Motion, Forces, and Energy in More Than One Dimension
... vertical acceleration; as we just argued, a vertical acceleration can only produce changes in the vertical component of velocity. So if there is no horizontal motion to start with, gravity can’t produce any. But suppose the object is moving with some initial horizontal component of velocity; what do ...
... vertical acceleration; as we just argued, a vertical acceleration can only produce changes in the vertical component of velocity. So if there is no horizontal motion to start with, gravity can’t produce any. But suppose the object is moving with some initial horizontal component of velocity; what do ...
Newton`s Second Law of Motion
... Consider a cart pushed along a track with a certain force. If the force remains the same while the mass of the cart decreases to half, the acceleration of the cart ...
... Consider a cart pushed along a track with a certain force. If the force remains the same while the mass of the cart decreases to half, the acceleration of the cart ...
Rotational Dynamics SL and Honors 2016 2017
... B.1 – Rigid bodies and rotational dynamics (CORE) Essential idea: The basic laws of mechanics have an extension when equivalent principles are applied to rotation. Actual objects have dimensions and they require the expansion of the point particle model to consider the possibility of different poin ...
... B.1 – Rigid bodies and rotational dynamics (CORE) Essential idea: The basic laws of mechanics have an extension when equivalent principles are applied to rotation. Actual objects have dimensions and they require the expansion of the point particle model to consider the possibility of different poin ...
Work-Kinetic Energy Theorem for Rotational Motion
... W 12 I 2f 12 Ii2 K Rf K Ri Conservation of energy is also valid for rotational systems We can also show that W which is the angular equivalent of W Fd . You are not responsible for W , but it is yet another relationship that is very similar to a linear equation. ...
... W 12 I 2f 12 Ii2 K Rf K Ri Conservation of energy is also valid for rotational systems We can also show that W which is the angular equivalent of W Fd . You are not responsible for W , but it is yet another relationship that is very similar to a linear equation. ...
Unit 5 Part 1 Simple Harmonic Motion Notes
... complete back and forth cycle). Notice the period is only dependent upon the mass of the oscillating body and the spring constant, . As the stiffness of the spring increases (as k increases), the period decreases (it takes less time to complete one cycle) so the object on the spring moves faster (wh ...
... complete back and forth cycle). Notice the period is only dependent upon the mass of the oscillating body and the spring constant, . As the stiffness of the spring increases (as k increases), the period decreases (it takes less time to complete one cycle) so the object on the spring moves faster (wh ...
Newton`s Third Law 1.0
... Road pushes forward on Tires (explains how a car moves) Gas pushes forward on Rocket (explains how a jet moves) Table pushes up on Book Moon pulls up on Earth Nail pulls right on Magnet ...
... Road pushes forward on Tires (explains how a car moves) Gas pushes forward on Rocket (explains how a jet moves) Table pushes up on Book Moon pulls up on Earth Nail pulls right on Magnet ...
Lab7_StaticEquilibrium
... the lever arm, d, or = d F. For the wheel in Figure 1 the lever arm for F2 is equal to the radius of the wheel, while the lever arm for F1 is zero. Why? Furthermore, torque is a vector and so we can specify its direction. (Torque is actually something called a pseudo vector, but don’t worry about ...
... the lever arm, d, or = d F. For the wheel in Figure 1 the lever arm for F2 is equal to the radius of the wheel, while the lever arm for F1 is zero. Why? Furthermore, torque is a vector and so we can specify its direction. (Torque is actually something called a pseudo vector, but don’t worry about ...
