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## High school physics

### Course: High school physics > Unit 3

Lesson 3: Graphs of projectile motion# Projectile motion graphs

Visualizing position, velocity and acceleration in two-dimensions for projectile motion.

## Want to join the conversation?

- Why is the second and third Vx are higher than the first one?(14 votes)
- All thanks to the angle and trigonometry magic.

After looking at the angle between**actual velocity vector**and**the horizontal component**of this velocity vector, we can state that:

1) in the second (blue) scenario this angle is zero;

2) in the third (yellow) scenario this angle is smaller than in the first scenario.

If above described makes sense, now we turn to finding velocity component. We do this by using cosine function:**cosine = horizontal component / velocity vector**. After manipulating it, we get something that explains everything!**horizontal component**=**cosine * velocity vector**

Now we get back to our observations about the magnitudes of the angles. If we work with angles which are less than 90 degrees, then we can infer from unit circle that**the smaller the angle, the higher the value of its cosine**.

So from our derived equation (horizontal component = cosine * velocity vector) we get that the higher the value of cosine, the higher the value of horizontal component (**important note**: this works provided that velocity vector has the same magnitude. In this case, this assumption (identical magnitude of velocity vector) is correct and is the one that Sal makes, too).

Now let's get back to our observations:

1) in blue scenario, the angle is zero; hence, cosine=1. This means that the**horizontal component is equal to actual velocity vector**. It actually can be seen - velocity vector is completely horizontal.

2) in yellow scenario, the angle is smaller than the angle in the first (red) scenario. This means that**cos(angle, red scenario) < cos(angle, yellow scenario**)! Hence, the horizontal component in the third (yellow) scenario is higher in value than the horizontal component in the first (red) scenario.(4 votes)

- At1:31in the top diagram, shouldn't the ball have a little positive acceleration as if was in state of rest and then we provided it with some velocity?(8 votes)
- maybe have a positive acceleration just before into air, once the ball out of your hand, there will be no force continue exerting on it, except gravitational force (assume air resistance is negligible), so in the whole journey only gravity affect acceleration.(9 votes)

- Why did Sal say that v(x) for the 3rd scenario (throwing downward -orange) is more similar to the 2nd scenario (throwing horizontally - blue) than the 1st (throwing upward - "salmon")? I would have thought the 1st and 3rd scenarios would have more in common as they both have v(y)>0.(6 votes)
- how the velocity along x direction be similar in both 2nd and 3rd condition?

(that is in blue and yellow)(4 votes)- Because there are no forces in that direction.(3 votes)

- At3:53, how is the blue graph's x initial velocity a little bit more than the red graph's x initial velocity?(5 votes)
- In this case/graph, we are talking about velocity along x- axis(Horizontal direction)

So, initial velocity= u cosӨ

For blue ball and for red ball Ө(angle with which the ball is projected) is different(it is 0 degrees for blue, and some angle more than 0 for red)

Now, assuming that the two balls are projected with same |initial velocity| (say u), then the initial velocity will only depend on cosӨ in initial velocity = u cosӨ, because u is same for both.

Now, let's see whose initial velocity will be more -

It'll be the one for which cos Ө will be more

For blue, cosӨ= cos0 = 1

For red, cosӨ= cos (some angle>0)= some value,say x<1

[because we know that as Ө increases, cosӨ decreases

cos(0)=1

therefore, cos(Ө>0)=x<1]

Now, we have,

Initial velocity of blue ball = u cosӨ = u*(1)= u

Initial velocity of red ball = u cosӨ = u*(x<1)= some value, say y<u

Therefore, initial velocity of blue ball> initial velocity of red ball

Hence, Sal plots blue graph's x initial velocity(initial velocity along x-axis or horizontal axis) a little bit more than the red graph's x initial velocity(initial velocity along x-axis or horizontal axis).

Hope this made you understand!(1 vote)

- Hi there, at4:42why does Sal draw the graph of the orange line at the same place as the blue line? I thought the orange line should be drawn at the same level as the red line. Thanks!(4 votes)
- why is the acceleration of the y-value negative? Why is the acceleration of the x-value 0.(2 votes)
- Vectors towards the center of the Earth are traditionally negative, so things falling towards the center of the Earth will have a constant acceleration of -9.8m/s/s(3 votes)

- I cannot understand why the acceleration in x direction is zero in all three cases? If we throw something in the air, we put force on it. So the acceleration in both directions should be made.(2 votes)
- Gravity acts in a downward direction. In actuality there is wind resistance acting horizontally against the object, but for the scope of introducing the concept, it is important to recognize that in the absence of wind resistance, there is no force acting horizontally on the object(3 votes)

- in the first graph of the second row (Vy graph) what would I have to do with the ball for the line to go upwards into the 1st quadrant? the person who through the ball at an angle still had a negative velocity. second question. if the ball hit the ground an bounced back up, would the velocity become positive?(3 votes)
- An object is launched up into the air at a 68° angle. Take up to be positive & down to be negative. Identify which one of the following POSITION vs. TIME graphs best represents the X-POSITION (rx) of the projectile & which graph best represents the Y-POSITION (ry). Ignore air drag.

Can some explained to me why the X-position in the case would start negative and trend constantly up to 0? this video shows it starting at zero...(2 votes)

## Video transcript

- [Instructor] So in
each of these pictures we have a different scenario. We have someone standing at
the edge of a cliff on Earth, and in this first scenario, they are launching a
projectile up into the air. In this one they're just
throwing it straight out. They're not throwing it up or
down but just straight out. And here they're throwing the projectile at an angle downwards. And so what we're going
to do in this video is think about for each of
these initial velocity vectors, what would the acceleration versus time, the velocity versus time, and the position versus
time graphs look like in both the y and the x directions. So I encourage you to pause this video and think about it on your own
or even take out some paper and try to solve it
before I work through it. So let's first think about acceleration in the vertical dimension, acceleration in the y direction. We're assuming we're on
Earth and we're going to ignore air resistance. We can assume we're in some
type of a laboratory vacuum and this person had maybe
an astronaut suit on even though they're on Earth. What would be the acceleration
in the vertical direction? Well the acceleration due to
gravity will be downwards, and it's going to be constant. We're going to assume
constant acceleration. So the acceleration is
going to look like this. And if the magnitude of the acceleration due to gravity is g, we could call this negative g to show that it is a downward acceleration. Once the projectile is let loose, that's the way it's
going to be accelerated. Now what about in the x direction? Well if we assume no air resistance, then there's not going
to be any acceleration or deceleration in the x direction. So it's just going to be, it's just going to stay right at zero and it's not going to change. And what I've just drawn
here is going to be true for all three of these scenarios because the direction
with which you throw it, that doesn't somehow affect
the acceleration due to gravity once the ball is actually
out of your hands. So now let's think about velocity. So what is going to be the
velocity in the y direction for this first scenario? Well we could take our
initial velocity vector that has this velocity at an angle and break it up into
its y and x components. So this would be its y component. We just take the top part of
this vector right over here, the head of it, and go to the left, and so that would be the
magnitude of its y component, and then this would be the
magnitude of its x component. So the y component, it starts positive, so it's like that, but remember our acceleration
is a constant negative. So our velocity is going to
decrease at a constant rate. So our velocity in this first scenario is going to look something, is going to look something like that. Now what about the velocity
in the x direction? We see that it starts positive, so it's going to start positive, and if we're in a world
with no air resistance, well then it's just
going to stay positive. Notice we have zero acceleration, so our velocity is just
going to stay positive. One of the things to really keep in mind when we start doing
two-dimensional projectile motion like we're doing right over here is once you break down your
vectors into x and y components, you can treat them
completely independently. That something will
decelerate in the y direction, but it doesn't mean that
it's going to decelerate in the x direction. Now what would the velocities look like for this blue scenario? Well our velocity in our y direction, we start off with no
velocity in our y direction so it's going to be right over here. But then we are going to
be accelerated downward, so our velocity is going
to get more and more and more negative as time passes. And notice the slope on
these two lines are the same because the rate of
acceleration is the same, even though you had a
different starting point. Now what about the velocity
in the x direction here? It looks like this x initial velocity is a little bit more than this one, so maybe it's a little bit higher, but it stays constant once again. Now let's look at this third scenario. In this third scenario, what is our y velocity,
our initial y velocity? Well it would look something like that. And our initial x velocity
would look something like that. If we were to break things
down into their components. So our y velocity is starting negative, is starting negative, and then it's just going to
get more and more negative once the individual lets go of the ball. Because you have that
constant acceleration, that negative acceleration, so it's gonna look something like that. And what about in the x direction? Well looks like in the x
direction right over here is very similar to that one, so it might look something like this. I'll draw it slightly higher
just so you can see it, but once again the velocity
x direction stays the same because in all three scenarios, you have zero acceleration
in the x direction. Now last but not least
let's think about position. So they all start in the exact same place at both the x and y dimension, but as we see, they all have
different initial velocities, at least in the y dimension. So let's start with
the salmon colored one. So the salmon colored one, it starts off with a some
type of positive y position, maybe based on the height of
where the individual's hand is. And then what's going to happen? Well it's going to have
positive but decreasing velocity up until this point. At this point its velocity is zero. So its position is going to go up but at ever decreasing
rates until you get right to that point right over there, and then we see the velocity
starts becoming more and more and more and more negative. So it would look something like, something like that. Now what would be the x position of this first scenario? Well if we make this position
right over here zero, then we would start our x
position would start over here, and since we have a constant
positive x velocity, our x position would just
increase at a constant rate. It would do something like that. Now what about this blue scenario? Well this blue scenario, we are starting in the exact same place as in our pink scenario, and then our initial y velocity is zero, and then it just gets
more and more and more and more negative. So it would look something, it would look something like this. Now what about the x position? Well our x position, we had a slightly higher velocity, at least the way that I drew it over here, so we our x position would
increase at a constant rate and it would be a slightly
higher constant rate. So it would have a slightly higher slope than we saw for the pink one. Now the yellow scenario, once again we're starting
in the exact same place, and here we're already starting
with a negative velocity and it's only gonna get more
and more and more negative. So it's just gonna do something like this. It's gonna get more and
more and more negative. It's a little bit hard to see, but it would do something like that. And if the in the x direction, our velocity is roughly the
same as the blue scenario, then our x position over
time for the yellow one is gonna look pretty pretty similar. So this is just a way to visualize how things would behave
in terms of position, velocity, and acceleration
in the y and x directions and to appreciate, one, how to draw and visualize these graphs and conceptualize them, but also to appreciate that you can treat, once you break your initial
velocity vectors down, you can treat the different dimensions, the x and the y dimensions, independently.