Torque Physics 6A Prepared by Vince Zaccone

Slides:



Advertisements
Similar presentations
Torque and Rotation Physics.
Advertisements

Equilibrium and Torque
Torque Torque is defined as the tendency to produce a change in rotational motion.
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: Rotational Statics and Rotational Dynamics Honors Physics.
Torque Physics 2 Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Lecture 15 Rotational Dynamics.
Static Equilibrium Physics 2 Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Torque We know that Newton’s second law ( ) explains that the net force is the source of an object’s acceleration. What is the source of.
Chapter-9 Rotational Dynamics
Torque and Equilibrium
Chapter 9 Rotational Dynamics.
1 UCT PHY1025F: Mechanics Physics 1025F Mechanics Dr. Steve Peterson EQUILIBRIUM.
Equilibrium is not just translational, is is also rotational. While a set of forces may not change the velocity of an object, it may change its speed of.
A ladder with length L weighing 400 N rests against a vertical frictionless wall as shown below. The center of gravity of the ladder is at the center of.
Force vs. Torque Forces cause accelerations
Rotational Equilibrium and Rotational Dynamics
Physics 111: Mechanics Lecture 10 Dale Gary NJIT Physics Department.
Chapter 9 – Rotational Dynamics
Chapter 9: Torque and Rotation
Rotational Equilibrium and Rotational Dynamics
Torque and Equilibrium Lecture 8 Pre-reading : KJF §8.1 and 8.2.
Rotational Dynamics and Static Equilibrium. Torque From experience, we know that the same force will be much more effective at rotating an object such.
 orque  orque  orque  orque  orque  orque  orque  orque  orque Chapter 10 Rotational Motion 10-4 Torque 10-5 Rotational Dynamics; Torque and Rotational.
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.
Torque.
Chapter 4 : statics 4-1 Torque Torque, , is the tendency of a force to rotate an object about some axis is an action that causes objects to rotate. Torque.
Rotational Motion – Part II
Physics 106: Mechanics Lecture 03
Physics 2 Chapter 10 problems Prepared by Vince Zaccone
Physics 106: Mechanics Lecture 02
D. Roberts PHYS 121 University of Maryland Physic² 121: Phundament°ls of Phy²ics I November 15, 2006.
Chapter 8 Rotational Equilibrium and Rotational Dynamics.
Rotational Equilibrium and Rotational Dynamics
Chapter-9 Rotational Dynamics. Translational and Rotational Motion.
Chapter 8: Torque and Angular Momentum
Chapter 9 Torque.
Rotational Equilibrium and Rotational Dynamics
Chapter 9: Rotational Dynamics
ROTATIONAL MOTION AND EQUILIBRIUM
Torque Chap 8 Units: m N 2.
Rotational Motion Honors Physics. Rotational Motion Objectives: Learn how to describe and measure rotational motion Learn how torque changes rotational.
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.
Chapter 8 Rotational Motion.
Two blocks (m 1 =2.5kg, m 2 =1.8kg) are hanging from a pulley as shown in the figure below. The moment of inertia through the axis of rotation passing.
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.
Torque Rotational Dynamics. There are 3 types of motion Translational Rotational Vibrational.
Torque. So far we have analyzed translational motion in terms of its angular quantities. But we have really only focused on the kinematics and energy.
Physics CHAPTER 8 ROTATIONAL MOTION. The Radian  The radian is a unit of angular measure  The radian can be defined as the arc length s along a circle.
Rotational Dynamics and Static Equilibrium
Chapter 9 Rotational Dynamics.
Rotational Motion – Dynamics AP Physics. Rotational and Translational Equalities Rotational Objects roll Inertia TORQUE Angular Acceleration Rotational.
Rotational Dynamics Rode, Kiana, Tiana, and Celina.
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.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 11 Physics, 4 th Edition James S. Walker.
– Rotational displacement is how far the object rotates. Units: fractions of a complete revolution; degrees; radians 1 complete revolution = 360º = 2 
Ying Yi PhD Chapter 9 Rotational Dynamics 1 PHYS HCC.
Monday, Apr. 14, 2008 PHYS , Spring 2008 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #21 Monday, Apr. 14, 2008 Dr. Jaehoon Yu Rolling Motion.
1 Rotational Dynamics The Action of Forces and Torques on Rigid Objects Chapter 9 Lesson 2 (a) Translation (b) Combined translation and rotation.
Mechanics Lecture 17, Slide 1 Physics 211 Lecture 17 Today’s Concepts: a) Torque Due to Gravity b) Static Equilibrium Next Monday 1:30-2:20pm, here: Hour.
9.1 Torque 1.
Objectives Calculate the torque created by a force.
Torque not at 90o.
Torque.
Torque and Rotation Physics.
Chapter 9 Torque.
Rotational Statics i.e. “Torque”
Presentation transcript:

Torque Physics 6A Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque Torque is what causes angular acceleration (just like a force causes linear acceleration) Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque Torque is what causes angular acceleration (just like a force causes linear acceleration) For a torque to be applied to an object, there needs to be a force that acts at some distance away from a pivot point. For example, consider tightening a bolt with a wrench. Which of the 3 forces shown will tighten the bolt? Pivot Point FA FC FB Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque Torque is what causes angular acceleration (just like a force causes linear acceleration) For a torque to be applied to an object, there needs to be a force that acts at some distance away from a pivot point. For example, consider tightening a bolt with a wrench. Which of the 3 forces shown will tighten the bolt? Pivot Point FA Force B will tend to rotate the bolt clockwise, which will tighten it. FC FB Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque Torque is what causes angular acceleration (just like a force causes linear acceleration) For a torque to be applied to an object, there needs to be a force that acts at some distance away from a pivot point. For example, consider tightening a bolt with a wrench. Which of the 3 forces shown will tighten the bolt? Pivot Point FA Force B will tend to rotate the bolt clockwise, which will tighten it. Notice that force A will tend to rotate the bolt counter-clockwise, loosening it. What does force C do? FC FB Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque Torque is what causes angular acceleration (just like a force causes linear acceleration) For a torque to be applied to an object, there needs to be a force that acts at some distance away from a pivot point. For example, consider tightening a bolt with a wrench. Which of the 3 forces shown will tighten the bolt? Pivot Point FA Force B will tend to rotate the bolt clockwise, which will tighten it. Notice that force A will tend to rotate the bolt counter-clockwise, loosening it. What does force C do? Force C doesn’t cause any rotation at all – there is no torque generated by force C. Why not? FC FB Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque Torque is what causes angular acceleration (just like a force causes linear acceleration) For a torque to be applied to an object, there needs to be a force that acts at some distance away from a pivot point. For example, consider tightening a bolt with a wrench. Which of the 3 forces shown will tighten the bolt? Pivot Point FA Force B will tend to rotate the bolt clockwise, which will tighten it. Notice that force A will tend to rotate the bolt counter-clockwise, loosening it. What does force C do? Force C doesn’t cause any rotation at all – there is no torque generated by force C. Why not? Force C points directly at the pivot point – no torque is created in this case. FC FB Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque Formula for torque: This is really just the magnitude of the torque. The angle in the formula is between the force and the radius (from the pivot point to where the force is applied). Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque Formula for torque: FA θ Pivot Point FA θ This is really just the magnitude of the torque. The angle in the formula is between the force and the radius (from the pivot point to where the force is applied). r Take a look at the diagram – r and θ are shown for force A. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque Formula for torque: FA θ Pivot Point FA θ This is really just the magnitude of the torque. The angle in the formula is between the force and the radius (from the pivot point to where the force is applied). r Take a look at the diagram – r and θ are shown for force A. There are 2 ways to interpret the formula. If you group the Fsin(θ) together, that represents the component of the force that is perpendicular to the radius. To get the most torque, the force should be applied perpendicular (can you see why from the formula?) Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque Formula for torque: FA θ Lever Arm Formula for torque: Pivot Point FA θ This is really just the magnitude of the torque. The angle in the formula is between the force and the radius (from the pivot point to where the force is applied). r Take a look at the diagram – r and θ are shown for force A. There are 2 ways to interpret the formula. If you group the F sin(θ) together, that represents the component of the force that is perpendicular to the radius. To get the most torque, the force should be applied perpendicular (can you see why from the formula?) The other option is to group the r sin(θ) together and call it the “lever arm” for the force. Think of this as the shortest distance from the pivot point to where the force is applied. This is the effective radius of the force. Again, to get maximum torque the angle should be 90°. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

F1 is applied at the right end, and F2 is at the center. F2=30N Example: Find the torque of each force shown with respect to the pivot point at the left end of the 2m long rod. F1 is applied at the right end, and F2 is at the center. F2=30N 120° 50° F1=20N Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

F1 is applied at the right end, and F2 is at the center. F2=30N Example: Find the torque of each force shown with respect to the pivot point at the left end of the 2m long rod. F1 is applied at the right end, and F2 is at the center. F2=30N 120° 50° We can simply use our definition of torque here. F1=20N Notice the sign convention: Counter-clockwise torque is positive. Clockwise torque is negative. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Torque We mentioned earlier that torques produce angular accelerations. We have a formula for this relationship: This is really just Newton’s 2nd law applied to rotational motion. The moment of inertia, I, takes the place of the mass, and we use angular acceleration instead of linear. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

F1 is applied at the right end, and F2 is at the center. F2=30N Example: Find the angular acceleration of the 2m long, uniform rod (mass=5kg) when it is subject to the 2 forces shown. F1 is applied at the right end, and F2 is at the center. F2=30N 120° 50° This is just like the last problem, so we can use the results here. We need to add up all the torques on the rod, then solve for . F1=20N Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

F1 is applied at the right end, and F2 is at the center. F2=30N Example: Find the angular acceleration of the 2m long, uniform rod (mass=5kg) when it is subject to the 2 forces shown. F1 is applied at the right end, and F2 is at the center. F2=30N 120° 50° This is just like the last problem, so we can use the results here. We need to add up all the torques on the rod, then solve for . F1=20N Look up this formula for the moment of inertia of a rod, with the axis at the end. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Static Equilibrium Sometimes an object is subject to several forces, but it does not accelerate. This is when the object is in equilibrium. We have done problems like this before, but we neglected the rotational motion. To incorporate this, we simply need to add a torque formula to our typical force formulas. Here’s an example: A uniform beam 4m long and weighing 2500N carries a 3500N weight 1.5m from the far end, as shown. It is supported by a hinge at the wall, and a metal wire running from the wall to the far end. Find the tension in the wire, and find the horizontal and vertical components of the force that the hinge exerts on the beam. 1.5m 60° Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

A uniform beam 4m long and weighing 2500N carries a 3500N weight 1 A uniform beam 4m long and weighing 2500N carries a 3500N weight 1.5m from the far end, as shown. It is supported by a hinge at the wall, and a metal wire running from the wall to the far end. Find the tension in the wire, and find the horizontal and vertical components of the force that the hinge exerts on the beam. 1.5m 60° We need to draw a diagram of all the forces, then write down force and torque equations: T Hy Hx 2500N 3500N T=Tension in wire Hx and Hy are the components of the force that the hinge exerts on the beam. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

We will save this equation and come back to it later. A uniform beam 4m long and weighing 2500N carries a 3500N weight 1.5m from the far end, as shown. It is supported by a hinge at the wall, and a metal wire running from the wall to the far end. Find the tension in the wire, and find the horizontal and vertical components of the force that the hinge exerts on the beam. 1.5m 60° We need to draw a diagram of all the forces, then write down force and torque equations: T Hy 30° Hx This could also be sin(60) We will save this equation and come back to it later. 2500N 3500N T=Tension in wire Hx and Hy are the components of the force the hinge exerts on the beam. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

We will save this equation and come back to it later. A uniform beam 4m long and weighing 2500N carries a 3500N weight 1.5m from the far end, as shown. It is supported by a hinge at the wall, and a metal wire running from the wall to the far end. Find the tension in the wire, and find the horizontal and vertical components of the force that the hinge exerts on the beam. 1.5m 60° We need to draw a diagram of all the forces, then write down force and torque equations: T Hy 30° Hx This could also be cos(60) We will save this equation and come back to it later. 2500N 3500N T=Tension in wire Hx and Hy are the components of the force the hinge exerts on the beam. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

A uniform beam 4m long and weighing 2500N carries a 3500N weight 1 A uniform beam 4m long and weighing 2500N carries a 3500N weight 1.5m from the far end, as shown. It is supported by a hinge at the wall, and a metal wire running from the wall to the far end. Find the tension in the wire, and find the horizontal and vertical components of the force that the hinge exerts on the beam. 1.5m 60° We need to draw a diagram of all the forces, then write down force and torque equations: T Hy Before we can fill in the torque equation we need to choose a pivot point. A convenient choice is where the hinge attaches to the beam. This simplifies the torque equation because the 2 unknown hinge forces will not create any torque about that point. Also, remember the sign convention – clockwise torques are negative and counterclockwise positive. 30° Hx Pivot point here 2500N 3500N T=Tension in wire Hx and Hy are the components of the force the hinge exerts on the beam. Now we can go back and substitute this value into the other equations to find the hinge forces. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB