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Physics: Conservation of Momentum 72 Views
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Description:
The Law of Conservation of Momentum says that total momentum always stays the same in a closed system. In an open system, though, all hell usually breaks loose.
Transcript
- 00:00
Conservation of momentum. It's not just a good idea, it's the law. [mumbling]
- 00:32
All right, well it's important to have a healthy respect for the law. [cop in cop car]
- 00:36
No kneeling around here and don't seed when you drive, don't litter and don't
- 00:41
forget to tell your mom you love her. That's not a law, that's just you know being
- 00:45
nice. Alright but the truth is, there are some laws that you just can't break. Like
Full Transcript
- 00:49
it's impossible, it can't be done. Try as hard as you want, it ain't gonna happen.
- 00:52
Those are the laws of physics, not the NFL. And if you try to break one of those [two people in lab]
- 00:58
physics laws, well you won't go to physics jail, or anything. But you might
- 01:01
not be too happy with the result. Try and break the law of gravity, for example.
- 01:05
I'll just watch from a safe distance. Well one of these laws of physics, is the
- 01:11
law of conservation of momentum. This law states, that in a closed system, the total
- 01:17
amount of momentum always stays the same. Now in the real world we don't run into
- 01:21
a lot of closed systems. For example when you roll a bowling ball down the lane,
- 01:25
the bowling balls momentum is transferred to the pins, or it's [bowling ball and bowling pins]
- 01:28
transferred to the gutter. Yeah it happens. But when the ball hits the pins,
- 01:32
pins don't just bounce around forever, maintaining their momentum, that gains
- 01:35
momentum is transferred to the side walls and the lane and whatever the
- 01:39
technical term is for the back of the lane. All of those surfaces deform
- 01:44
slightly, as the momentum of the pins, is transferred. So the momentum goes to
- 01:49
these other things, within the system. But the effect is so small, we can't see it.
- 01:54
Of course, physics tends to look at ideal systems. And as we know from the fact [cop in cop car with Ferrari speeding by]
- 01:59
that we still don't have our own Ferrari, well the real world is almost never
- 02:03
ideal. But there's an equation, that expresses the conservation of momentum
- 02:07
and it's this one right here. Well this is just fancy math way of saying, that
- 02:13
the sum of all momenta, for all objects within a closed system, before the
- 02:19
objects interact, equals the sum of momentum for the objects, after they [equation on note page]
- 02:25
interact. And fortunately we can write it in a much simpler format. Yah, there
- 02:30
we go. But really it doesn't matter, because when we start doing the math, for
- 02:34
actual objects, actually interacting with each other. We replace both sides, of
- 02:39
these equation,s with the numbers for the objects. So if we just so happened, to
- 02:44
have someone, oh I don't know, sitting on a skateboard and then throwing a
- 02:48
medicine ball to someone. Well our equation would look like this. This equation says
- 02:54
that the initial momentum of the skateboarder, that's the P sub s I, plus [equation]
- 02:59
the initial momentum of the medicine ball P sub B I, equals the final momentum
- 03:05
of the skateboarder, plus the final momentum of the ball.
- 03:07
And since momentum equals mass, times velocity. We can swap those variables
- 03:12
into the equation, in place of P. So now we have this equation. Which says that,
- 03:22
the skateboarders mass, times his initial velocity, plus the ball's mass, times its
- 03:28
initial velocity, equals the skateboarders mass, times his final [formula]
- 03:33
velocity, plus the ball's mass, times its final velocity. Looking at this you can
- 03:38
see that if we have more than two objects, the equations can get a little
- 03:42
long-winded. Which is why we use that shorter
- 03:46
equation earlier. But let's go ahead and see how we would solve this equation. In
- 03:50
our scenario, we have teenagers performing physics in public. There's
- 03:54
nothing criminal in that, although it is a little weird. I've got my eye on you
- 03:57
citizens. At the start of this experiment, the skateboarder and the ball are not in [two people throwing ball to each other]
- 04:01
motion. Which means each initial velocity is a big fat zero. Let's put those values
- 04:07
into our equation. Before we go any further, we can solve the left side of
- 04:10
this thing right now. Whatever masses we're dealing with, are
- 04:12
irrelevant. Anything times zero in California, equals zero. So the initial
- 04:18
momentum of the skateboarder is zero, and the initial momentum of the medicine
- 04:20
ball zero and zero plus zero equals, seventy three billion 360. Oh wait hold
- 04:24
on, I spilled my coffee on my calculator earlier, it's on the fritz. [coffee on calculator]
- 04:27
All right zero, plus zero, is zero. Got it? So we got zilch. That's right, right hand
- 04:31
side will also have to evaluate to zero. That's only gonna happen if one of the
- 04:36
momentum on the right hand side is negative. Well remember momentum is a
- 04:40
vector quantity, so it has a magnitude and a direction.
- 04:44
Well the convention, to have any motion from left to right be a positive, value in any
- 04:48
motion from right to left be negative. Really doesn't matter though. You can set
- 04:52
whichever direction you want is positive and the other as negative. Just make sure
- 04:56
you're being consistent. The important thing to recognize here, is that we have [man throwing woman a ball while on skateboard]
- 04:59
two masses acting in opposite directions. One will have a negative velocity and
- 05:05
therefore have a negative momentum as well. So now we can set one velocity to
- 05:09
be negative in our equation, or just make the overall momentum be negative, like
- 05:13
this. And once we've done that we can see something interesting. With a bit of
- 05:18
algebra, we can add the negative momentum, to each side of our equation and find
- 05:22
that the final momentum for the skateboard, equals the final momentum for
- 05:24
the medicine ball. See how everything balances out all nice and pretty and [long equation]
- 05:29
laws of physics can be you know satisfying like that. Okay folks
- 05:34
experiment over. Let's keep moving, nothing else here to see. In that
- 05:38
skateboard experiment, we had two objects interacting and it was pretty friendly
- 05:41
interaction. But alot of times interactions between objects are gonna take the form
- 05:45
of, collisions. The collision can be a minor fender bender, or a five car pileup.[major car crash]
- 05:50
And collisions can be elastic, or inelastic. An elastic collision, occurs
- 05:57
when two objects collide and then bounce off each other going in different
- 06:02
directions. Think of playing pool. When the cue ball, hits the eight ball, the
- 06:06
balls don't just stick together, they go in different directions. Unless both
- 06:09
balls are covered in syrup, which is why waffle Wednesdays and pool tables are
- 06:14
not a good mix. An inelastic collision on the other hand, occurs when two objects
- 06:20
collide and then stick together. Say you're riding a bike, when a possum [man riding bike with possum on his back]
- 06:24
decides to hitch a ride. Well since conservation of momentum is
- 06:28
the law and you and your bike have now gained mass, in the form of a probably
- 06:33
dead marsupial. You'll therefore lose velocity. After all that's the only way
- 06:38
that momentum would stay the same, with an increase in mass. Just be careful that
- 06:43
this one looks kind of bitey, even if he is
- 06:45
potentially dead. Alright well because these problems can get confusing fast,
- 06:49
let's walk through the steps one by one, so we have a roadmap to solve them.
- 06:52
Step one, identify all the objects that interact with each other. We have two [chalk board step, and biker with possum on back]
- 06:57
objects that start off stuck together already, like the bike rider and his
- 07:01
bicycle. We can usually consider those as one object. Step two, if there are objects
- 07:07
moving in opposite directions, at any point, assign the velocity for one of the
- 07:11
directions a positive value and the velocity of the opposite direction a
- 07:15
negative value. Got that? Good. With our biker possum collision, all the velocity
- 07:21
was in the same direction. But typically we use right as the positive direction.
- 07:27
If you're feeling wild and rebellious, well go ahead and flip it around. [rebellious people]
- 07:32
Alright step three, set our balanced momentum equation. It should look
- 07:36
something like in this one. With mass and initial velocity for each object on the
- 07:40
left side and mass and final velocity for each object on the right. If we have
- 07:44
more than two objects interacting with each other, then we add the extra objects
- 07:47
to both sides of the equation, there we go.
- 07:50
Step four, if two objects stick together after a collision, we know the final
- 07:54
velocity will be the same for both objects. That means we can simplify the
- 07:58
right side of our equation, by adding up the masses of each object and [equation]
- 08:01
multiplying that sum, by the final velocity. I'll save a little work that
- 08:04
way. Alright, step 5, plug in whatever values we've been
- 08:08
provided, or have found experimentally. Since we set up our equations in advance,
- 08:13
it should be pretty straightforward. Just make sure not to mix up your masses
- 08:16
and velocities. You don't want to multiply object ones mass and object
- 08:20
twos velocity. I can't write you a ticket for that, but I can give you a [cop talking]
- 08:24
stern look. So be careful. Alright step six, remember to make the velocities
- 08:29
negative for whichever velocity direction, we've designated as our
- 08:33
negative one. If you skip this step well your right side, won't balance with your
- 08:37
left side. Which means the equation will crash and burn.
- 08:40
Step 7, solve for our unknown variable. A lot to say on this one I trust that you
- 08:45
have the requisite math skills under your belt. Alright, step eight, celebrate
- 08:50
with a doughnut. Oh sure, cops and donuts are a cliche but [cops in donut shop]
- 08:53
tell me you don't like, a nice fresh glaze and a circle of fried dough.
- 08:57
Yeah that's what I thought. Alright one last thing before we look at some problems.
- 09:01
All the motion we've looked at so far has been along one dimension. I'm not
- 09:08
sure if you've looked around lately, but life is 3d. So although we're not going
- 09:12
to deal with it right now, in the future you're likely to run across problems
- 09:15
that deal with momenta, in two, three, or if supernatural forces are involved, five
- 09:21
or six dimensions. Who knows? Which means we might have to use trigonometry to
- 09:25
break the momentum down to XY and z components. We're just telling you now so[people freaking out in classroom]
- 09:29
you don't freak out, in some of the advanced physics class later. Alright
- 09:33
well we've got your attention. Let's talk about driving safely in dangerous
- 09:36
conditions. Say we've got an icy road, three cars are driving, with car a in
- 09:40
front, driving responsibly. Car B is making sure to keep an appropriate
- 09:44
amount of space between her car and car A. Meanwhile some jerk, in car C,
- 09:49
comes barreling in. Going way over the proper speed limit for the weather. Car
- 09:54
C collides with car B and they stick together going forward, until car B hits [three vehicle car crash]
- 09:58
car A. Now all three cars are conjoined at the bumper, headed in the same
- 10:03
direction and we've got a big mess to straighten out.
- 10:05
What's the conservation of momentum equation, for this scenario and we need
- 10:10
to break it down to masses and velocities. Okay, so we know the shorthand
- 10:14
equation, the sum of momentum before interaction, equals the sum of momenta
- 10:18
after the interaction. But we could also write it like this, with P sub a P sub B
- 10:23
and P sub C. But we need to break it down to masses and velocities. So let's work on the
- 10:28
left side first. Makes sense, since it's the, you know, before side. We'll go step [equation formula]
- 10:34
by step. We know our three objects are cars A, B
- 10:37
and C. So we'll start with M sub a times, V sub AI and we'll add, M sub B, times V
- 10:42
sub B I and last but not least we got the one that started it all, M sub C
- 10:47
times V sub C I, aka jerk. All right, how about the right side. We definitely need
- 10:54
to add up the masses of each car, but since they're all sliding along this icy
- 10:58
low friction road together. We'll only have one velocity to deal with. [cars conjoined in crash]
- 11:03
So the right side of the equation will be, M sub A, plus M sub B, plus M sub C and
- 11:09
all of that will be multiplied by V sub F. Alright now we don't have any values
- 11:14
here, we're just setting up the equation. Do we have any negative momentum to deal with? Well
- 11:18
no, this wasn't a head-on collision. All the cars we're moving in the same
- 11:22
direction, so we don't need to worry about anything negative there. Here's how
- 11:26
we want our equation to be, before we plug in any values, right there. Okay,
- 11:30
let's think about another scenario. And say we've got two ice skating kangaroos. [kangaroos ice skating]
- 11:34
Which may sound crazy to you, but I've seen some things in this line of work
- 11:38
man. Yeah, I've seen some things. Anywho, well they're working on their ice
- 11:43
dancing routine and at one part of the routine they come together on the ice,
- 11:46
standing motionless, facing each other. It's really a beautiful, marsupial moment.
- 11:49
Then they push off, going in opposite directions. You can hear the music
- 11:53
crescendoing, kangaroo one has a mass of 102 kilograms,
- 11:56
slides away with the velocity of 2.1 meters a second. Kangaroo two who we're
- 12:01
gonna call kanga two. Because well it just sounds cooler, has a mass of 109 [2 kangaroos ice skating]
- 12:04
kilograms. What's kanga two's velocity as he gracefully
- 12:07
slides away? Well let's walk through this thing step by step. First we identify our
- 12:12
objects. Easy enough, we've got kanga 1 and kanga two step 2. If we have
- 12:16
motion in opposite directions, we set one is positive, the other is negative. In
- 12:20
this case kanga one's velocity has already said is positive 2.1
- 12:24
meters a second. So kanga 2 will be negative velocity and momentum. Next we
- 12:28
set up our before-and-after equation. Sum of moment of each kangaroo, before they
- 12:33
push off each other, equals the sum of momenta, after they push off each other. [kangaroo formula]
- 12:37
All right, step four says, if two objects stick together after their interaction,
- 12:42
we add up their masses and multiply that by the final velocity. But in this case
- 12:47
we have two animals that start off together, then move apart. So we can
- 12:51
add up their masses and multiply that, by the initial velocity. Okay, so now we've
- 12:56
got our equation set up. Step five says, we can start putting in the numbers. All [equation written out]
- 13:01
right on the left side, we've got one hundred two kilograms, plus hundred nine
- 13:04
kilograms and an initial velocity of nada.
- 13:07
On the right we've got a mass of 102 kilograms, times velocity of 2.1 meters a
- 13:11
second, plus a mass of 109 kilograms, times velocity were solving for. What
- 13:15
is that number? All right, right away we can see the left side is going to equal
- 13:19
zero and we can do that math on kanga one, to find a momentum of two hundred
- 13:23
fourteen point two kilogram meters per second. Then we can subtract kanga two's
- 13:28
momentum, the mass, times the unknown velocity there, from both sides of the [equation worked out]
- 13:32
equation. Leaving us with negative 109 kilograms, times V sub 2f, equaling two
- 13:38
hundred fourteen point two kilogram meters per second. And now people all we
- 13:42
have to do is, divide each side by negative 109 kilograms, to solve for the
- 13:46
missing velocity. And Kenga two's velocity equals about negative 2.0 kilogram
- 13:51
meters a second. Which makes sense kanga two has a smidge more mass, than kanga one
- 13:56
so his velocity should be a smidge less. Truth is you can break most laws. I might [cop in cop car]
- 14:02
not see you speed on the highway and if you're super careful, jaywalking isn't
- 14:06
gonna be a big deal most of the time. And your mom might say you get away with
- 14:09
murder, but that's just a figure of speech. Please don't take her literally.
- 14:13
But yeah you're not breaking the law of conservation of momentum. Don't even
- 14:16
bother trying. All right if the Isaac Newton and Rene Descartes
- 14:20
say it's law, well you better take their word for it. [court room with people in it]
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