Poll You push a bobsled on ice. There is a kinetic frictional force on the bobsled by the ice. The kinetic frictional force on the bobsled while you are.

Slides:



Advertisements
Similar presentations
Angular Quantities Correspondence between linear and rotational quantities:
Advertisements

Torque and Rotation Physics.
Torque Rotational Equilibrium Rotational Dynamics
Torque and Rotation Physics.
AP Physics. The angle “ θ ” used to represent rotational position  Units: radians or degrees (remember 2 π rad = 360 o ) Change in rotational position.
Centripetal Acceleration. Acceleration in a circular path at constant speed a c =(v t 2 )/r Centripetal acceleration=(tangential speed) 2 /radius of circular.
Physics Montwood High School R. Casao
Force vs. Torque Forces cause accelerations
Rotational Equilibrium and Rotational Dynamics
Chapter 9 – Rotational Dynamics
TorqueTorque A turning force. Torque (T) – a turning force Torque depends on the linear force applied and the distance from the fulcrum (pivot point)
1. How is torque calculated?. Torque = Force X length of torque arm T = F x l.
Seesaws 1 Seesaws. Seesaws 2 Introductory Question You and a child half your height lean out over the edge of a pool at the same angle. If you both let.
Chapter 8 Rotational Equilibrium and Rotational Dynamics.
Torque and Rotational Equilibrium
Rotational Mechanics.
Causing Rotational Motion In order to make an object start rotating about an axis, a force is required However, not only the amount of force applied but.
Rotational Equilibrium
Torque Torque is an influence which tends to change the rotational motion of an object. One way to quantify a torque is Torque = Force applied x lever.
Torque.
Chapter 8 Rotational Equilibrium and Rotational Dynamics.
Rotational Equilibrium and Rotational Dynamics
Rotation about a fixed axis
Chapter 9: Rotational Dynamics
Day 9, Physics 131.
ROTATIONAL MOTION AND EQUILIBRIUM
Torque and Rotation Physics. Torque Force is the action that creates changes in linear motion. For rotational motion, the same force can cause very different.
Circular Motion. Uniform Circular Motion Speed of object may be constant Velocity is constantly changing Direction of the velocity is tangent to the circle.
Motion and Forces in 2 and 3 Dimensions Torque and Rotation.
It’s time to anchor these concepts we have been talking about. Translational (linear) motion Rotational (circular) motion.
Rotational Kinetic Energy An object rotating about some axis with an angular speed, , has rotational kinetic energy even though it may not have.
Seesaws.
Rotational Motion 1. Translational Motion vs. Rotational Motion Translational motion ___________ ______________________________ Example: motion of a bullet.
1 Rotation of a Rigid Body Readings: Chapter How can we characterize the acceleration during rotation? - translational acceleration and - angular.
Angular Momentum. Angular Momentum ( L ) Conservation of Momentum The total angular momentum of a rotating object remains constant if the net torque.
Static Equilibrium Physics 150/250 Center of Mass Types of Motion
Chapter 8 Rotational Motion
Rotational Dynamics 8.3. Newton’s Second Law of Rotation Net positive torque, counterclockwise acceleration. Net negative torque, clockwise acceleration.
R F F F F MOMENT of FORCE = F x r.
Chapter 8 Review. 1. How is torque calculated? T = F x l.
Torque and Equilibrium
Application of Forces Learning Objectives:
Chapter 8: Rotational Equilibrium and Rotational Dynamics
This is the same as both situations above Springs and Hooke’s Law k is the “force constant”
AP Physics Review Rotational Motion.
Introducing: Motion and Forces
ROTATIONAL MOTION Rotation axis: rotation occurs about an axis that does not move: fixed axis.
Rotational Motion – Part II
College Physics, 7th Edition
Rotational Motion – Part II
Rotational Equilibrium and Dynamics
Ch. 8 Rotational Motion.
9.1 Torque 1.
Objectives Calculate the torque created by a force.
Net Force.
Torque A torque (due to a force) causes angular acceleration.
Torque.
Moments A moment of a force is a measure of its tendency to cause a body to rotate about a point or axis. It is the same as torque. A moment (M) is calculated.
Rigid Body in Equilibrium
Rotational Motion – Part II
Bell Work: Centripetal Motion
Collisions at an Angle The total momentum of the two football players prior to the collision is the vector sum of their individual momentums. The larger.
Rotational Motion – Part II
Rotational Motion – Part II
Rotational Motion – Part II
Rotational Motion – Part II
Moments and Centers of Mass
Rotational Motion – Part II
Rigid Body in Equilibrium
Tor-que? Statics II.
Presentation transcript:

Poll You push a bobsled on ice. There is a kinetic frictional force on the bobsled by the ice. The kinetic frictional force on the bobsled while you are pushing it Is always equal to kFN Depends on the acceleration of the bobsled Depends on the velocity of the bobsled. Depends on how hard you push it.

Poll Suppose that you push horizontally with a force F on the bobsled. There is also a frictional force fk on the bobsled. It moves in the +x direction. If it is speeding up, F > fk F < fk F = fk

Poll Suppose that you push horizontally with a force F on the bobsled. There is also a frictional force fk on the bobsled. It moves in the +x direction. If it is slowing down, F > fk F < fk F = fk

Poll Suppose that you push horizontally with a force F on the bobsled. There is also a frictional force fk on the bobsled. It moves in the +x direction. If it has a constant velocity F > fk F < fk F = fk

Center of Mass

Center of Mass

Equilibrium If the net force on an object is zero, then the center of mass of the object does not accelerate. This is called translational equilibrium.

See-saw

Torque F1 d1 Torque  = Fd where d is called the moment arm. If F causes counterclockwise rotation, then the torque by F on the object is positive. If F causes clockwise rotation, then the torque by B on the object is negative.

Equilibrium This condition keeps the object’s center of mass at rest (or uniform motion, actually). This condition keeps the object from rotating (or uniform rotation, actually). Translational equilibrium Rotational equilibrium

Example F1 d1 A child of mass 30 kg sits at the end of the seesaw at a distance of 3-m from the center of the seesaw. If a 90-kg adult wants to balance the child (so that the seesaw does not rotate), where should he sit?

Example Continued… F1 F2 d1 d2 What is the normal force on the seesaw by the fulcrum if the mass of the seesaw is 100 kg?

Hint on HW3 #4 F1 d1 d2 F2 What if F2 acts at an angle? Find F.

Hint on HW3 #3