# Elliptical Trajectory, or Parabolic?

Discuss whether this statement is correct: “In the absence of air resistance, the trajectory of a projectile thrown near the earth’s surface is an ellipse, not a parabola.”

Is the above statement right?

To the best of my knowledge, a particle projected from the earth's surface follows a parabolic trajectory under constant acceleration (of course an approximation)

One of my friends pointed out that in case of variable acceleration, one which follows the inverse square law; the path is an ellipse.

So, what is correct? If it is indeed an ellipse, I'm having trouble deriving the equation of its trajectory. Could someone please post a solution, or method to derive the actual trajectory's equation?

P.S. If the parabolic trajectory is an approximation, then making appropriate changes in the equation obtained should yield a parabola's equation, right?

• The answer is that a very small portion of a curve that is not just a line, e.g. an ellipse, looks like a small portion of a parabola. This question already has an answer here: physics.stackexchange.com/q/97716/20427
– user87745
Commented Dec 8, 2017 at 7:27
• If the distance is short enough "straight line" is a good enough approximation of any curve to shoot somebody dead. So the question is actually "what is the real curve?", and the answer is "not pretty". Another question could be "what would the real trajectory of a projectile be in a universe with just a homogeneous spherical planet in vacuum, assuming the gun is massless?" Commented Dec 8, 2017 at 13:17
• If you really want to get pedantic, in "idealized" conditions the trajectory of a body under the influence of a single gravity field that can be modeled by a point mass is neither an ellipse nor parabola, but a geodesic. The math for geodesics is not that easy, so often we use an ellipse to model an orbit. An ellipse is not a function in one variable, so for short enough trajectories we simplify even further and use a parabola (which is a function in one variable) to model the trajectory. A parabola is an accurate enough model to hit targets with cannons and mortars, so it is used often. Commented Dec 8, 2017 at 19:22

A parabola and an ellipse are both conic sections, which can be constructed in a plane as all the points where the distances from some reference point (the "focus") and some reference line (the "directrix") have some ratio $e$ (the "eccentricity"). An ellipse has $0<e<1$ a parabola has $e=1$.

In a typical intro physics "Billy throws a baseball"-type problem, the distance between the focus and the directrix for the "parabolic" trajectory might be a few meters. If the trajectory is secretly an ellipse due to Earth's gravity, Kepler's Laws predict that the other focus of the ellipse is the Earth's center of mass, and symmetry requires the path goes only a few meters from that point as well. That means we can estimate the eccentricity directly. Using the standard notation,

By Klaas van Aarsen [GFDL or CC BY-SA 3.0], via Wikimedia Commons

we have semimajor axis $a$ about half of Earth's radius $\rm 10^{6.5}\,m$, the distance from the focus to the end of the ellipse $a-c$ of order a few meters, and eccentricity $$e = \sqrt{1-\frac{b^2}{a^2}} = \frac ca \approx 1 - \mathcal O\left(10^{-6}\right).$$

That's a very good approximation of a parabola. That also suggests that if you wanted to worry about the difference between a parabolic path and an elliptical path at the part-per-thousand level, you'd start to worry about paths where the distance between the path and the focus (or equivalently, for scaling purposes, the distance between the launching and landing points for your projectile) of a few kilometers or tens of kilometers. Which is, in fact, where you start to hear about people taking into account Earth's curvature in engineering projects --- for example a very long suspension bridge, where the towers cannot be both "all vertical" and "all parallel."

• And if you throw the object hard enough (escape velocity) its trajectory could be a parabola regardless... Commented Dec 8, 2017 at 14:57

If gravity is uniform - the force has the same magnitude and direction everywhere, the trajectory is a parabola. This is a very good approximation for trajectories that don't go very far.

But in fact the force is not perfectly uniform. It actually does point to the center of the earth. It is stronger nearer the center. The trajectory for this case is an ellipse.

A typical parabolic trajectory hits the ground before it gets very far. If it didn't, it would be a very long skinny ellipse.

A parabola is an infinitely long ellipse.

For typical trajectories that hit the ground quickly, parabolic and elliptical trajectories are almost identical.

The rotation of the earth does have an effect. From the point of view of an inertial observer floating in space, the initial velocity of a thrown rock is about the speed of rotation of the earth's surface at that latitude.

The earth rotates $360$ degrees in $1$ sidereal day = $85604.1$ sec, or about $0.0042$ degrees/sec. So gravity isn't quite uniform. It has tilted a bit by the end of the trajectory. But in a flight lasting only a couple seconds, it isn't enough to notice.

The observer in space sees an observer on the ground moving sideways at the speed of the earth's surface. The ground observer is following a circular path. In those few seconds, he deviates from a straight line at $0.0042$ degrees/sec. To a good approximation, he is moving at uniform speed on a straight line. This gives the same result as if he wasn't moving.

If the rock fell through the earth and orbited, it would follow an ellipse as seen by the space observer. It would not be as skinny as I had thought. To the observer on earth, the motion would look complicated.

So thanks to Peter for pointing this out.

• By "hit the ground quickly" do you mean that the earth doesn't rotate much while the projectile is in flight?
– MaxW
Commented Dec 8, 2017 at 4:50
• Could you please derive the equation of the ellipse? It'll be mathematically pleasing and reassuring Commented Dec 8, 2017 at 5:34
• See this for the derivation. Commented Dec 8, 2017 at 5:35
• @MaxW Good point. Relative to the reference system of the earth's gravitational center the projectile's path is neither an ellipse nor a parabola. (E.g. a gun bullet shot west may have almost no velocity in the direction of the actual shot and move only vertically towards the earth's center, at certain latitudes). Relative to the sun it's all drowned out anyway by the 30km/s orbital speed of earth. Etc. Commented Dec 8, 2017 at 13:14
• It is noteworthy that the real trajectory, even in vacuum, is also not an ellipse because of the inhomogeneous mass distribution and hence grvitational field anomalies of our planet. Just a few percent max, but still. Commented Dec 8, 2017 at 13:16

The current problem

The key Point here is “…thrown near the earth’s surface…”.

That sentence usually means:

1. Gravitational acceleration is constant and equal to $\rm g$.

2. The ground can be considered a flat surface and gravitational force is normal to the surface.

With this 2 conditions we assume gravity as a constant force only acting on the vertical ($\rm y$) direction, or

$$\rm F_{Gy}=mg=m \frac{d^2y}{dt^2} \tag{1}$$ $$\rm F_{Gx}=0=m \frac{d^2x}{dt^2} \tag{2}$$ Solving these 2 equations one gets $$y=\rm \frac{1}{2}gt^2+v_{0y}t+y_0 \tag{3}$$ And $$\rm x=v_{0x}t+x_0 \tag{4}$$

Which is the parameterized form of a parabola with time $\rm t$ as parameter.

However, this is just the local view of the problem, meaning that you are just considering short distances when compared to earth’s radius.

The general problem

Considering that earth is a spherical object, it is possible to demonstrate that it’s gravitational force is equivalent to the gravity of a point mass located at it’s center. The trajectories of objects moving as the result of such forces obeys Kepler’s laws, replacing the sun by the center of the round object.

Kepler’s first law says that such trajectories are in fact ellipses (one could demonstrate it by solving Newton’s second law, but I won't bother if you do that ;-)

The big difference here is that gravity is not considered constant neither in magnitude (it is inversely proportional to the distance from the object to the center of earth) nor in direction (it point towards the center all the time).

Therefore, before continuing the discussion with your friend, please make sure you guys decide whether to consider “…thrown near the earth’s surface…” or not.

PS: by "thrown near the earth’s surface" I'm assuming you mean short distances and altitudes, sorry if I'm wrong.

• Ah.. It seems that the parabolic flight is a significant figures argument. In other words the ellipse is so elongated and a near earth trajectory is such a small arc of the ellipse that a parabola will do. Correct?
– MaxW
Commented Dec 8, 2017 at 17:17
• ellipsis→ellipses. Ellipsis is another thing. Commented Dec 8, 2017 at 19:05
• @Ruslan. You’re right. Unfortunately this will happen when a person is not a native English speaker, I’ll edit it. But, you can always edit it ;-) Commented Dec 8, 2017 at 19:55
• @MaxW. When solving physics problems, one always have to make assumptions, and simplify things, otherwise the problem may end up having infinite degrees of freedom becoming impossible to solve. In this particular situation, it may or may not be the case. If you neglect earth’s curvature, the flat earth is the sin of the angle formed by the starting point, the ending point, and the center of earth. For small angles the sin of an angle becomes equivalent to the arc length. Commented Dec 8, 2017 at 20:22
• I didn't edit because the text in the image should also be fixed. It's a bit more work, while you might have the sources for the image, whatever they are, so it's easier for you. Commented Dec 8, 2017 at 20:37

When you see the usual claim that the path of a thrown object is a parabola in the absence of air resistance it is done with a flat earth and constant gravity. From those assumptions, you can derive that the path is a parabola. The difference between the ellipse and the parabola comes because the gravitational acceleration varies with distance from the center of the earth. Both are good approximations for reasonable speeds of throwing an object. At that level of approximation you can't tell the difference.

In Newtonian dynamics, orbits are conic sections like ellipses or parabolas in the correct gravitational field of a point mass. The orbit outside a spherically symmetric body is the same as the orbit around a point mass. If we regard the earth as spherically symmetric, as long as you can't throw an object with escape velocity the orbit will be elliptical, not parabolic. Note that we have two different parabolic trajectories in this discussion. One is parabolic in a coordinate system with flat ground and constant gravity. The other is parabolic relative to the CM of the earth and the projectile with proper Newtonian gravity. All that is required for a parabolic trajectory in the second is that the total energy be zero. The statement is true if 1) you assume the earth is spherically symmetric and 2) you can't throw an object with escape velocity. I would ask somebody making this statement to justify that the difference between the elliptical orbit and the flat ground constant acceleration parabola is greater than the error created by the asymmetries of the earth. I suspect that it is true, but it will be some work.

Lets take a very simple case that helps answer the question.

An object is "thrown out" from the International Space Station (which is "near" earth's surface and no air resistance). What is its trajectory? It should be obvious that it is elliptical. Therefore, the above quoted statement is correct.