Center of Mass. Consider motion of object as if all mass located at C of G.

Slides:



Advertisements
Similar presentations
Pulleys at an Angle. FBD-S m 1 = 100 kg m 2 = 300 kg 30° vivi 0 t10 s θ30° µ0 m1m1 100 kg m2m2 300 kg No Friction.
Advertisements

BA A = turning point B = position of 3 rd wheel/trace, mid way along beam C= possible counterweight position, above 3 rd wheel/trace C 0.87m Beams 0.9t.
Physics Subject Area Test
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.
Newton’s First & Second Law
L-10(M-9) torque and rotational inertia We consider the rotation of rigid bodies. A rigid body is an extended object in which the mass is distributed.
Foundations of Physics
Centre of Mass Created by J Harris
Center of Gravity Unit 6. Center of gravity- the point on an object located at the object’s average position of weight Symmetrical object (baseball)-
Torque and Center of Mass
Ch. 11 Rotational Mechanics Torque. TORQUE n Produced when a force is applied with leverage. n Force produces acceleration. n Torque produces rotation.
Alta High Conceptual Physics
Center of Gravity. Center of Gravity(CG): point located at the center of an object’s weight distribution. For symmetric object, it is located at geometric.
COMPOSITE BODIES (Section 9.3) Today’s Objective: Students will be able to determine the location of the center of gravity, center of mass, or centroid.
Example 8.1 The uniform crate has a mass of 20kg. If a force
Momentum is a Momentum vectors Impulse Defined as a Impulse is.
Physics 203 – College Physics I Department of Physics – The Citadel Physics 203 College Physics I Fall 2012 S. A. Yost Chapter 8 Part 3 Chapter 9 Angular.
12 Static Equilibrium and Elasticity Conditions for Equilibrium The Center of Gravity Some Examples of Static Equilibrium Omit sections 4, 5, 6. Stress.
 Force Due to Gravity. What’s the difference between Mass and Weight?  Mass (m) is the amount of material an object is made from. Also, mass is the.
Motion and Forces in 2 and 3 Dimensions Torque and Rotation.
Rotational Equilibrium & Dynamics
1© Manhattan Press (H.K.) Ltd. 1.7 Stability 2 © Manhattan Press (H.K.) Ltd. Stability 1.7 Stability (SB p. 75) What makes objects more stable than others?
Chapter 8: Equilibrium and Mechanical Advantage
Center of Mass AP Physics C Mrs. Coyle. Center of Mass The point of an object at which all the mass of the object is thought to be concentrated. Average.
Warm Up What is the tension in a 2.75 m cord that whirls a 5.6 kg object in a circular path at a speed of 4.83 m/s?
Center of Gravity. Definitions Center of gravity (c.g.) = the point located at the center of the object’s weight distribution Center of mass (c.m.) =
Chapter 10 Center of Gravity Center of Gravity Center of Gravity – (CG) the point at the center of its weight distribution.
Center of Gravity.
CG CM Center of Mass The Center of Mass (CM) of an object or objects is the point that moves as if all of the mass were concentrated there and all the.
Circular Motion / Rotational Mechanics Notes 5’s.
By: Brandon Chabala & Kyle Hahn.  Point at the center of an object’s weight distribution, where the force of gravity can be considered to act  All shapes.
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.
Project. Lesson #65 Topic: Center of Mass / Gravity Objectives: (After this class I will be able to) 1. Define center of gravity / mass 2. Locate an object’s.
12/25/20151FORCE BY DR AJAY KUMAR DAVV INDORE. 12/25/20152 Meaning& Nature of Force Force produces motion, stops motion and prevent motion. It may increase.
Where is the center or mass of a wrench?  Center-of-Mass A mechanical system moves as if all of its mass were concentrated at this point A very special.
Rotational Motion of an Object Physics Matters: Chapter 7.
Center of Mass Definition “The center of mass (or mass center) is the mean location of all the mass in a system” Marked with:
Center of Gravity Chapter 10.
Finding the Center of Mass (or gravity). Simplifying a system When we have a system such as a group of objects, or a complex structure with different.
Physics Chapter 8 – Rotational Motion Part 1.
Learning Objectives : 1.To understand Toppling and Toppling due to a slope Book Reference : Pages 102.
Loads & Forces. L1 L2 F2 F1 F1 x L1 = F2 x L2 F1 = (L2 x F2) L1 Formula for calculating load.
Newton’s Law of Universal Gravitation. Law of Universal Gravitation.
L-10 Torque and Rotational Motion
L-10 torque and rotational inertia
L-10(M-9) torque and rotational inertia
L-10 torque and rotational inertia
Rotational Equilibrium
Key Areas covered Resolving the weight of an object on a slope into a component acting down the slope and a component acting normal to the slope. Systems.
Ch. 8 Rotational Motion.
Foundations of Physics
EDEXCEL IGCSE / CERTIFICATE IN PHYSICS 1-5 The Turning Effect of Forces ’
12 Static Equilibrium and Elasticity
11.1 Torque To make an object turn or rotate, apply a torque.
L-10 torque and rotational inertia
Center of Gravity Chapter 10.
Example 7-12 A group of extended bodies, each with a known CM. Find the CM of the group.
Center of mass.
PHY131H1F - Class 19 Today, Chapter 12:
Stability and Centre of Gravity
Density Definition and Equation Examples
Key Areas covered Resolving the weight of an object on a slope into a component acting down the slope and a component acting normal to the slope. Systems.
Chapter 4 Force Ewen et al (2005)
Chapter 10 : Center of Gravity
TURNING EFFECT OF FORCES
Stable objects have: a low centre of gravity
Coverage of the 1st Long test
Center of Gravity Chapter 10.
EQUILIBRIUM AND CENTRE OF GRAVITY
Moments and Stability Elliott.
Presentation transcript:

Center of Mass

Consider motion of object as if all mass located at C of G.

Center of Gravity – Average position of weight Average position of mass Center of Mass –

C of M does not have to be on the object.

Locating Center of Gravity

Center of Gravity = Balance Point

m1m1 m2m2 m3m3 m4m4 A Στ A = m 1 gx 1 + m 2 gx 2 + m 3 gx 3 + m 4 gx 4 CM (m 1 +m 2 +m 3 +m 4 ) Στ A = (m 1 + m 2 + m 3 + m 4 )g x CM A

m 1 gx 1 + m 2 gx 2 + m 3 gx 3 + m 4 gx 4 (m 1 + m 2 + m 3 + m 4 )g x CM = m 1 x 1 + m 2 x 2 + m 3 x 3 + m 4 x 4 + … x CM = m 1 + m 2 + m 3 + m 4 + …

Calculating CM 2- dimensions Platform: 6.0 m x 6.0 m 100. kg 500. kg 3 corners CM?

Toppling Object is stable if its CG is above its base of support.

More stability if CG is low and base of support is wide.

Calculating Angle of Stability θ h b θ tan θ = h/bθ = tan -1 (h/b)

5.0 cm 8.0 cm To what angle can the block tip before it topples over? 58º

If CG is underneath base of support, object remains stable.