Rigid Body in Equilibrium

Slides:



Advertisements
Similar presentations
Mechanics of Rigid Body. C
Advertisements

Physics 111: Mechanics Lecture 12
Rotational Equilibrium and Rotational Dynamics
Statics Worksheet Solutions
Chapter-9 Rotational Dynamics
Q12. Static Equilibrium.
AP Physics. The angle “ θ ” used to represent rotational position  Units: radians or degrees (remember 2 π rad = 360 o ) Change in rotational position.
Physics 7C lecture 15 Quilibrium
 PROGRAM OF “PHYSICS” Lecturer: Dr. DO Xuan Hoi Room 413
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.
PHYS16 – Lecture 26 Ch. 12 Static Equilibrium. Static Equil. Pre-question If ball 2 has twice the mass of ball 1 and the system is in static equilibrium.
1. How is torque calculated?. Torque = Force X length of torque arm T = F x l.
Chapter 8 Rotational Equilibrium and Rotational Dynamics.
Chapter 12: Static Equilibrium Conditions for equilibrium  First condition for equilibrium When a particle is in equilibrium (no acceleration), in an.
Chapter 8 Rotational Equilibrium and Rotational Dynamics.
Torque.
Reading Quiz 1. Viscous friction is
Physics 106: Mechanics Lecture 07
Physics 106: Mechanics Lecture 08
Physics 151: Lecture 26 Today’s Agenda
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.
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
Classical Mechanics Review 4: Units 1-19
Chapter-9 Rotational Dynamics. Translational and Rotational Motion.
Static Conditions of Equilibrium: Static Equilibrium:
Chapter 9 Torque.
Equilibrium of a Rigid Body
Wednesday, Nov. 12, 2003PHYS , Fall 2003 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #19 Wednesday, Nov. 12, 2003 Dr. Jaehoon Yu 1.Conditions.
Torque and Equilibrium Practice
Static Equilibrium (Serway ) Physics 1D03.
1© Manhattan Press (H.K.) Ltd. 1.5 Static equilibrium of a rigid body.
Torque Rotational Dynamics. There are 3 types of motion Translational Rotational Vibrational.
Home work Thesis 1. Hair tension and it’s applications 2. Frictions and their applications 3. Frictional reduction 4. The moon movements 5. Water moving.
Rotational Motion and Equilibrium
Chapter 8 Rotational Motion.
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.
ROTATION AND INERTIA Chapter 8 Section 2. Center of Mass  Center of Mass – The point at which all the mass of the body can be considered to the concentrated.
-More on Center of Gravity -More on Static Equilibrium
Rotational Motion 1. Translational Motion vs. Rotational Motion Translational motion ___________ ______________________________ Example: motion of a bullet.
First condition of equilibrium: Fnet = 0
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.
Definition of Torque Statics and Dynamics of a rigid object
Spring 2002 Lecture #17 Dr. Jaehoon Yu 1.Conditions for Equilibrium 2.Center of Gravity 3.Elastic Properties of Solids Young’s Modulus Shear Modulus.
Wednesday, Apr. 7, 2004PHYS , Spring 2004 Dr. Jaehoon Yu 1 PHYS 1441 – Section 004 Lecture #18 Wednesday, Apr. 7, 2004 Dr. Jaehoon Yu Torque Moment.
Chapter 8 Review. 1. How is torque calculated? T = F x l.
Torque and Equilibrium
Statics. Identifying Static Situations Objects that do not move linearly (translational motion) or rotate (rotational motion) are static.
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.
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.
Ying Yi PhD Chapter 9 Rotational Dynamics 1 PHYS HCC.
Wednesday, Nov. 13, 2002PHYS , Fall 2002 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #17 Wednesday, Nov. 13, 2002 Dr. Jaehoon Yu 1.Conditions.
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.
PHYS 298 Spring 2017 Week 10: Conservation of angular momentum
PHYS 1443 – Section 003 Lecture #19
This is the same as both situations above Springs and Hooke’s Law k is the “force constant”
Classical Mechanics Review 4: Units 1-22
Static Equilibrium and Torque
Wednesday, May 9 noon-1:50PM
Torque.
PHYS 1443 – Section 003 Lecture #17
PHYS 1443 – Section 501 Lecture #22
Aim: How do we explain torque?
Figure 12.1  A single force F acts on a rigid object at the point P.
Chapter 9 Torque.
Rotational Statics i.e. “Torque”
Statics.
Rigid Body in Equilibrium
Presentation transcript:

Aim: How do we explain applications of Newton’s Second Law for Rotation?

Rigid Body in Equilibrium Two conditions for Complete Equilibrium of an object: The net external force must equal zero The net external torque must be zero about any axis ∑F = 0 Translational Equilibrium ∑τ = 0 Rotational Equilibrium

Thought Question Is it possible to have a situation in which an object is in translational equilibrium but not rotational equilibrium? Yes, an accelerating wheel Is it possible to have a situation in which an object is in rotational equilibrium but not translational equilibrium? Yes, an object that slides while accelerating

Static Equilibrium Object is at rest with no angular speed. ω=0 and vcm = 0

Seasaw Problem Two children weighing 500 N and 350 N are on a uniform board weighing 40 N supported at its center. If the 500 N child is 1.50 m from the center, determine where the 350 N child must sit to balance the system τ1=τ2 r1F1=r2F2 1.5(500)=r(350) r=2.14 m b) The upward force exerted on the board by the support ΣF = 0=500 + 350+40 + Fp Fp=890 N

Seasaw a) 2.14 m from center b) 890 N

Standing on a Horizontal Beam A uniform horizontal beam of length 8.00 m and weight 200 N is attached to a wall by a pin connection. Its far end is supported by a cable that makes an angle of 53 degrees with the horizontal. If a 600 N man stands 2.00 m from the wall, find the tension in the cable and the force exerted by the wall on the beam.

Standing on a Horizontal Beam T=313 N and R=581 N

Leaning Ladder Problem A uniform ladder of length l and mass m rests against a smooth, vertical wall. If the coefficient of static friction between the ladder and ground is μs=0.40, find the minimum angle θmin such that the ladder does not slip.

Leaning Ladder Problem