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Physics: Practicing Perfect Projectiles 15 Views
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Description:
Time for some fun with 2-D motion. We'll use horizontal speed and distance to find vertical motion, and more. So... a 2-D experiment, but 3-D excitement.
Transcript
- 00:01
No practicing perfect projectiles more fun with two t emotion
- 00:06
I put next one together being the rocket's trajectory I
- 00:10
can't forget the equation court Wait forget that i'm getting
- 00:15
more complex No All right here we go Ladies and
- 00:23
gentlemen we regret to inform you for it War now
Full Transcript
- 00:26
the proud country of shmoop sylvania has put up with
- 00:29
our old enemy East ignorance is stand for too long
- 00:34
We plan on launching a barrage of smart rockets to
- 00:36
attack their lack of knowledge and its core thes rockets
- 00:39
will carry payloads of literature algebra history and oh so
- 00:43
much more All right rocket scientists what is rocket science
- 00:47
But physics put in emotion explode emotion one of our
- 00:52
favorite kinds Well but before we just start launching rockets
- 00:55
willy nilly it'll help if we can figure out how
- 00:58
far they're going to go and how long it'll take
- 01:00
to get him there So consider this lesson Rocket science
- 01:03
one oh one here the equations we're going to need
- 01:06
for this lesson We saw these in the last lesson
- 01:08
but yeah let's go over it again just to make
- 01:10
sure we remember him We've got the one for displacement
- 01:14
in the extraction which we find by multiplying the velocity
- 01:17
and the extraction by the elapsed time we could also
- 01:20
find the change in displacement vice of tracking the initial
- 01:22
displacement from the final displacement like in this equation right
- 01:26
here and these are the only equations will need for
- 01:29
motion along the x axis because we're not gonna have
- 01:31
any acceleration along the x axis but the only acceleration
- 01:35
will be dealing with will be in the uae direction
- 01:37
Yeah and that'll be gravity doing it's a you know
- 01:40
gravity thing So we'll be using to equations for an
- 01:43
emotion on the y axis first this one it tells
- 01:46
us that the change in displacement in the uae direction
- 01:50
equals the initial velocity in the white direction multiplied by
- 01:52
the time plus one half the acceleration of gravity times
- 01:55
time squared And if we don't know how much time
- 01:58
a particular emotion takes well in that case we can
- 02:00
put this equation to use what's it telling us while
- 02:03
the square of the final velocity in the wider action
- 02:05
equals the square the initial y velocity plus two times
- 02:09
the acceleration of gravity times the change in displacement along
- 02:12
that why axis So yeah we have a history with
- 02:15
these three equations Phone we go way back but we're
- 02:17
doing something new with them Today we'll be using more
- 02:20
than one to help us find whatever solution that we're
- 02:23
looking for but remember we can't get our ex variables
- 02:26
mixed up with our wives variables i have to remain
- 02:28
separate it's that time that links them together and while
- 02:32
we're keeping our x and y separate let's talk about
- 02:34
how to talk about him while hotshot physicists use different
- 02:38
terms when it comes to these different motions when we're
- 02:41
talking about motion in the extraction will use the term
- 02:44
range to describe the maximum horizontal distance of projectile travels
- 02:49
but when we're looking at vertical motion will use the
- 02:51
term maximum height to describe well that maximum height of
- 02:55
our projectile And we might think of a projectile only
- 02:58
in terms of missiles or bullets or whatever but term
- 03:01
doesn't have to refer to things that go bang when
- 03:04
a hunter kicks a football well that football is now
- 03:07
a projectile If you accidentally knock your fork off the
- 03:10
dinner table the fork is now projectile and if we
- 03:13
toss you a soda that can is a projectile although
- 03:16
it might be an example of an explosion No well
- 03:19
now we're dealing with something as complicated as rocket science
- 03:22
we're gonna have to expand our arsenal of handy physics
- 03:25
trip First of all everything will be dealing with here
- 03:28
will still have zero acceleration along the x axis and
- 03:32
it'll also have the acceleration of gravity in the y
- 03:35
axis There won't be any other accelerations to wrap our
- 03:39
minds around Let's take a look at the full trajectory
- 03:41
of one of our smart rockets All right what is
- 03:43
this trajectory Tell us about the vertical velocity Well for
- 03:47
one thing we know there's an initial vertical velocity This
- 03:51
isn't the case where a car drives off the side
- 03:53
of a cliff This rocket is going up up up
- 03:55
been away But as we know from that one time
- 03:59
we were throwing our little cousin in here What goes
- 04:02
up You must come down with a nice pretty problem
- 04:05
like this We can see that the overall motion is
- 04:07
symmetrical You could fold it right in half So when
- 04:10
a projectile begins and ends its vertical motion in the
- 04:13
same position like here where it begins and ends at
- 04:17
the zero point for why then the max height will
- 04:20
occur halfway through whatever time period we're looking at You
- 04:23
might see that Height referred to as the change in
- 04:26
height or delta y and the upward velocity that occurs
- 04:30
during the first half of the motion will be equally
- 04:32
matched by that downward motion in the second half And
- 04:35
when we look at the halfway mark again will find
- 04:38
that the y velocity at that precise moment is zero
- 04:42
meters per second just hanging in the air for one
- 04:44
tiny sliver of time Then gravity wins the battle in
- 04:47
the velocity turns downward now believe it or not this
- 04:50
type of motion isn't restricted on ly two rockets What
- 04:53
if we head to the basketball court so we can
- 04:55
show off our sick moves and our three point range
- 04:58
Okay that was an air ball which is perfect it's
- 05:02
what we're trying to do Really Because then we can
- 05:04
show you this graph just like the rocket The best
- 05:07
well traveled in a parabola See how we have our
- 05:10
velocity arrows there at every point on the graph the
- 05:13
horizontal motion has the same velocity which is why all
- 05:17
those arrows are the same size But the vertical arrows
- 05:20
change if you line them up Like looking at the
- 05:23
third basketball from the right and the third basket ball
- 05:26
from the left we see that the arrows are pointing
- 05:29
in different directions but they have the same magnitude Yeah
- 05:33
remember this equation where we're finding the final velocity Yeah
- 05:37
well if the change in displacement in the white direction
- 05:40
is zero it means the whole second half of the
- 05:43
right side will equal zero leaving us with final velocity
- 05:47
equal in the initial velocity at least in terms of
- 05:49
magnitude moving in a direction So let's put this stuff
- 05:52
in action Let's say that shmoop er man in bizarro
- 05:55
shmoop her man that trooper man's evil twin We're having
- 05:58
a friendly game A catch near the fortress of learning
- 06:01
you know is friendly again The catch is you can
- 06:03
get with your evil twin Well since they're twins they
- 06:06
throw with the same velocities both vertical and horizontal and
- 06:10
they throw and catch from the same height Now these
- 06:13
aren't normal people tossing a baseball around so they're putting
- 06:16
some oomph into these things Let's say they're throwing in
- 06:20
catching the ball from one point five meters off the
- 06:22
ground and the ball reaches a mac sight of one
- 06:24
hundred one point Five meters How much time does it
- 06:27
take the ball to travel between this superhuman pair Okay
- 06:31
well first of all let's figure out what we know
- 06:33
what we don't know and what we want to know
- 06:36
Well let's look at the motion in the uae direction
- 06:38
First of all we know that max height is one
- 06:40
hundred one point five meters and the starting height is
- 06:43
one point Five meters when we subtract the initial list
- 06:45
placement from the max when you find a change in
- 06:47
displacement of one hundred meters no what about the initial
- 06:50
y velocity It must be pretty high but we don't
- 06:54
know what it is at this point We do know
- 06:56
that the initial velocity is the same as the final
- 06:58
velocity when the ball reaches bizarro shmoop her man And
- 07:02
we know that when the balls at its highest point
- 07:04
the velocity in the uae direction is zero meters per
- 07:07
second which is the key right there Now we know
- 07:10
nothing about the horizontal motion velocity distance No clue but
- 07:15
we're only trying to find the time here so we
- 07:17
don't need all that stuff What we need to do
- 07:19
is figure out how long the ball takes to reach
- 07:21
the max tight or alternatively how long it takes the
- 07:25
ball to fall from the max height Clever each half
- 07:29
of the balls flight will take the same amount of
- 07:30
time So what equation will we use Well we've got
- 07:34
two to choose from for vertical motion Well first we've
- 07:38
got this one for the change in displacement on the
- 07:40
y axis and then we've got this one to find
- 07:42
the final velocity when we're trying to find the time
- 07:45
people and only one equation has time in it and
- 07:48
everything so it looks like we'll be choosing bachelor number
- 07:51
one We'll use the change in height of one hundred
- 07:53
meters and we'll find the time it takes for the
- 07:56
ball to go from its peak to pizarro's glove Why
- 08:00
Because that lets us set the initial velocity at zero
- 08:03
zero meters per second which simplifies the equation a whole
- 08:07
lot for us because the first part of the equation
- 08:09
on the right side the initial loss any times time
- 08:11
will equal zero when the initial velocity equals zero which
- 08:14
means that the change in displacement equals one half the
- 08:18
acceleration and gravity Times the square of the time period
- 08:22
Now we just have to isolate a that tea Well
- 08:25
in most cases we've set the acceleration of gravity as
- 08:27
a negative number but remember it's totally upto us and
- 08:30
in this case we're actually going to use the positive
- 08:32
version Why Because we're all about the power of positivity
- 08:36
and keeping the acceleration positive will really help We'll show
- 08:40
you why in a second so the acceleration of gravity
- 08:42
will be nine point eight meters per seconds squared And
- 08:45
when we have that we get four point nine meters
- 08:48
per second squared And now let's divide both sides of
- 08:50
the equation by that number Leaving us with time squared
- 08:53
equals one hundred meters over four point nine meters per
- 08:55
second squared I was still not done because we need
- 08:58
t not t squared So time equals the square root
- 09:02
of one hundred meters over four point nine years per
- 09:04
second squared Which is why we used a positive value
- 09:07
for the acceleration and gravity because finding a negative square
- 09:10
route leads us into the land of imaginary numbers And
- 09:13
this story is about a superhero and his evil twins
- 09:17
Oh that needs to be you know grounded in reality
- 09:20
when we put the numbers into our trusty calculator we
- 09:22
find that t equals four point five two seconds but
- 09:25
hold on remember this was on ly for the second
- 09:28
half of the trajectory the time for the first half
- 09:32
is the same so we just have to do double
- 09:34
our result to get the total time which means the
- 09:37
ball is in the air for nine point oh four
- 09:39
seconds and were able to figure out the time But
- 09:41
what about the velocities Both horizontal and vertical Well there's
- 09:44
no way we'd actually be able to calculate that is
- 09:47
there Well actually no atleast for the horizontal velocity because
- 09:52
we need one more piece of information which is the
- 09:54
distance or range between the two super twins So we'll
- 09:58
say it's well half a kilometre better known asked five
- 10:01
hundred meters and we'll keep the vertical values the same
- 10:05
as what we were using before Now we can get
- 10:07
there so let's tackle the vertical velocity first this time
- 10:11
we'll use that other equation we were looking at and
- 10:13
we'll use the same trick we did last time by
- 10:15
focusing on the second half of the trajectory which once
- 10:18
again lets us use an initial velocity of zero And
- 10:21
to be frank it's not really a trick Because if
- 10:24
we looked at the whole trajectory are changing displacement would
- 10:27
equal zero And then our equation would just tell us
- 10:30
that the final velocity equals the initial velocity and you
- 10:33
do like a public chasing its tail which is pretty
- 10:36
cute but not helpful in doing physics All right let's
- 10:39
put numbers into this equation So the final velocity squared
- 10:42
equals two times the acceleration of gravity and we'll use
- 10:45
the positive number again So that's nine point eight meters
- 10:48
per seconds squared times the change in vertical displacement which
- 10:51
is a hundred meters So we find the final velocity
- 10:54
squared equals nineteen hundred sixty meters per second And then
- 10:58
we need the square route to get the actual velocity
- 11:00
which comes out forty four point three meters per second
- 11:04
and remember people the final velocity equals the initial velocity
- 11:07
So we killed two birds with one stone here or
- 11:10
a one baseball and not just for the vertical velocity
- 11:14
for horizontal motion We only have one equation worry about
- 11:17
and that's this One where the changing displacement equals of
- 11:20
velocity times the time Remember the vertical and horizontal motions
- 11:24
are linked by that t there An earlier we figured
- 11:27
out that the time elapsed was nine point oh four
- 11:30
seconds and our distance or displacement for the throw is
- 11:33
five hundred meters In order to isolate the velocity we
- 11:36
need divide both sides by the change in time or
- 11:39
delta t Once we've done that we find that the
- 11:42
velocity equals the distance divided by the time so the
- 11:45
velocity in the ex direction equals five hundred meters divided
- 11:48
by nine point Oh four seconds giving us a horizontal
- 11:51
velocity of fifty five point three meters per second which
- 11:55
is equivalent to about one hundred twenty four miles an
- 11:57
hour which is really fast right Well once again we
- 12:00
were able to get all the answers by looking at
- 12:02
the two perpendicular motions separately which should be everything we
- 12:06
need to launch our smart rockets and wipe east ignorant 00:12:10.6 --> [endTime] to stand off the map
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