-
- [Voiceover] Two identical
spheres are released from
-
a device at time equals
zero, from the same height H,
-
as shown above, or T
equals zero I should say.
-
Sphere A has no initial velocity
and falls straight down.
-
Sphere B is given an initial
horizontal velocity of
-
magnitude V sub zero, and
travels a horizontal distance D
-
before it reaches the ground.
-
The spheres reach the ground
at the same time T sub F,
-
even though sphere B has more distance
-
to cover before landing.
-
Air resistance is negligible.
-
The dots below represent spheres A and B.
-
Draw a free-body diagram
showing and labeling the forces,
-
not components, exerted on each sphere
-
at time T sub F over two.
-
So we can see our spheres here,
-
when I guess this little
this thing releases,
-
sphere A goes straight down.
-
Sphere B, it it will
go, well it's vertical,
-
and the vertical direction,
it'll go down just the same way.
-
It'll be accelerated in just
the same way as sphere A,
-
but it has some horizontal
velocity that makes it move out
-
and hit the ground D to the right.
-
And when it hits the
ground, that's T sub F.
-
When they're up here, that's
right when they're released,
-
it's T equals zero, and then
this is at T equals T sub F.
-
And they say a free-body
diagram at T sub F over two.
-
So this is while both
of them are in flight.
-
So while both of them are in flight,
-
the only force acting on each of them,
-
is just going to be the force of gravity.
-
And since the spheres are identical,
-
the force of that gravity
is going to be identical.
-
They have the same mass, so let me draw.
-
So that right over there
is the force of gravity
-
on sphere A, and that is
the force of gravity on
-
sphere B.
-
And so we could write, force of gravity,
-
force of,
-
force of gravity.
-
And if we want, we could,
we could say the magnitude
-
is F sub G, if we want. F sub G.
-
Or we could label it as M
times the gravitational field.
-
So this is equal to,
-
is equal to M times the
gravitational field.
-
And that's it, while they're mid flight,
-
the only force acting on them,
-
we're assuming air
resistance is negligible,
-
is the force of gravity's
going to be the same because
-
they have the same mass,
they're identical spheres.
-
Alright, let's tackle
the next part of this.
-
On the axes below,
sketch and label a graph
-
of the horizontal components
of the velocity of sphere A
-
and of sphere B as a function of time.
-
Alright, I'll do sphere A first.
-
This is pretty straight forward.
-
Sphere A, if you will
remember, let's go up here.
-
Sphere A has no horizontal
velocity the entire time
-
we're talking about it, it only,
-
it's only going to be accelerated
in the vertical direction.
-
It's going to be accelerated downwards.
-
So sphere A has no horizontal velocity,
-
so I will draw a line like this.
-
So sphere A has no horizontal
velocity the entire time.
-
Now sphere, sphere B,
-
sphere B is going to be
-
a little bit more interesting,
slightly more interesting.
-
It's velocity, they tell us,
that it's initial velocity is
-
V sub zero, it's initial
horizontal velocity I should say,
-
has a magnitude of V sub zero.
-
And since air resistance is negligible,
-
it's gonna continue going
to the right at V sub zero
-
until it hits the ground.
-
So, so sphere B, this is,
-
and I'm just gonna pick
one of these as V sub zero.
-
Let's say that this right
over here is V sub zero.
-
That's the magnitude of
it's horizontal velocity.
-
Well sphere B is going
to be at that velocity,
-
actually let me just make
it a little bit clearer.
-
It's gonna be at that
velocity until, until V F.
-
So if we say this right
over here, or not V F,
-
until the final time, until T F.
-
So this is T equals zero to T F.
-
The entire time while the ball's in the,
-
while that sphere is in the air,
-
it's going to have the
horizontal component
-
of its velocity is just
going to be constant.
-
It's not going to be
slowed down by anything
-
because we're assuming air
resistance is negligible.
-
And then right when it hits the ground,
-
it essentially, if you
think about the force
-
that is stopping it is
essentially friction,
-
but then it very quickly
goes down to a velocity of a
-
a magnitude of velocity,
-
of horizontal magnitude velocity of zero.
-
Alright, alright now let's
tackle the last part of this.
-
Now you could label this if you want,
-
this is, let me actually let me label it,
-
this is B, sphere B, and this is sphere,
-
that is sphere A right over there.
-
In sphere B if you want, you could show,
-
it would overwrite sphere A, so your B
-
would be zero after that.
-
It's not continuing to
move on to the right,
-
or at least they don't tell
us anything about, about that.
-
Finally, in a clear, coherent, paragl
-
(laughs)
-
clear, coherent,
paragraph-length response,
-
explain why the spheres reach
the ground at the same time
-
even though they travel
different distances.
-
Include references in your
answers to parts A and B.
-
Alright, so let me think about it.
-
I'll try to write a clear, coherent,
-
paragraph-length response.
-
So I'll say, the entire time the,
-
or let me say from,
-
from T equals zero...
-
to T equals T sub F,
-
the only force
-
acting on the spheres
-
is the downward force of gravity.
-
Is the downward force,
-
force of (mumbles) of gravity.
-
At T equals zero,
-
at T equals zero, they both,
-
they both have zero vertical velocity or
-
the magnitude of the velocity
in the vertical direction
-
is zero for both of em.
-
Let me write it that way.
-
The, the magnitude
-
of both of their velocities,
-
both of their velocities,
-
velocities,
-
in the vertical
-
direction
-
(writes sentence)
-
is zero.
-
After T equals zero,
-
they are accelerated,
-
they are accelerated at the same rate.
-
Accelerated
-
(writing)
-
at the same,
-
they're accelerated at the same rate.
-
so their vertical component of velocity,
-
their vertical
-
(writing)
-
component, components of velocity,
-
velocity are always the same.
-
Of velocity are always
-
(writing)
-
the same.
-
And they have the same
vertical distance to cover,
-
and they have the same,
-
(writing)
-
the same vertical distance to cover.
-
Vertical distance to cover.
-
So they hit the ground at the same time.
-
Let me make sure that makes sense.
-
After T equals zero, they are
accelerated at the same rate,
-
so their vertical
components of velocity are
-
always the same.
-
Let me, actually let me,
let me write this this way.
-
Since they have the same, since,
-
actually let me,
-
since they have the same
-
vertical distance to cover,
-
vertical distance to cover,
-
(writing)
-
they will hit the ground at the same time.
-
They will hit the ground
-
(writes sentence)
-
at the same time.
-
Same time.
-
They do have different
horizontal velocities,
-
but that does not affect their,
that does effect the time
-
their velocities or the distance
in the vertical direction.
-
They have different horizontal,
-
(writes sentence)
-
horizontal velocities,
-
but that
-
(writes sentence)
-
does not effect
-
the time in which they,
-
they cover the same vertical distance,
-
effect the time in which
-
(writes sentence)
-
they cover the same
-
vertical distance.
-
And you could write
something to that effect,
-
and you could also write
that yes, if you were to add
-
the components of spheres Bs velocities,
-
it would actually have a larger velocity
-
if you were to add the components.
-
If you're not thinking you needed
-
the horizontal or the vertical direction,
-
and so it does indeed cover
more distance and space
-
over the same amount of time.
-
But if you think about it just
in the vertical direction,
-
it's covering the same
distance, in the same time,
-
at any given point in time
in the vertical direction.
-
It actually has the same velocity
-
It's being accelerated in the same way
-
that starts off at, of
magnitude of velocity of zero.