specific orbital energy”) is given by the sum of the potential and kinetic energy

Modify your code to display the energy on the screen as the animation runs. You can do this with the T animation command.

Modify your initial conditions to simulate a non-circular orbit, changing the initial velocityand position of the (Note that if the total energy becomes positive, the Earth will escape the Sun’s gravity.) What shape do these orbits take? At what part of the planet’s orbit does it move faster? Spend at least half an hour playing around with different initial conditions and seeing what happens, and write about that in your report. In particular, how does the planet move if the total energy is very negative? Small and negative? Small and positive?
With initial conditions appropriate for an elliptical orbit, modify Newton’s law of gravity a bit. Specifically, change the force law to Fg= ttMm, where s is some small Simulate your orbit again, ensuring that the planet leaves trails behind it. What happens?1
Finally, consider what happens if you move the Sun away from the origin. Suppose youput the Sun at coordinates (0.2, 3). Change your code to simulate orbits around a star not at the origin.

1It turns out there is some history here. In regions of very strong gravity, Einstein’s general relativity modifies the force from gravity in a similar way. The orbit of Mercury is close enough to the Sun that GR causes its orbit to precess about one percent of one degree every century; this was known to astronomers and unexplained at the time of Einstein. Einstein was aware of this, and concluded his paper introducing GR by pointing out that his correction to the law of gravity explains exactly the anomaly in the precession of Mercury’s orbit.

ComputingGM : Remember your freshman physics; what is v2/r? I know some of you took or taught Physics 211 with me or Physics 215 with Prof. Laiho; treat it as a

215 problem! If you’re not sure how to go about this, discuss with other students, but tell me how this goes on your report.)

Debugging: If something is wrong with…–Animation?Run your program without anim and see what it is printing out

–Thephysics (“planet disappears”): print out everything your algorithm is doing, and examine the very first step in (You can see output one page at a time with ./myprogram | less.

–Elliptical orbits: is your total energy positive ornegative?

Animation:

–You can make your planet leave behind a “trail” so you can visualize its orbit with the ct3 animation command. Its syntax is ct3 〈trail index〉〈x〉〈y〉〈z〉〈radius〉,where:

∗ 〈trail index〉 controls which trail you are adding to in this case you only want to leave behind one trail, so just set this to 0

∗ 〈(x,y,z)〉 is the location to draw the object. Since you are simulating orbits in the xy-plane, just set z to zero.

∗ 〈r〉 is the radius of the ball to draw.

–Sincethe Sun doesn’t move, you can draw it at the origin with the c3

–If your simulation runs too fast, reduce the timestep; if it runs too slowly, you candraw only one animation frame every 10, 100, timesteps. To do this you might write something like:

int steps=0, stepsperframe=10; ... for (loop over time...) { steps++; // note that this means the same as "steps=steps+1" if (steps stepsperframe) { <do anim things> } <do physics update (Euler-Cromer-Aspel, leapfrog, etc.)> }

Displayingthe energy (or whatever else) on the simulation: An example of an elaborate way to do this would be:

printf(“T 0.9 -0.9\n”);

printf(“Energy (U + V = E): e + e = e\n”,potential,kinetic,potential+kinetic);

(Notice that this is a two-line anim command: the first line (T 0.9 -0.9) instructs the computer to print some text at a specified point in the window, in this case near the top left. The second line contains the text to be printed.) Remember, the more information you have about what your code is doing, the more physics you can learn from it, and the easier it will be to fix bugs.

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