Torque. Center of Gravity The point at which all the weight is considered to be concentrated The point at which an object can be lifted w/o producing.

Slides:



Advertisements
Similar presentations
Mechanics of Rigid Body. C
Advertisements

Torque Rotational Equilibrium Rotational Dynamics
1. A motorcycle plus rider has a mass of 1000 kg. They travel inside a loop with a radius of 6 m. At the lowest point, the speed is 20 m/s. What force.
Torque and Equilibrium
1 UCT PHY1025F: Mechanics Physics 1025F Mechanics Dr. Steve Peterson EQUILIBRIUM.
 In Chap. 6 we studied the equilibrium of point- objects (mass m) with the application of Newton’s Laws  Therefore, no linear (translational) acceleration,
PHYS 218 sec Review Chap. 11 Equilibrium and Elasticity.
Force vs. Torque Forces cause accelerations
(W= weight!) W = m  g The main force acting on the body is the gravitational force! Gravitational force W applies at the center of gravity CG of the.
1. How is torque calculated?. Torque = Force X length of torque arm T = F x l.
Torque and Center of Mass
Force applied at a distance causing a rotating effect
Chapter 8 Rotational Equilibrium and Rotational Dynamics.
Torque and Rotational Equilibrium
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.
MHS Physics Department AP Unit I E 2 Torque and rotational statics.
Physics 106: Mechanics Lecture 07
Physics 106: Mechanics Lecture 08
Statics. Static Equilibrium  There are three conditions for static equilibrium. 1.The object is at rest 2.There is no net force 3.There is no net torque.
Statics. Static Equilibrium  There are three conditions for static equilibrium. 1.The object is at rest 2.There is no net force 3.There is no net torque.
D. Roberts PHYS 121 University of Maryland Physic² 121: Phundament°ls of Phy²ics I November 15, 2006.
First condition of equilibrium: Fnet = 0
Equilibrium of a Rigid Body
Chapter 7 Rotational Motion.
ROTATIONAL MOTION AND EQUILIBRIUM
AP Physics B I.E Circular Motion and Rotation. I.E.1 Uniform Circular Motion.
Torque and Equilibrium Practice
Waterballoon-face collision
PARALLEL FORCES Forces that act in the same or opposite directions at different points on an object.
© John Parkinson 1 WHAT WAS THAT? © John Parkinson 2 MOMENTS.
Motion and Forces in 2 and 3 Dimensions Torque and Rotation.
Chapter 8 Statics Statics. Equilibrium An object either at rest or moving with a constant velocity is said to be in equilibrium An object either at rest.
Center of Mass, Moment of Inertia, & Rotational Equilibrium Rotation Physics Mr. McCallister.
Torque Rotational Dynamics. There are 3 types of motion Translational Rotational Vibrational.
Rotational Equilibrium & Dynamics
Chapter 12 Equilibrium and elasticity. Equilibrium We already introduced the concept of equilibrium in Chapter 8: dU(x)/dx = 0 More general definition.
Torque DO NOW: Serway Read Pages 306 – 308 Do Example page 309 Define and Utilize : Moment.
Physics 106 Lesson #2 Static Equilibrium Dr. Andrew Tomasch 2405 Randall Lab
Lots of fun! Win valuable prizes!. 1. Two people sit on a balanced seesaw. When one person leans toward the center of the seesaw, that person's end of.
First condition of equilibrium: Fnet = 0
Chapter 7-8 Pretest.
Chapter 8 Review. 1. How is torque calculated? T = F x l.
Torque and Equilibrium
Equilibrium. The First Condition of Equilibrium In a situation involving equilibrium, there is no acceleration (no change in velocity). Thus the net force.
Chapter 12 Lecture 21: Static Equilibrium and Elasticity: I HW8 (problems):11.7, 11.25, 11.39, 11.58, 12.5, 12.24, 12.35, Due on Friday, April 1.
Chapter 8 Rotational Equilibrium and Rotational Dynamics
Copyright Sautter The next slide is a quick promo for my books after which the presentation will begin Thanks for your patience! Walt S.
Ying Yi PhD Chapter 9 Rotational Dynamics 1 PHYS HCC.
1 Rotational Dynamics The Action of Forces and Torques on Rigid Objects Chapter 9 Lesson 2 (a) Translation (b) Combined translation and rotation.
Torque & Equilibrium AP Physics.
© 2010 Pearson Education, Inc. PowerPoint ® Lectures for College Physics: A Strategic Approach, Second Edition Chapter 7 Rotational Motion.
Physics book - Ch 9 Conceptual Book – Ch 11
Ch 8 : Rotational Motion .
Torque.
Introduction to Torque
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.
Torque at 90o This has NOTHING to do with torque but it comes up when you google images…go figure.
Ch. 8 Rotational Motion.
Torque and Equilibrium
Rotational Dynamics.
Equilibrium and Torque
Torque not at 90o.
Rotational Inertia 8.2.
Chapter 10:Dynamics of Rotational Motion
Moment of a Force.
Rigid Body in Equilibrium
Introduction to Torque
Physics 101: Lecture 14 Torque and Equilibrium
Rotational Statics i.e. “Torque”
Rigid Body in Equilibrium
Presentation transcript:

Torque

Center of Gravity The point at which all the weight is considered to be concentrated The point at which an object can be lifted w/o producing rotation

Center of Gravity In asymmetric objects, the center of gravity may not be the geometric center

Translational Equilibrium Occurs when an object is not accelerating

Rotational Equilibrium Occurs when an object is not rotating or the rotation is uniform

Torque The rotational effect of an object produced by a net force that is not applied to the center of gravity

WAWA WBWB A B C Torque arm C = Pivot Point or Center of rotation FTFT

Pivot Point Reference point from which to measure rotational forces

Torque Arm The length between the pivot point and the point where a force is applied

Torque The product of the applied force and the length of its torque arm:

WAWA WBWB A B C Torque arm 6 m 4 m FTFT Torque A = W A x 6 m Torque B = W B x 4 m

Torque Arm A WAWA WBWB Torque Arm B A B Torque A = W A Acos  Torque B = W B Bcos    FTFT

FAFA FNFN  F N = F A sin   l sin  Torque =F A l sin 

Calculate the torque on a 250 cm rod with a pivot point at one end and a g object sitting on the other end

A person ties a rope to one end of a 10.0 m I- beam & tries lift it by pulling with 2500 N at 37 o from horizontal