A gravity assist maneuver allows a spacecraft to increase its speed by flying by a moving planet, where the spacecraft gains velocity equal to twice the planet's velocity (VS2 = VS1 + 2*VP1) while the planet's velocity decreases by a negligible amount due to the spacecraft's much smaller mass.
Gravity Assist Speed Calculation: Physics Explained
Added:Gravity assist. It is a flyby maneuver around a moving planet to gain an increase in the speed of the spacecraft.
In this video, we will calculate how much speed the spacecraft can actually get. Here is the setup of the problem.
The positive direction of the coordinate system is going right. At T1, the spacecraft has a velocity of VS1 and it is going left. Its mass is MS. Also at T1, the planet has a velocity of VP1 and a mass of MP. At T2, the spacecraft completes the flyby and it has a velocity of VS2. Its mass does not change and it is still MS. The planet at T2 has a velocity of VP2. Its mass does not change and it is still MP. To calculate the speed of the spacecraft and the speed of the planet at t2, we need to write out the governing equations. Classical physics tells us that the energy between the spacecraft and the planet should be conserved. So we have the equation of the conservation of energy. We can also write out the equation of the conservation of momentum. Now we have two equations and two unknowns which are v2 and vp2.
Theoretically, we can calculate their values, but it's not quite straightforward. We need to use some tricks. Let's rearrange equation 1.1 and remove the 1/2 on both sides of the equation. Then do factoring operations to get equation 1.3, which is the key of the trick. Now, let's work on equation 2.1 and do a simple rearrangement to get equation 2.2. Then factor out the mass to get equation 2.3.
Now, if you compare equations 1.3 and 2.3, you will notice that they have two terms in common. By simply dividing equation 1.3 by 2.3, we get equation 1.4. Then we want to multiply equation 1.4 with the mass of the planet to get equation 1.5. Then by subtracting 2.2 from 1.5, we can eliminate VP2 and get equation 1.6.
In this equation, the only unknown is V S2, which means we have solved VS2. Now, let's just rearrange the equation to only have VS2 on the left side of the equation. This is the speed of the spacecraft at T2. Everything else on the right side of the equation is known. We will discuss this equation a bit more later. But before doing that, let's calculate the speed of the planet as well. The calculation is similar. We just need to start from equation 1.4. The difference here is to multiply equation 1.4 with MS and we get equation 1.5 prime. Then we can add equation 1.5 prime with 2.2 to get equation 1.6 prime. In this equation, the only unknown is VP2, which means we have solved VP2. Let's just rearrange the equation to have VP2 on the left side of the equation only. Everything else on the right side of the equation is known.
Now we have solved both the speed of the spacecraft and the speed of the planet.
But the equations look complicated.
Let's see whether we can simplify them.
We know that the mass of the spacecraft is much much smaller than the mass of a planet. If you divide MS by MP, it is almost zero. We rewrite the equation like this. Here we simply divide both the denominator and numerator by MP. We know MP / MP is 1 and MS / MP is 0. We rewrite the equation and get the final version of the equation for the speed of the spacecraft. We can also simplify the equation for the speed of the planet.
The trick is the same, dividing both the denominator and numerator by MP. Then we get our final version of the equation for the speed of the planet.
Looking at the simplified equations, it tells us that the speed of the spacecraft increases. It's the sum of its initial speed and twice the speed of the planet. While the speed of the planet virtually does not change, its speed actually decreases by a tiny tiny bit. If you look at the right side of the full equation for the speed of the planet, there is a negative term which is very very close to zero, but not exactly zero. This means the planet loses a tiny bit of its energy. This energy is transferred to the spacecraft.
So basically by flying by the planet, the spacecraft interacts with the gravitational field of the planet and extracts energy from it. Now let's bring back the images and look at the animation again. This flyby maneuver increases the speed of the spacecraft.
But what if the planet is moving in the other direction? Well, we can simply add the negative sign in the equation for the speed of the spacecraft. This new equation tells us that by flying by the planet this time the spacecraft will have its speed decreased. Now you have it. These are the two simple cases of gravity assist maneuver.
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