### Video Transcript

In this video, weāre going to be
looking at escape speed. Escape speed is the speed at which
a projectile must be launched in order to escape from the gravitational pull of a
massive object such as a planet. For example, if this amateur
astronaut were to leave the ramp at escape speed, they would completely escape the
gravitational pull of the Earth. Although unfortunately for them, as
weāll find out later, they would have to be cycling at around 11,000 meters per
second in order to achieve this. In this video, weāll look at how we
can calculate escape speeds like this. And weāll also look at how the
motion of projectiles changes as their launch speed approaches escape speed.

So, to start off with, letās
consider exactly what it means for a projectile to escape the gravitational pull of
a planet. So, hereās a planet. And letās say that we have some
test mass which is initially at rest on the surface of the planet. Now, letās say that we project our
test mass directly away from the planet with some initial speed š£. Well, as anyone whoās ever thrown
an object in the air will attest to, would expect our test mass to travel away from
the planet before slowing down coming momentarily to a stop and then falling back
down to the surface of the planet. Now, if we were to increase the
initial speed š£ at which we projected our test mass, then weād see that once again
our object would travel away from the planet, this time, reaching a greater distance
before it stopped but then, once more, falling back down to where it started.

In fact, for a planetary mass of
big š and a test mass of little š, we know that there will always be an attractive
gravitational force between the two masses. And the size of this force is given
by this expression, where big šŗ is the gravitational constant equal to 6.67 times
10 to the negative 11 meters cubed per kilogram per second squared and š is the
distance between the centers of mass of the two objects. So, weāve seen that increasing the
speed at which we project our test mass away from the planet will increase its
maximum distance from the planet. But this equation makes it clear
that no matter how far away our test mass gets from the planet, it will always
experience some attractive force that pulls it back toward the planet.

Given this, we might start to
wonder whether it really is possible for our test mass to escape the gravitational
pull of the planet. However, looking at this equation,
we can see that the attractive force between the two masses is inversely
proportional to the distance between the masses squared. In other words, increasing the
distance between them decreases the attractive force. This means that if we could put an
infinite distance between our planet and our test mass, then the size of the
attractive force between them would be reduced to zero, at which point we could say
that itās escaped from the planet. In other words, in order for our
test mass to escape the gravitational pull of our planet, we would have to project
it from the planetās surface with sufficient speed that it could be carried to an
infinite distance.

So, how is this possible? Well, it turns out that this
question is easily answered if we consider how potential energy works in a radial
gravitational field such as the one that exists around our planet. The potential energy of the test
mass, šø p, when separated from the planetary mass by a distance of š is given by
this expression. Now, gravitational potential energy
is defined in such a way that when the separation between the two masses is
infinite, the gravitational potential energy is zero. And for any finite value of š, the
potential energy is negative. And to be precise, š is actually
the distance between the centers of mass of the two masses.

Now, it might seem strange to say
that an object can have a negative potential energy. However, throughout physics, we
often defined potential energies as negative to indicate something being bound to
something else. For example, in an atom, electrons
are often described as having negative potential energy to signify that theyāre
bound to the nucleus. In this case, our test mess having
a negative potential energy signifies that it is bound by gravitational attraction
to the planet. The fact that its gravitational
potential energy is negative signifies that we would have to give it energy in order
to free it, at which point its potential energy would be zero. And the way that we can do this is
by projecting our test mass at a certain speed, in other words, by giving it kinetic
energy.

So, if our test mass is initially
on the surface of the planet, we can work out how much energy weād need to give it
to free it from the planetās gravitational pull by writing down a simple equation to
show the energy changes that take place. The test mass initially has
potential energy šø p, and we want to give it just enough kinetic energy so that
itās freed from the gravitational pull of the planet. In other words, we want to increase
its overall energy to zero, signifying that itās no longer bound to the planet. In place of šø p, we can substitute
negative šŗ times big š times little š over š. And in place of the kinetic energy
šø k, we can substitute a half šš£ squared, where š£ is the speed at which we
project the test mass.

And so, we obtain this expression,
which we can rearrange by adding šŗ times big š times little š over š to both
sides. This shows us that the amount of
kinetic energy we would need to give our test mass in order to free it from the
gravitational pull of the planet is equal to the magnitude of its gravitational
potential energy. And solving this equation for š£
will tell us the escape speed. To do this, we can start by
dividing both sides of the equation by little š, which leaves us with a half š£
squared equals šŗ times big š over š. Then, to get rid of this fraction,
we can multiply both sides of the equation by two, giving us š£ squared equals two
šŗš over š. And finally, we can take the square
root of both sides of this equation to give us š£ equals the square root of two
times šŗ times big š over š.

So, there we have it. This equation tells us the escape
speed š£ for a projectile at distance š from the center of mass of an object with
mass capital š. And we can change the symbol š£ to
š£ sub e to signify that this is the escape speed. Now, any projectile will always
experience an attractive gravitational force pulling it back towards the object that
it was launched away from. And this force causes it to
accelerate towards that mass. However, a projectile traveling at
the escape speed will never experience a large enough attractive force to pull it
back towards the other mass, which enables the projectile to travel away
indefinitely.

One interesting thing we can notice
about this equation is that itās independent of the mass of the projectile, and itās
also independent of the angle at which that projectile is launched. In fact, the escape speed of a
projectile only depends on two things, the mass of the other object ā in this case,
a planet ā and its distance from the center of mass of this object ā in this case,
the radius of a planet. So, a relatively small projectile
traveling directly away from the planet and a relatively large object launched at a
tangent to the planetās surface would both have exactly the same escape speed. Note that, in this case, weāre
ignoring any gravitational interactions between our two projectiles.

In this example, the object
travelling directly away from the planet would follow a straight path and the
projectile launched parallel to the planetās surface would follow a curved path. However, both objects would be able
to travel an infinite distance away from the planet. Now, letās zoom in on the surface
of this planet and consider what the distanceātime graph would look like for a
projectile launched vertically at escape speed. Specifically, weāll have the
projectileās height on the š¦-axis, that is, its distance away from the surface of
the planet. And weāll put time on the
š„-axis.

For a projectile launched at escape
speed, we get a graph that looks something like this. We can see that initially the
gradient of the line is very steep and that this gradient decreases as time
passes. This indicates that initially the
height of the object is increasing at a very high rate, corresponding to a very high
speed, and at a later time the speed has decreased somewhat. However, the height continues to
increase indefinitely. Now, a distanceātime graph like
this might seem somewhat unusual for a projectile. Usually, projectile problems
involving an object that travels away from the ground but then dropped back down to
the ground. So, weāre used to seeing a certain
type of symmetrical curve like this one. And the mathematical name for this
type of curve is a parabola.

The distanceātime graph for a
projectile traveling at escape speed, however, is very much not a parabola. Even without looking at this curve
closely, the fact that itās not symmetrical means that it canāt be a parabola. This object just keeps getting
higher and higher as time goes on. The reason for this discrepancy is
that often when weāre looking at projectiles, weāre dealing with initial speeds that
are much lower than the escape speed. So, if we call the initial speed of
our projectile š¢, then we could say that š¢ is much less than the escape speed š£
e.

If we launch a projectile at a
relatively low speed like this, this means it only reaches a relatively low height
before falling back down to Earth. If we just look at this very small
length scale, we can see that the curvature of the planet in this region is actually
not very obvious. And in fact, a lot of the time when
we deal with projectiles, we can simplify our calculations by assuming that the
Earth is flat. Effectively for small length
scales, the gravitational field of the Earth is approximately uniform, which means
that the gravitational force acting on objects is approximately constant. In fact, in these cases, we often
calculate the gravitational force acting on an object simply by multiplying its mass
by a constant, lowercase š.

In fact, this is Just an
approximation that works for small length scales. And itās this approximation that
gives us our characteristic parabolic distanceātime graph for projectiles moving at
low speeds. In fact, we know that the
gravitational force experienced by a projectile is not constant. Planets have radial magnetic
fields, which means that the force decreases with increasing distance from the
planet, as given by this equation, leading to distanceātime graphs for projectiles
which are not parabola shapes. So, projectiles that are launched
at speeds much lower than the escape speed will have approximately parabola-shaped
distanceātime graphs. But as the launch speed of a
projectile starts to approach the escape speed, its distanceātime graph will deviate
more and more from a true parabola.

One other useful graph that we can
draw to show the behavior of our projectile is a graph of energy against time. And on this one set of axes, we can
represent both the kinetic energy, which weāll draw in red, and the gravitational
potential energy, which weāll draw in blue. Letās start by considering a
projectile whose initial speed is much less than the escape speed. And letās say that this projectile
is launched at time zero. In this case, this is what our
graph would look like.

Looking first at the red line
showing kinetic energy, we can see that at the instant the projectile is launched,
the kinetic energy takes a maximum value. As the projectile travels away from
the planet, its kinetic energy is converted into gravitational potential energy. So, we can see that over this time
interval the gravitational potential energy, which was initially at some negative
minimum value, increases to a maximum value. And the kinetic energy decreases to
zero. Itās important to note here that
because kinetic energy is converted directly into gravitational potential energy and
there are no other forms of energy loss in this system, the size of this change in
kinetic energy, which we could call Īšø k, is exactly the same as the size in the
change of the potential energy, which we can call Īšø p.

At this moment in time, the
gravitational potential energy takes a maximum value and the kinetic energy is
zero. This means that here the projectile
has reached the top of its trajectory. And after this, it starts to fall
back down to the ground. This means that gravitational
potential energy is converted back into kinetic energy. So, we see the gravitational
potential energy decreasing back down to its minimum value and the kinetic energy
increases back up to its initial value as it accelerates towards the ground. Finally, the projectile hits the
ground, at which point the kinetic energy decreases immediately to zero and the
gravitational potential energy has returned to its initial value.

Now, if we increase the initial
speed of this projectile but keep it lower than the escape speed, then our graph
instead looks like this. So, we can see that this isnāt
drastically different. Because the projectile is launched
to the highest speed, it has a higher initial kinetic energy. Because more kinetic energy is
being converted into gravitational potential energy, this means the maximum
gravitational potential energy is higher by a corresponding amount. And because this means the
projectile was launched further, the entire process takes a longer amount of
time.

Crucially, we can see that the
initial amount of kinetic energy given to the projectile is still smaller than the
magnitude of the gravitational potential energy. And we can recall that in order to
escape from the gravitational pull of a planet, our projectile needs kinetic energy
equal to the magnitude of the gravitational potential energy.

So, finally, letās now see what
this graph looks like when the initial launch speed is equal to the escape
speed. This time, we can see that the
initial kinetic energy of the projectile is equal in magnitude to the initial
gravitational potential energy. This means that the conditions are
met for the projectile to escape the gravitational pull of the planet. In other words, the projectile has
enough energy to travel to an infinite distance away from the planet. Kinetic energy is still being
converted into gravitational potential energy. But because the projectile is
effectively traveling to an infinite distance away, this will take an infinite
amount of time. So, on our graph, we simply see
that kinetic energy tends to a minimum value and gravitational potential energy
tends to a maximum value, but we never actually see them get there.

Okay, so far, in this lesson, weāve
seen how we can calculate the escape speed of a projectile and how we can represent
the trajectories of projectiles with various speeds on both distanceātime graphs and
energyātime graphs. Now weāre armed with this
information; letās try answering a practice question.

Europa is a moon of Jupiter that
has a mass of 4.80 times 10 to the power of 22 kilograms and a radius of 1,560
kilometers. At what speed would an object have
to be launched vertically off the surface of Europa in order to escape its
gravity? Give your answer to three
significant figures.

So, in this question, weāre
thinking about an object on the surface of one of Jupiterās moons, known as
Europa. And weāre being asked to find a
speed, letās call this š£, at which we could launch this object vertically off the
surface of Europa that would enable it to escape its gravity. Letās start by thinking about
exactly what it means for this object to escape Europaās gravity.

Well, our object on the surface of
Europa, or indeed any object on the surface of any planet, has a certain
gravitational potential energy šø p, which is given by this equation, where šŗ is
the gravitational constant, big š is the mass of the planet or moon in question ā
in this case, it would be Europaās mass ā little š is the mass of the object, and
š is the distance between the centers of mass of the two masses that weāre
considering. So, in this case, it would be the
distance between the center of mass of Europa and the center of mass of our
object.

Now, we can see that this potential
energy is negative. In physics, we use negative
potential energies to represent when something is bound to something else. For example, in this question, our
object is bound to Europa by a gravitational force. The fact that this is negative
represents the fact that we would need to give the object energy in order to free
it. Effectively, the magnitude of all
this is the amount of kinetic energy we would need to give our object in order for
it to be freed from the gravitational pull of Europa. So, we can say that our object will
escape the gravitational pull of Europa when its kinetic energy, given by a half
šš£ squared, is equal to šŗ times big š times little š divided by š.

Now, if we rearrange this
expression to make š£ the subject, we obtain this expression. This tells us the speed at which an
object must be launched in order to escape the gravity of some other mass,
represented by big š. The speed is known as the escape
speed. And itās often denoted as š£ sub
e. We can use this equation directly
to work out the escape speed of our object on Europa. In this case, the value of big š
is the mass of Europa, which weāre told is 4.80 times 10 to the power of 22
kilograms. And š in this equation is the
distance between the center of mass of our object and the center of mass of
Europa.

Now, we havenāt been given this
quantity exactly. However, we have been told the
radius of Europa is 1,560 kilometers. Because planets and moons are
pretty much spherical, this means that center of mass is located in the middle. And as long as our object isnāt too
big, its center of mass will be very close to the surface of Europa. This means that we can use the
radius of Europa as the distance between our two centers of mass. And since this value has been given
in kilometers, weāll multiply it by 1,000 to give us the value in meters.

Finally, the other value that we
need in our equation is šŗ, the gravitational constant. This has a value of 6.67 times 10
to the power of negative 11 meters cubed per kilogram per second squared. Substituting these three values
into our equation gives us this expression. And if we enter all of this into
our calculator, we obtain a value of 2,025.99 and so on meters per second, which to
three significant figures is 2,030 meters per second. This is the speed at which an
object with any mass would have to be launched off the surface of Europa in order to
escape its gravity. In other words, itās the escape
speed.

Letās finish with a summary of the
key points that weāve looked at in this video. Weāve seen that an object
travelling at or faster than a planetās escape speed will be able to escape that
planetās gravity and travel away from the planet indefinitely. Weāve seen that we can calculate an
objectās escape speed using this equation, where šŗ is the gravitational constant,
š is the mass of the planet that the object is traveling away from, and š is the
distance between the centers of mass of the object and the planet. Finally, we looked at positionātime
and energyātime graphs for projectiles traveling in a range of speeds. And we saw that the faster a
projectile is launched, the more the shape of its positionātime graph deviates from
a parabola. This is a summary of escape
speed.