< Return to Video

Newton's second law | Middle school physics | Khan Academy

  • 0:00 - 0:02
    - [Instructor] According
    to Newton's first law,
  • 0:02 - 0:04
    if the net force acting
    on an object is zero,
  • 0:04 - 0:06
    the object's motion will not change.
  • 0:06 - 0:09
    This means, for example, if an
    object is at rest on a table
  • 0:09 - 0:10
    or, say, somewhere in intergalactic space
  • 0:10 - 0:11
    where the net force is zero,
  • 0:11 - 0:15
    then the object will
    continue to be at rest.
  • 0:15 - 0:16
    On the other hand, if
    the object was moving,
  • 0:16 - 0:19
    and again, if the net
    force on it was zero,
  • 0:19 - 0:21
    then it'll continue to move
  • 0:21 - 0:24
    with that exact same velocity forever.
  • 0:24 - 0:26
    But now, here's a question.
  • 0:26 - 0:30
    What if the net force acting
    on an object is not zero?
  • 0:30 - 0:34
    Well, then the object's
    motion will change.
  • 0:34 - 0:39
    So, a net force will
    change the object's motion.
  • 0:39 - 0:44
    In other words, a net
    force causes acceleration.
  • 0:44 - 0:46
    But how exactly are they connected?
  • 0:46 - 0:47
    That's what we're gonna find out
  • 0:47 - 0:49
    in this video, so let's begin.
  • 0:49 - 0:50
    So how do we do this?
  • 0:50 - 0:52
    Well, we take a bunch of masses,
  • 0:52 - 0:55
    apply a net force and measure that,
  • 0:55 - 0:57
    and then measure how much
    acceleration they get
  • 0:57 - 0:59
    because of the net force.
  • 0:59 - 1:02
    And then if we do enough trials,
    maybe we can see a pattern
  • 1:02 - 1:04
    and maybe we can see the
    connection between them.
  • 1:04 - 1:06
    But of course, the big question is,
  • 1:06 - 1:09
    how do we measure net
    force acting on an object?
  • 1:09 - 1:12
    And how do we measure
    the acceleration of it?
  • 1:12 - 1:14
    Well, let's look at it one by one.
  • 1:14 - 1:16
    So first of all, how do
    we measure a net force?
  • 1:16 - 1:19
    Well, a cool equipment that
    we can use to measure forces
  • 1:19 - 1:20
    is a spring balance.
  • 1:20 - 1:21
    And the way the spring balance works
  • 1:21 - 1:23
    is that there's a spring over here.
  • 1:23 - 1:26
    So if you pull on it, say from this side,
  • 1:26 - 1:28
    then the spring is compressed
  • 1:28 - 1:30
    and therefore it pulls back,
  • 1:30 - 1:31
    and the number, the reading over here,
  • 1:31 - 1:33
    tells you exactly with how much force
  • 1:33 - 1:35
    the spring is pulling back on you.
  • 1:35 - 1:38
    So in this example, the
    spring is pulling on my hand
  • 1:38 - 1:41
    with a force of exactly two newtons.
  • 1:41 - 1:43
    If you had pushed it from this end,
  • 1:43 - 1:45
    then the spring is pushing
  • 1:45 - 1:46
    with the force of exactly two newtons.
  • 1:46 - 1:47
    And now since I know
  • 1:47 - 1:49
    with exactly how much force it is pushing,
  • 1:49 - 1:52
    I can use this to push on our objects.
  • 1:52 - 1:55
    And look, I will now know
    exactly with what force
  • 1:55 - 1:57
    we are pushing on the object.
  • 1:57 - 1:58
    Pretty cool, isn't it?
  • 1:58 - 2:01
    But wait a second. That is only one force.
  • 2:01 - 2:04
    Remember, our goal is to
    figure out the net force.
  • 2:04 - 2:05
    How do we do that?
  • 2:05 - 2:06
    How do we figure out how much net force
  • 2:06 - 2:07
    is acting on an object?
  • 2:07 - 2:08
    Well, let's see, if you
    were to keep these objects
  • 2:08 - 2:11
    on a table, then there are
    forces in the vertical,
  • 2:11 - 2:13
    like gravity and normal force,
  • 2:13 - 2:15
    but they get balanced, they
    are balanced, isn't it?
  • 2:15 - 2:17
    So we don't have to
    worry about those forces.
  • 2:17 - 2:20
    We only have to worry about
    the forces in the horizontal.
  • 2:20 - 2:21
    So one of the forces in the horizontal
  • 2:21 - 2:23
    is our spring force, which we know.
  • 2:23 - 2:24
    But what about the other forces?
  • 2:24 - 2:26
    The other forces are the force of friction
  • 2:26 - 2:27
    and air resistance.
  • 2:27 - 2:29
    We can minimize friction drastically
  • 2:29 - 2:31
    by using an air hockey table, right?
  • 2:31 - 2:33
    And if the velocities are not too high,
  • 2:33 - 2:35
    then even the air
    resistance is very minimal.
  • 2:35 - 2:37
    So look, in the horizontal,
  • 2:37 - 2:38
    there's only one effective force,
  • 2:38 - 2:39
    and that is the spring force.
  • 2:39 - 2:43
    So that itself becomes the
    net force. Amazing, right?
  • 2:43 - 2:45
    Okay, so that's how we
    can measure the net force.
  • 2:45 - 2:47
    What about the acceleration?
    How do we measure that?
  • 2:47 - 2:49
    Well, for that, we can use a motion sensor
  • 2:49 - 2:52
    which will periodically
    monitor the velocity,
  • 2:52 - 2:55
    and it'll give you a velocity-time graph.
  • 2:55 - 2:56
    And by analyzing the graph,
  • 2:56 - 2:58
    we can measure the acceleration.
  • 2:58 - 3:00
    Okay, so with that, we
    have everything needed.
  • 3:00 - 3:02
    We can go ahead and plan our experiment.
  • 3:02 - 3:04
    But how do we do that?
  • 3:04 - 3:05
    Well, one of the best ways to do that
  • 3:05 - 3:08
    is to think about the variables involved.
  • 3:09 - 3:11
    So, what are the variables
    involved over here?
  • 3:11 - 3:12
    Well, we have the net force.
  • 3:12 - 3:16
    Since this is the variable that
    we can change independently,
  • 3:16 - 3:18
    we call this the independent variable.
  • 3:18 - 3:20
    Then, of course, there is the acceleration
  • 3:20 - 3:21
    that we're gonna measure.
  • 3:21 - 3:25
    This acceleration is dependent
    on the net force, right?
  • 3:25 - 3:27
    So we call this the dependent variable.
  • 3:27 - 3:28
    So now for our experiment,
  • 3:28 - 3:31
    we can push this object
    with different net forces.
  • 3:31 - 3:34
    Say we'll do three trials,
    and then for each of them,
  • 3:34 - 3:36
    we'll figure out what the acceleration is.
  • 3:36 - 3:38
    And by measuring the acceleration,
  • 3:38 - 3:39
    maybe we can make a connection
  • 3:39 - 3:41
    between the net force and
    the acceleration, isn't it?
  • 3:41 - 3:43
    Okay, that sounds like a plan,
  • 3:43 - 3:46
    but there's another variable
    over here, the mass.
  • 3:46 - 3:49
    What do we do about that?
    Should we also change that?
  • 3:49 - 3:51
    Well, here's an important
    thing about doing experiments.
  • 3:51 - 3:55
    You should always change
    just one variable at a time.
  • 3:55 - 3:57
    Since you're already
    changing the net force,
  • 3:57 - 3:58
    this particular variable,
  • 3:58 - 4:01
    we wanna make sure the mass is a constant.
  • 4:01 - 4:03
    So we're gonna use the same
    value of the mass everywhere.
  • 4:03 - 4:07
    And therefore we call
    this the control variable
  • 4:07 - 4:09
    because we're not changing that.
  • 4:09 - 4:10
    It's going to be a constant.
  • 4:10 - 4:12
    So what mass can we use?
    Well, we can use any one.
  • 4:12 - 4:14
    Let's just use one kilogram mass.
  • 4:14 - 4:16
    So we now have our plan.
  • 4:16 - 4:18
    We're gonna push the one kilogram object
  • 4:18 - 4:19
    with different forces,
    and we're gonna measure
  • 4:19 - 4:22
    what the acceleration's going to be.
  • 4:22 - 4:24
    All right, so, we'll start by pushing
  • 4:24 - 4:26
    with two newtons of force
    on the one kilogram object.
  • 4:26 - 4:28
    And once we let go of this,
  • 4:28 - 4:30
    the object will start accelerating,
  • 4:30 - 4:33
    and we will also keep that
    contact for about a second.
  • 4:33 - 4:35
    So we'll put the force for about a second.
  • 4:35 - 4:37
    We'll try to make sure that
    this stays at two newtons
  • 4:37 - 4:39
    so the force is a constant, okay?
  • 4:39 - 4:42
    So let's do that. And there we have it.
  • 4:42 - 4:45
    Once we let go of the contact,
    the object stops accelerating
  • 4:45 - 4:46
    and it continues to move
  • 4:46 - 4:49
    within a straight line
    with a constant velocity.
  • 4:49 - 4:51
    So let's look at what our
    motion sensor has detected,
  • 4:51 - 4:53
    and let's see what the
    velocity-time graph looks like.
  • 4:53 - 4:56
    There we have it. Let's see
    if that graph makes sense.
  • 4:56 - 4:59
    For the first one second,
    the object was accelerating
  • 4:59 - 5:01
    because there was a
    net force acting on it.
  • 5:01 - 5:04
    And you can see, the
    velocity is increasing.
  • 5:04 - 5:06
    After the one second, the contact is lost
  • 5:06 - 5:08
    and the object moves
    with a constant velocity,
  • 5:08 - 5:11
    and that's why, look,
    the velocity stays put.
  • 5:11 - 5:13
    But how much is the acceleration?
  • 5:13 - 5:14
    We have to look at this.
  • 5:14 - 5:17
    And you can see, the object's
    velocity increased from zero
  • 5:17 - 5:21
    to two meters per second in one second.
  • 5:21 - 5:23
    So that is the acceleration.
  • 5:23 - 5:27
    Zero to two meters per
    second in one second.
  • 5:27 - 5:29
    All right, we're gonna do second trial,
  • 5:29 - 5:31
    but this time, we're gonna
    put four newtons of force.
  • 5:31 - 5:35
    And again, we'll push it for
    about one second and let it go.
  • 5:35 - 5:36
    All right? Here we go.
  • 5:36 - 5:39
    Boom! What do we notice?
  • 5:39 - 5:42
    Well, we notice that the
    object travels much faster.
  • 5:42 - 5:44
    So let's see what the
    velocity-time graph looks like.
  • 5:44 - 5:47
    What does our motion sensor give us?
  • 5:47 - 5:51
    Now the velocity-time
    graph looks like this!
  • 5:51 - 5:53
    Ooh, what is it saying?
  • 5:53 - 5:56
    Well, it's saying now in the first second
  • 5:56 - 5:58
    while the object was accelerating,
  • 5:58 - 6:00
    when the net force was acting,
  • 6:00 - 6:04
    the velocity increased from
    zero to four meters per second.
  • 6:04 - 6:06
    And then the object continues to move
  • 6:06 - 6:08
    with a constant velocity
    of four meters per second
  • 6:08 - 6:10
    because the contact was lost.
  • 6:10 - 6:14
    So now the acceleration is
    zero to four meters per second
  • 6:14 - 6:16
    in one second.
  • 6:16 - 6:18
    The acceleration became higher
  • 6:18 - 6:20
    when the net force became higher.
  • 6:20 - 6:22
    Does this make intuitive sense?
  • 6:22 - 6:24
    I think yes, it makes intuitive sense
  • 6:24 - 6:26
    that when you apply a larger net force,
  • 6:26 - 6:28
    the object accelerates larger.
  • 6:28 - 6:31
    And we are also experimentally
    seeing that. That's amazing.
  • 6:31 - 6:33
    Okay, if we did one more trial,
  • 6:33 - 6:34
    we get very similar results.
  • 6:34 - 6:36
    And this time, our motion sensor gives us
  • 6:36 - 6:38
    something like this.
  • 6:38 - 6:41
    And notice we get even
    higher acceleration.
  • 6:41 - 6:43
    This time, the acceleration
    is, in one second,
  • 6:43 - 6:46
    it goes from zero to
    five meters per second.
  • 6:46 - 6:48
    So the acceleration has further increased.
  • 6:48 - 6:50
    So what is the connection that we see?
  • 6:50 - 6:53
    We see for a higher net force,
  • 6:53 - 6:57
    more the net force, more
    is the acceleration,
  • 6:57 - 6:59
    provided the mass stays the constant.
  • 6:59 - 7:02
    We should always be careful
    about the control variable
  • 7:02 - 7:03
    that we have used.
  • 7:03 - 7:05
    Amazing, isn't it?
  • 7:05 - 7:07
    But now this brings up the last question.
  • 7:07 - 7:09
    What if you want to vary the mass?
  • 7:09 - 7:11
    We want to see the effect of what happens
  • 7:11 - 7:12
    when the mass changes.
  • 7:12 - 7:14
    Well, we should always make sure
  • 7:14 - 7:16
    only one variable is changing.
  • 7:16 - 7:17
    So if we want to vary the mass,
  • 7:17 - 7:20
    we have to keep this variable the same.
  • 7:20 - 7:22
    So, we'll repeat this experiment.
  • 7:22 - 7:24
    This time, we'll keep
    the net force the same.
  • 7:24 - 7:26
    Let's keep the net
    force, say, four newtons.
  • 7:26 - 7:29
    And let's vary the mass. Let's
    make the mass one kilogram.
  • 7:29 - 7:31
    Then let's repeat the
    experiment with two kilograms
  • 7:31 - 7:34
    and maybe with four kilograms.
  • 7:35 - 7:35
    All right, first up,
  • 7:35 - 7:37
    we'll put four newtons for one kilogram.
  • 7:37 - 7:40
    We actually already did this,
    but let's do it one more time.
  • 7:40 - 7:42
    We'll push it for one second, let it go.
  • 7:42 - 7:44
    And what does the motion sensor give us?
  • 7:44 - 7:46
    Well, it gives us an acceleration
  • 7:46 - 7:49
    of zero to four meters
    per second in one second.
  • 7:49 - 7:52
    Okay, let's repeat this, four newtons,
  • 7:52 - 7:54
    but this time for two kilogram object.
  • 7:54 - 7:57
    Again, push it for about
    a second, let it go.
  • 7:57 - 7:59
    What does the motion sensor give us?
  • 7:59 - 8:02
    (gasps) The acceleration is
    smaller. Can you see that?
  • 8:02 - 8:07
    It went from zero to two meters
    per second in one second.
  • 8:07 - 8:10
    Does that make sense? I think yes.
  • 8:10 - 8:12
    I mean, if you were to
    push a heavier object
  • 8:12 - 8:13
    with the same force,
  • 8:13 - 8:18
    you intuitively expect
    it to accelerate lesser.
  • 8:18 - 8:19
    And that's exactly what we get.
  • 8:19 - 8:22
    So as the mass increased,
    the acceleration reduced.
  • 8:22 - 8:24
    So let's do one last trial.
  • 8:24 - 8:26
    This time, the mass is four kilograms.
  • 8:26 - 8:27
    Again, we push it with the same force,
  • 8:27 - 8:29
    four newtons, for about a second.
  • 8:29 - 8:32
    We can already see the
    acceleration was much lower.
  • 8:32 - 8:34
    What does the motion sensor give us?
  • 8:34 - 8:37
    Well, it gives us (laughs)
  • 8:37 - 8:39
    much lower acceleration this time from,
  • 8:39 - 8:43
    it went from zero to one meters
    per second in one second.
  • 8:43 - 8:44
    So what do we notice?
  • 8:44 - 8:46
    We notice that for a given force,
  • 8:46 - 8:49
    if that force is the same,
    if the mass increases,
  • 8:49 - 8:52
    the acceleration reduces.
  • 8:52 - 8:55
    So more mass gives you less acceleration
  • 8:55 - 8:58
    for the exact same net force.
  • 8:58 - 9:03
    This is the essence of what we
    call the Newton's second law.
  • 9:03 - 9:05
    Of course, we could be more quantitative,
  • 9:05 - 9:07
    but I think this captures
    the essence beautifully.
  • 9:07 - 9:08
    Newton's second law is one
    of the most important laws
  • 9:08 - 9:11
    in physics because it allows
    us to predict the motion
  • 9:11 - 9:15
    provided we know the net
    force acting on the object.
Title:
Newton's second law | Middle school physics | Khan Academy
Description:

more » « less
Video Language:
English
Team:
Khan Academy
Duration:
09:17

English subtitles

Incomplete

Revisions