Lectures

Center of Gravity

by Jared Rovny
(1)

Questions about the lecture
My Notes
  • Required.
Save Cancel
    Learning Material 2
    • PDF
      Slides Equilibrium Physics.pdf
    • PDF
      Download Lecture Overview
    Report mistake
    Transcript

    00:01 Lastly, before we finish this lecture.

    00:03 We're briefly going to consider the idea of the center of gravity.

    00:06 We're going to do this so briefly because we will see how the center of gravity is related to the center of mass which we've already discussed.

    00:12 We'll introduce this topic as brief topic by a way of a quick example which asks us to find the center of gravity for a system of two masses, 10 kg and 5 kg, located respectively at 1 and 4 meters away from the origin.

    00:27 The way the center of gravity is defined is very similar to the center of mass.

    00:31 Say, the position X of the center of gravity is simply going to be again, the forces of gravity times the position of the object.

    00:49 In other words, what I'm saying here is that we have force of gravity on object one times its position plus the force of gravity on object two times its position plus any other object you have on your system.

    00:59 And just like we did with the center of mass, we do want a position, a position coordinate at the end of the day and so we need to divide by the units of force.

    01:07 We'll add up all of our forces, all of our gravitational forces acting on our object, however many there are.

    01:14 And so in this problem we only have two masses, so let's just write down with the gravitational forces for these two objects.

    01:22 We again have a gravitational force, we have mass 1 times gravity, is its force, times its position, plus mass two times gravity times its position divided by and again the sum of the gravitational forces.

    01:41 And now we get to see why this is such a simple idea, the center of gravity relative to the center of mass, because look what happens to this factor of G in the numerator and denominator.

    01:51 We can factor this out. And then I'll factor it out from the denominator as well.

    02:02 And then we see immediately what happen is that these factors of G cancel.

    02:09 The expression that we have left here after we've cancel our factors of G, looks exactly like the equation that we have for the center of mass.

    02:16 We have masses times their positions, all added up divided by the total mass of our system and so the center of gravity will be in fact exactly the same as the center of mass when and only when these factors of G where able to be factored out from the numerator and denominator and be the same for each object in our system.

    02:34 So the only time that the center of gravity might be different from the center of mass is if you have some more exotic questions or a strange system or maybe have a big object or maybe object in space that are being experience by different amounts of gravity.

    02:47 But these are more atypical situations are not something we're going to have to worry about.

    02:51 And so for our case again, we can cancel these factors of G and actually plug in our values and see what we get.

    02:57 So here we have mass 1 is equal to 10 kg is multiplied by its distance which is 1 meter, plus our second mass which is 5 kg times its position which is 4 meters and then again we'll divided by the total sum of the mass which is 10 kg plus 5 kg.

    03:14 And so all we have to do is simplify here. We have 10 plus 20, divided by 15.

    03:19 This is 30 divided by 15, which is simply 2 meters.

    03:25 And so our center of gravity as at a position of 2 meters which is located between the two masses that we've introduced.

    03:32 This finishes our quick discussion of the center of gravity and this lecture covering torque, equilibrium and systems and the center of gravity.

    03:39 Thanks for watching.


    About the Lecture

    The lecture Center of Gravity by Jared Rovny is from the course Equilibrium.


    Included Quiz Questions

    1. They are the same if each object experiences the same gravitational acceleration.
    2. They are the same always.
    3. They are different always.
    4. They are the same if all the objects are experiencing force according to Newton’s law of gravity.
    5. They always have different units.
    1. The center of mass and the center of gravity will be at x=0
    2. The center of mass will be at x=0, but the center of gravity will depend on the masses.
    3. The center of gravity will be at x=0, but the center of mass will depend on the masses.
    4. The center of mass and the center of gravity will depend on the masses.
    5. The center of mass and the center of gravity will depend on the location of the masses.
    1. distance (like meters), and distance (like meters)
    2. mass (like kilograms), and gravity (like Newtons)
    3. mass (like kilograms), and gravity (like meters per second squared)
    4. distance (like meters), and gravity (like Newtons)
    5. mass (like kilograms), and gravity (like Newtons)

    Author of lecture Center of Gravity

     Jared Rovny

    Jared Rovny


    Customer reviews

    (1)
    5,0 of 5 stars
    5 Stars
    5
    4 Stars
    0
    3 Stars
    0
    2 Stars
    0
    1  Star
    0