Chap 11.20.

Slides:



Advertisements
Similar presentations
December 4 AP Physics.
Advertisements

Find the tension T in each cable and the magnitude and direction of the force exerted on the strut by the pivot in each of the arrangements in Fig. below.
Equilibrium and Torque
Equilibrium An object is in “Equilibrium” when:
CH12.Problems JH.131. Take the lower center as rotation center then: M2 (L/4) = M3 (3L/4)  M2= 3 M3 Now the upper center: M1 (L/4) = (M2+M3)
Forces and moments Resolving forces.
Torque Physics 6A Prepared by Vince Zaccone
Static Equilibrium Physics 2 Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Q12. Static Equilibrium.
Quiz * Vector A has a magnitude of 4 units and makes an angle of 37°
Make a sketch Problem: A 10.0 kg box is pulled along a horizontal surface by a rope that makes a 30.0 o angle with the horizontal. The tension in the rope.
Forces applied at an Angle & Inclined Planes
Chapter 9 Torque.
12. Static Equilibrium.
CHAPTER 8 Rotational Equilibrium Torque: Torque: The tendency of a force to rotate a body about some axis. d F  = F d  = F · d (in this situation) Lever.
The Turning Effect of Forces You should be able to: state what the centre of gravity of an object is. describe a simple experiment to determine the centre.
Torque problem 9-33 The uniform gate in the diagram below has a mass of 51.0 kg. Assume that the force exerted on the gate by the upper hinge acts in the.
1. How is torque calculated?. Torque = Force X length of torque arm T = F x l.
Force applied at a distance causing a rotating effect
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.
 Point at which all other points on the object rotate around  During motion the CM will move in the same path that a simple particle would move if subjected.
Equilibrium of Particles Free-body Diagram Equilibrium of Rigid Bodies
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.
T082 Q1. A uniform horizontal beam of length 6
An Introduction to Statics Unit 3, Presentation 4.
Chapter 9 Torque.
Why did the bridge fall into the Mississippi River?  bridge+collapse&total=206&start=0&num=10&so=0&type=search&plindex=1.
Physics 111 Practice Problem Statements 12 Static Equilibrium SJ 8th Ed.: Chap 12.1 – 12.3 Contents 13-5, 13-7, 13-17*, 13-19*, 13-20, 13-23, 13-25, 13-28*,
Statics: Torque Equilibrium TTorque Equilibrium How to solve Example Whiteboards Torque and force Example Whiteboards.
Review for Dynamics test Page 1Page 1 - Net force with weight Page 2Page 2 - Friction on a level surface Page 3 Page 3 - Inclined Plane Page 4 Page 4.
Torque and Equilibrium Practice
Waterballoon-face collision
PARALLEL FORCES Forces that act in the same or opposite directions at different points on an object.
Static Equilibrium (Serway ) Physics 1D03.
Statics: Trans. and Tors.. Force Equilibrium: 1.Draw Picture 2.Calculate weights 3.Express/calculate components 4.Set up a = 0 equation for x and another.
Derivation of the proportionality of velocity and radius for an object in circular motion under a constant centripetal force.
Torque Rotational Dynamics. There are 3 types of motion Translational Rotational Vibrational.
Chapter 8: Equilibrium and Mechanical Advantage
Applications & Examples of Newton’s Laws. Forces are VECTORS!! Newton’s 2 nd Law: ∑F = ma ∑F = VECTOR SUM of all forces on mass m  Need VECTOR addition.
Lecture 17: Torque & Rotational Equilibrium. Questions of Yesterday You are riding on a Ferris wheel moving at constant speed. 1a) At what point is the.
Chapter 11 Equilibrium. If an object is in equilibrium then its motion is not changing. Therefore, according to Newton's second law, the net force must.
Problem 4-c 1.2 m y 1.5 m z x 5 kN A B C E D  1 m 2 m A 3-m pole is supported by a ball-and-socket joint at A and by the cables CD and CE. Knowing that.
Chap 5: 8 The Tow Truck. Model the Problem Forces on Car Cable Gravity Ramp Net Force.
Applications & Examples of Newton’s Laws. Forces are VECTORS!! Newton’s 2 nd Law: ∑F = ma ∑F = VECTOR SUM of all forces on mass m  Need VECTOR addition.
1. The following diagram shows a system of forces acting on a particle in a plane. A third force is added so that the particle rests in equilibrium. Find.
The centre of gravity is that point at which the sum of the gravitational forces due to all individual masses comprising the system appears to act. The.
AP Chapter 4. Force - a push or pull Contact Force – Noncontact Force – mass.
Equilibrium. The First Condition of Equilibrium In a situation involving equilibrium, there is no acceleration (no change in velocity). Thus the net force.
EQUILIBRIUM The sum of the forces is zero. The acceleration is zero. ΣF = 0 a=0.
More About Force 3) When one object exerts a force on a second object, the second exerts an equal and opposite force on the first. F AB = -F BA.
Chapter 8 Rotational Equilibrium and Rotational Dynamics
Today: (Ch. 3) Tomorrow: (Ch. 4) Forces and Motion in Two and Three Dimensions Equilibrium and Examples Projectile Motion.
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.
Question 3 in section 7.6 of the AS Text Book 10m 6m A crane is used to raise one end of a 15kN girder of length 10.0m off the ground. When the end of.
How do you start the rotation of an object? How do you open an door? What did we learn about the best way to open a door? The most efficient way to open.
Chapter 12. Rotation of a Rigid Body
Force Equilibrium: Torque Equilibrium: Do Maths
Introduction to Torque
Torque not at 90o.
Moment of a Force.
Steps to Solving a Force Problem
Introduction to Torque
Equilibrium Chapter 9.
Chapter 9 Torque.
Aim: How do we solve static equilibrium problems?
Static Equilibrium.
Presentation transcript:

Chap 11.20

11. 20 A nonuniform beam 4. 50 m long and weighing 1 11.20 A nonuniform beam 4.50 m long and weighing 1.00 kN makes an angle of 25° below the horizontal. It is held in position by a frictionless pivot at its upper right end and by a cable 3.00 m farther down the beam and perpendicular to it. The center of gravity of the beam is 2.00 m down the beam from the pivot. Lighting equipment exerts a 5.00-kN downward force on the lower left end of the beam. Find the tension T in the cable and the horizontal and vertical components of the force exerted on the beam by the pivot. Start by sketching a free-body diagram of the beam

Forces on the Beam Gravity (of Beam) Cable Weight of Lamp Pivot Horizontal Vertical Gravity (weight of) Beam 0 −1kN Cable (tension)  C − C cos65° C sin65° Weight of Lamp 0 − 5kN Pivot Px Py Horizontal Equation: 0 − C cos65°+ 0 + Px = 0 Vertical Equation: − 1kN + C sin65° − 5kN + Py = 0

Torque Torque (fulcrum is Pivot) = F x d = F ∙ d⊥ Gravity (of Beam) + 1kN ∙ 2cos25° Cable − C ∙ 3 Weight of Lamp + 5kN ∙ 4.5 cos25° Pivot distance is 0 0 Equation: + 1kN ∙ 2cos25° − 3C + 5kN ∙ 4.5cos25° + 0 = 0

Solving Torque Eq: + 1kN ∙ 2cos25° − 3C + 5kN ∙ 4.5cos25° + 0 = 0 (2kN+22.5kN) ∙ cos25° = 3C C = 24.5kN cos25° / 3 = 24500 N x .9063/3 = 7401 N Horizontal Eq: 0 − C cos65°+ 0 + Px = 0 Px = C cos65° = 7401 * .4226 = 3128 N Vertical Eq: − 1kN + C sin65° − 5kN + Py = 0 Py = 6kN − C sin65° = 6000N – .9063*7401 N = 6000N – 6708N = – 708 N

Another Look