Linear Momentum Center of Mass

Size: px
Start display at page:

Download "Linear Momentum Center of Mass"

Transcription

1 Linear Momentum Center of Mass Lana Sheridan De Anza College Nov 14, 2017

2 Last time the ballistic pendulum 2D collisions center of mass finding the center of mass

3 Overview center of mass examples center of mass for continuous mass distributions

4 Center of Mass Last lecture we introduced the center of mass, the average point of the mass for a collection of particles: r CM = 1 m i r i M i This is a vector equation, so we can also express it as a set of component equations, one for each dimension.

5 Example Three technique Particles for determining athe plane es Figure 9.16 An experimental center of gravity of a wrench. A system consists of three particles located as shown. Find the center of mass of the system. The masses of the particles are m 1 = m 2 = 1.0 kg and m 3 = 2.0 kg. 8. Find the cenm kg and y (m) 3 2 m 3 Example 9.10) Two ated on the x axis, ticle is located on wn. The vector indin of the system s 1 0 S r CM m 1 m x (m) 3 he center of mass developed in this section. 1 Serway & Jewett, page 269.

6 Example dimensions: can find the x and y coordinates of the center of mass separately. Total mass, M = 2(1.0 kg) kg = 4 kg. x-direction: x CM = 1 m i x i M i = 1 M (m 1x 1 + m 2 x 2 + m 3 x 3 ) = 1 4 ( ) = 0.75 m

7 Example 9.10 x-direction: x CM = 0.75 m y-direction: y CM = 1 m i y i M i = 1 M (m 1y 1 + m 2 y 2 + m 3 y 3 ) = 1 ( ) 4 = 1.0 m

8 Example 9.10 x-direction: x CM = 0.75 m y-direction: y CM = 1 m i y i M i = 1 M (m 1y 1 + m 2 y 2 + m 3 y 3 ) = 1 ( ) 4 = 1.0 m Putting both components together: r CM = (0.75 i j) m

9 Continuous mass distribution On a microscopic scale we don t really believe mass is continuously distributed. (Atoms, etc.!) However, on a macroscopic scale it sure seems like it is, and its a very good approximation. It is also much easier than trying to describe every last atom / subatomic particle in a solid. We need to revise our previous center of mass (CM) definition to suit this case: 1 r CM = lim r i m i m i 0 M r CM = 1 r dm M i

10 Continuous mass distribution r CM = 1 r dm 9.6 The Center of Mass M 269 xtended object in (9.34) An extended object can be considered to be a distribution of small elements of mass m i. y.32 and lies on an axis of r of mass of a uniass of a sphere or s, each small mass all these forces is z S r i S r CM m i CM x

11 Discrete vs Continuous mass distribution Compare a discrete and continuous mass distribution along 1 dimension. Assume all particles have equal mass and each are separated by one meter. Where is the center of mass of this distribution? y x

12 Discrete vs Continuous mass distribution Compare a discrete and continuous mass distribution along 1 dimension. Assume all particles have equal mass and each are separated by one meter. Where is the center of mass of this distribution? y x

13 Discrete vs Continuous mass distribution y x The calculation would be: x CM = 1 m i x i M i

14 Discrete vs Continuous mass distribution y x The calculation would be: x CM = 1 m i x i M = 1 6m = 2.5 m i 5 m i The center of mass is at the midpoint of the line of point masses. i=0

15 Discrete vs Continuous mass distribution.75 i^ j^2 m Center of mass of a rod of uniform density. Density, ρ = M V, is mass per unit volume. Here however, we will consider a rod that can be treated as 1 dimensional. We need the mass per unit length: λ = M L. lies midway ength. y L dm = l dx.19, so y CM 5 ause we need Figure 9.19 (Example 9.11) The tion in Where Equa- is the center geometry of mass? used to find the center of mass of a uniform rod. x dx x

16 Discrete vs Continuous mass distribution.75 i^ j^2 m Center of mass of a rod of uniform density. Density, ρ = M V, is mass per unit volume. Here however, we will consider a rod that can be treated as 1 dimensional. We need the mass per unit length: λ = M L. lies midway ength. y L dm = l dx.19, so y CM 5 ause we need Figure 9.19 (Example 9.11) The tion in Where Equa- is the center geometry of mass? used to find the center of mass of a uniform rod. x dx x

17 Discrete vs Continuous mass distribution How to do the calculation: x CM = 1 x dm M = 1 x dm M Observe that dm = λ dx: x CM = 1 x(λ dx) M = 1 L M λ x dx 0

18 Discrete vs Continuous mass distribution Observe that dm = λ dx: x CM = 1 x(λ dx) M = 1 L M λ x dx 0

19 Discrete vs Continuous mass distribution Observe that dm = λ dx: x CM = 1 x(λ dx) M = 1 L M λ x dx 0 = 1 ( ) L 2 M λ 2 0 = 1 ( ) M L 2 M L 2 = L 2 In this case (uniform density) the center of mass is at the center of the rod.

20 established with a plumb bob) is drawn when the wrench has stopped swinging. The wrench is then hung from point C, and a second vertical line CD is drawn. The center of gravity is halfway through the thickness of the wrench, under the intersection of these two lines. In general, if the wrench is hung freely from any point, the vertical line through this point must pass through the center of gravity. Center of Mass Intuition Question Quick Quiz A baseball bat of uniform density is cut at the location of its center of mass as shown. Which piece has the smaller mass? (d) impossible to determine Q uick Quiz 9.7 A baseball bat of uniform density is cut at the location of its center of mass as shown in Figure Which piece has the smaller mass? (a) the piece on the right (b) the piece on the left (c) both pieces have the same mass Figure 9.17 (Quick Quiz 9.7) A baseball bat cut at the location of its center of mass. (A) the piece on the right Example 9.10 (B) the piece on the left The Center of Mass of Three Particles A system consists of three particles located as shown in Figure Find the center of mass of the system. The masses of the particles are m 1 5 m kg and m kg. (C) both pieces have the same mass (D) impossible to determine SOLUTIO N y ( 3 2 m Conceptualize Figure 9.18 shows the three masses. Your intuition should tell you that the 1 Serway & Jewett, page 269. Figure 9.18 (Example 9.10) Two particles are located on the x axis, and a single particle is located on 1

21 established with a plumb bob) is drawn when the wrench has stopped swinging. The wrench is then hung from point C, and a second vertical line CD is drawn. The center of gravity is halfway through the thickness of the wrench, under the intersection of these two lines. In general, if the wrench is hung freely from any point, the vertical line through this point must pass through the center of gravity. Center of Mass Intuition Question Quick Quiz A baseball bat of uniform density is cut at the location of its center of mass as shown. Which piece has the smaller mass? (d) impossible to determine Q uick Quiz 9.7 A baseball bat of uniform density is cut at the location of its center of mass as shown in Figure Which piece has the smaller mass? (a) the piece on the right (b) the piece on the left (c) both pieces have the same mass Figure 9.17 (Quick Quiz 9.7) A baseball bat cut at the location of its center of mass. (A) the piece on the right Example 9.10 (B) the piece on the left The Center of Mass of Three Particles A system consists of three particles located as shown in Figure Find the center of mass of the system. The masses of the particles are m 1 5 m kg and m kg. SOLUTIO N (C) both pieces have the same mass (D) impossible to determine y ( 3 2 m Conceptualize Figure 9.18 shows the three masses. Your intuition should tell you that the 1 Serway & Jewett, page 269. Figure 9.18 (Example 9.10) Two particles are located on the x axis, and a single particle is located on 1

22 Continuous mass distribution: Another Example Center of mass of a cylinder of uniform density, ρ. z dr r R L (Exam- ) Calculating I e z axis for a solid cylinder.

23 Continuous mass distribution: Another Example Let s choose our axes so that z points along the length of the cylinder, and the origin is right in the center of the cylinder. Probably, you can easily guess where the CM will be.

24 Continuous mass distribution: Another Example Let s choose our axes so that z points along the length of the cylinder, and the origin is right in the center of the cylinder. Probably, you can easily guess where the CM will be. At the origin!

25 Continuous mass distribution: Another Example How could we prove it?

26 Continuous mass distribution: Another Example How could we prove it? Along the z-direction this cylinder is very similar to the thin rod we just considered. Observe that dm = (πr 2 )ρ dz: z CM = 1 z(πr 2 ρ dz) M = (πr2 )ρ πr 2 Lρ L/2 L/2 z dz

27 Continuous mass distribution: Another Example How could we prove it? Along the z-direction this cylinder is very similar to the thin rod we just considered. Observe that dm = (πr 2 )ρ dz: z CM = 1 z(πr 2 ρ dz) M = (πr2 )ρ πr 2 Lρ = 0 L/2 L/2 z dz

28 Continuous mass distribution: Another Example Along the x-direction this cylinder we are looking down on a circle. Let x = r cos θ, y = r sin θ Observe that dm = (2yL)ρ dx: (Looking at just the positive x part of the cylinder, viewed top down.) 1 Or, leave the integral in terms of x and use the substitution u = x 2.

29 Continuous mass distribution: Another Example Along the x-direction this cylinder we are looking down on a circle. Let x = r cos θ, y = r sin θ Observe that dm = (2yL)ρ dx: x CM = 1 x(2yl)ρ dx M = = = 0 Lρ πr 2 L ρ πr 2 0 π r 2 (2 sin θ cos θ)( r sin θ dθ) [ 2 3 r 3 sin 3 θ ] 0 π 1 Or, leave the integral in terms of x and use the substitution u = x 2.

30 Continuous mass distribution: Another Example By symmetry the evaluation for y CM must go exactly the same way as for x CM, therefore, y CM = 0. This is what we expected all along, but this same technique can be used in cases where we cannot guess the answer.

31 Summary center of mass for continuous mass distributions 3rd Collected Homework! due Monday, Nov 20. Next Test Monday, Nov 27. (Uncollected) Homework Serway & Jewett, Ch 9, onward from page 288. Probs: 45, 47, 48, 49, 50 Look at example 9.12 and make sure you understand it. Read Chapter 9, if you haven t already.

Linear Momentum 2D Collisions Extended or Composite Systems Center of Mass

Linear Momentum 2D Collisions Extended or Composite Systems Center of Mass Linear Momentum 2D Collisions Extended or Composite Systems Center of Mass Lana Sheridan De Anza College Nov 13, 2017 Last time inelastic collisions perfectly inelastic collisions the ballistic pendulum

More information

Extended or Composite Systems Systems of Many Particles Deformation

Extended or Composite Systems Systems of Many Particles Deformation Extended or Composite Systems Systems of Many Particles Deformation Lana Sheridan De Anza College Nov 15, 2017 Overview last center of mass example systems of many particles deforming systems Continuous

More information

Linear Momentum 2D Collisions Extended or Composite Systems Center of Mass

Linear Momentum 2D Collisions Extended or Composite Systems Center of Mass Linear Momentum 2D Collisions Extended or Composite Systems Center of Mass Lana Sheridan De Anza College Nov 13, 2017 Last time inelastic collisions perfectly inelastic collisions the ballistic pendulum

More information

Rotation Moment of Inertia and Applications

Rotation Moment of Inertia and Applications Rotation Moment of Inertia and Applications Lana Sheridan De Anza College Nov 20, 2016 Last time net torque Newton s second law for rotation moments of inertia calculating moments of inertia Overview calculating

More information

Linear Momentum Inelastic Collisions

Linear Momentum Inelastic Collisions Linear Momentum Inelastic Collisions Lana Sheridan De Anza College Nov 9, 2017 Last time collisions elastic collisions Overview inelastic collisions the ballistic pendulum Linear Momentum and Collisions

More information

Rotation Angular Momentum

Rotation Angular Momentum Rotation Angular Momentum Lana Sheridan De Anza College Nov 28, 2017 Last time rolling motion Overview Definition of angular momentum relation to Newton s 2nd law angular impulse angular momentum of rigid

More information

Dynamics Energy and Work

Dynamics Energy and Work Dynamics Energy and Work Lana Sheridan De Anza College Oct 24, 2017 Last Time resistive forces: Drag Equation Drag Equation, One more point What if the object is not dropped from rest? (See Ch 6, prob

More information

Kinematics Motion in 1-Dimension

Kinematics Motion in 1-Dimension Kinematics Motion in 1-Dimension Lana Sheridan De Anza College Jan 16, 2018 Last time unit conversions (non-si units) order of magnitude calculations how to solve problems Overview 1-D kinematics quantities

More information

Rotation Torque Moment of Inertia

Rotation Torque Moment of Inertia Rotation Torque Moment of Inertia Lana Sheridan De Anza College Nov 17, 2017 Last time rotational quantities rotational kinematics torque Quick review of Vector Expressions Let a, b, and c be (non-null)

More information

Rotational Motion Rotational Kinematics

Rotational Motion Rotational Kinematics Rotational Motion Rotational Kinematics Lana Sheridan De Anza College Nov 16, 2017 Last time 3D center of mass example systems of many particles deforming systems Overview rotation relating rotational

More information

Mechanics Oscillations Simple Harmonic Motion

Mechanics Oscillations Simple Harmonic Motion Mechanics Oscillations Simple Harmonic Motion Lana Sheridan De Anza College Dec 3, 2018 Last time gravity Newton s universal law of gravitation gravitational field gravitational potential energy Overview

More information

Linear Momentum Collisions

Linear Momentum Collisions Linear Momentum Collisions Lana Sheridan De Anza College Nov 8, 2017 Last time applying the rocket equation conservation of momentum in isolated systems nonisolated systems impulse average force Overview

More information

Linear Momentum. Lana Sheridan. Nov 6, De Anza College

Linear Momentum. Lana Sheridan. Nov 6, De Anza College Linear Momentum Lana Sheridan De Anza College Nov 6, 2017 Last time energy practice Overview introducing momentum Newton s Second Law: more general form relation to force relation to Newton s third law

More information

Rotation Atwood Machine with Massive Pulley Energy of Rotation

Rotation Atwood Machine with Massive Pulley Energy of Rotation Rotation Atwood Machine with Massive Pulley Energy of Rotation Lana Sheridan De Anza College Nov 21, 2017 Last time calculating moments of inertia the parallel axis theorem Overview applications of moments

More information

Kinematics Motion in 1-Dimension

Kinematics Motion in 1-Dimension Kinematics Motion in 1-Dimension Lana Sheridan De Anza College Jan 15, 219 Last time how to solve problems 1-D kinematics Overview 1-D kinematics quantities of motion graphs of kinematic quantities vs

More information

Static Equilibrium Gravitation

Static Equilibrium Gravitation Static Equilibrium Gravitation Lana Sheridan De Anza College Dec 6, 2017 Overview One more static equilibrium example Newton s Law of Universal Gravitation gravitational potential energy little g Example

More information

Rotation Angular Momentum Conservation of Angular Momentum

Rotation Angular Momentum Conservation of Angular Momentum Rotation Angular Momentum Conservation of Angular Momentum Lana Sheridan De Anza College Nov 29, 2017 Last time Definition of angular momentum relation to Newton s 2nd law angular impulse angular momentum

More information

Mechanics Units, Dimensional Analysis, and Unit Conversion

Mechanics Units, Dimensional Analysis, and Unit Conversion Mechanics Units, Dimensional Analysis, and Unit Conversion Lana Sheridan De Anza College Sept 25, 2018 Last time introduced the course basic ideas about science and physics Overview introduce SI units

More information

Energy Energy and Friction

Energy Energy and Friction Energy Energy and Friction Lana Sheridan De Anza College Oct 31, 2017 Last time energy conservation isolated and nonisolated systems Overview Isolated system example Kinetic friction and energy Practice

More information

Linear Momentum Collisions and Energy Collisions in 2 Dimensions

Linear Momentum Collisions and Energy Collisions in 2 Dimensions Linear Momentum Collisions and Energy Collisions in 2 Dimensions Lana Sheridan De Anza College Mar 1, 2019 Last time collisions elastic collision example inelastic collisions Overview the ballistic pendulum

More information

Dynamics Applying Newton s Laws Introducing Energy

Dynamics Applying Newton s Laws Introducing Energy Dynamics Applying Newton s Laws Introducing Energy Lana Sheridan De Anza College Oct 23, 2017 Last time introduced resistive forces model 1: Stokes drag Overview finish resistive forces energy work Model

More information

Kinematics Kinematic Equations and Falling Objects

Kinematics Kinematic Equations and Falling Objects Kinematics Kinematic Equations and Falling Objects Lana Sheridan De Anza College Sept 28, 2017 Last time kinematic quantities relating graphs Overview derivation of kinematics equations using kinematics

More information

Introduction to Mechanics Time of Flight Range of a Projectile Trajectory Equation

Introduction to Mechanics Time of Flight Range of a Projectile Trajectory Equation Introduction to Mechanics Time of Flight Range of a Projectile Trajectory Equation Lana Sheridan De Anza College Feb 12, 2018 Last time projectiles launched horizontally projectiles launched at an angle

More information

Rotation Work and Power of Rotation Rolling Motion Examples and Review

Rotation Work and Power of Rotation Rolling Motion Examples and Review Rotation Work and Power of Rotation Rolling Motion Examples and Review Lana Sheridan De Anza College Nov 22, 2017 Last time applications of moments of inertia Atwood machine with massive pulley kinetic

More information

Kinematics Part I: Motion in 1 Dimension

Kinematics Part I: Motion in 1 Dimension Kinematics Part I: Motion in 1 Dimension Lana Sheridan De Anza College Sept 26, 2017 Last time introduced the course Overview basic ideas about physics units and symbols for scaling units motion in 1-dimension

More information

Thermodynamics Heat Transfer

Thermodynamics Heat Transfer Thermodynamics Heat Transfer Lana Sheridan De Anza College April 30, 2018 Last time heat transfer conduction Newton s law of cooling Overview continue heat transfer mechanisms conduction over a distance

More information

Waves Pulse Propagation The Wave Equation

Waves Pulse Propagation The Wave Equation Waves Pulse Propagation The Wave Equation Lana Sheridan De Anza College May 16, 2018 Last time oscillations simple harmonic motion (SHM) spring systems energy in SHM introducing waves kinds of waves wave

More information

Oscillations Simple Harmonic Motion

Oscillations Simple Harmonic Motion Oscillations Simple Harmonic Motion Lana Sheridan De Anza College Dec 1, 2017 Overview oscillations simple harmonic motion (SHM) spring systems energy in SHM pendula damped oscillations Oscillations and

More information

Dynamics Applying Newton s Laws The Drag Equation

Dynamics Applying Newton s Laws The Drag Equation Dynamics Applying Newton s Laws The Drag Equation Lana Sheridan De Anza College Feb 8, 2019 Last time introduced resistive forces model 1: Stokes drag Overview model 2: the Drag Equation finish resistive

More information

Kinematics Kinematic Equations and Falling Objects

Kinematics Kinematic Equations and Falling Objects Kinematics Kinematic Equations and Falling Objects Lana Sheridan De Anza College Sept 28, 2017 Last time kinematic quantities relating graphs Overview derivation of kinematics equations using kinematics

More information

Introduction to Mechanics Unit Conversions Order of Magnitude

Introduction to Mechanics Unit Conversions Order of Magnitude Introduction to Mechanics Unit Conversions Order of Magnitude Lana Sheridan De Anza College Sept 28, 2017 Last time symbols for scaling units scientific notation precision and accuracy dimensional analysis

More information

Electricity and Magnetism Current

Electricity and Magnetism Current Electricity and Magnetism Current Lana Sheridan De Anza College Feb 2, 2018 Last time dielectrics and capacitors uses of capacitors Overview current current density drift speed Motion of Charge Up until

More information

Energy Work Kinetic Energy Potential Energy

Energy Work Kinetic Energy Potential Energy Energy Work Kinetic Energy Potential Energy Lana Sheridan De Anza College Oct 25, 2017 Last time energy work Overview Work as an integral Kinetic energy Work-Kinetic energy theorem Potential energy N through

More information

2D Motion Projectile Motion

2D Motion Projectile Motion 2D Motion Projectile Motion Lana heridan De Anza College Oct 3, 2017 Last time vectors vector operations Warm Up: Quick review of Vector Expressions Let a, b, and c be (non-null) vectors. Let l, m, and

More information

Linear Momentum Isolated Systems Nonisolated Systems: Impulse

Linear Momentum Isolated Systems Nonisolated Systems: Impulse Linear Momentum Isolated Systems Nonisolated Systems: Impulse Lana Sheridan De Anza College Nov 7, 2016 Last time introduced momentum Newton s Second Law: more general form relation to force relation to

More information

Energy Energy and Friction

Energy Energy and Friction Energy Energy and Friction Lana heridan De Anza College Oct 31, 2017 Last time energy conservation isolated and nonisolated systems Overview Isolated system example Kinetic friction and energy Practice

More information

Waves Wave Speed on a String Pulse Propagation The Wave Equation

Waves Wave Speed on a String Pulse Propagation The Wave Equation Waves Wave Speed on a String Pulse Propagation The Wave Equation Lana Sheridan De Anza College May 16, 2018 Last time oscillations simple harmonic motion (SHM) spring systems energy in SHM introducing

More information

Waves Standing Waves and Sound Beats Nonsinusoidal Wave Patterns

Waves Standing Waves and Sound Beats Nonsinusoidal Wave Patterns Waves Standing Waves and Sound Beats Nonsinusoidal Wave Patterns Lana Sheridan De Anza College May 24, 2018 Last time interference and sound standing waves and sound musical instruments Reminder: Speed

More information

Introduction to Mechanics Dynamics Forces Newton s Laws

Introduction to Mechanics Dynamics Forces Newton s Laws Introduction to Mechanics Dynamics Forces Newton s Laws Lana heridan De Anza College Feb 20, 2018 Last time Newton s second law mass and weight examples free-body diagrams Overview Newton s second law

More information

Electricity and Magnetism DC Circuits Using Kirchhoff s Laws

Electricity and Magnetism DC Circuits Using Kirchhoff s Laws Electricity and Magnetism DC Circuits Using Kirchhoff s Laws Lana Sheridan De Anza College Feb 9, 08 Last time power Kirchhoff s laws Overview more Kirchhoff examples Example with Two Batteries Find the

More information

Waves Solutions to the Wave Equation Sine Waves Transverse Speed and Acceleration

Waves Solutions to the Wave Equation Sine Waves Transverse Speed and Acceleration Waves Solutions to the Wave Equation Sine Waves Transverse Speed and Acceleration Lana Sheridan De Anza College May 17, 2018 Last time pulse propagation the wave equation Overview solutions to the wave

More information

Electricity and Magnetism Electric Field

Electricity and Magnetism Electric Field Electricity and Magnetism Electric Field Lana Sheridan De Anza College Jan 11, 2018 Last time Coulomb s Law force from many charges R/2 +8Q Warm Up Question (c) articles. p Fig. 21-19 Question 9. 10 In

More information

Introduction to Mechanics Units and Measurements

Introduction to Mechanics Units and Measurements Introduction to Mechanics Units and Measurements Lana Sheridan De Anza College Jan 9, 2018 Last time introduced the course basic ideas about science and physics Overview models, hypotheses, theories, and

More information

Kinematics Varying Accelerations (1D) Vectors (2D)

Kinematics Varying Accelerations (1D) Vectors (2D) Kinematics Varying Accelerations (1D) Vectors (2D) Lana heridan De Anza College ept 29, 2017 Last time kinematic equations using kinematic equations Overview falling objects and g varying acceleration

More information

Lecture 10 - Moment of Inertia

Lecture 10 - Moment of Inertia Lecture 10 - oment of Inertia A Puzzle... Question For any object, there are typically many ways to calculate the moment of inertia I = r 2 dm, usually by doing the integration by considering different

More information

Electricity and Magnetism Overview of Course Charge and Conduction

Electricity and Magnetism Overview of Course Charge and Conduction Electricity and Magnetism Overview of Course Charge and Conduction Lana Sheridan De Anza College Jan 8, 2018 Overview of the Course Topics charge static electric interactions electric fields electric potential

More information

Introduction to Mechanics Non-uniform Circular Motion Introducing Energy

Introduction to Mechanics Non-uniform Circular Motion Introducing Energy Introduction to Mechanics Non-uniform Circular Motion Introducing Energy Lana Sheridan De Anza College Nov 20, 2017 Last time applying the idea of centripetal force banked turns Overview non-uniform circular

More information

Waves Standing Waves Sound Waves

Waves Standing Waves Sound Waves Waves Standing Waves Sound Waves Lana Sheridan De Anza College May 23, 2018 Last time finish up reflection and transmission standing waves Warm Up Question: Standing Waves and Resonance In the following

More information

Electricity and Magnetism Coulomb s Law

Electricity and Magnetism Coulomb s Law Electricity and Magnetism Coulomb s Law Lana Sheridan De Anza College Jan 10, 2018 Last time introduced charge conductors insulators induced charge Overview Force from a point charge Quantization of charge

More information

Energy Energy Diagrams and Equilibrium Conservation Laws Isolated and Nonisolated Systems

Energy Energy Diagrams and Equilibrium Conservation Laws Isolated and Nonisolated Systems Energy Energy Diagrams and Equilibrium Conservation Laws Isolated and Nonisolated Systems Lana Sheridan De Anza College Oct 30, 2017 Last time gravitational and spring potential energies conservative and

More information

Introduction to Mechanics Projectiles Time of Flight

Introduction to Mechanics Projectiles Time of Flight Introduction to Mechanics Projectiles Time of Flight Lana Sheridan De Anza College Oct 24, 2017 Last time height of a projectile Warm Up Question # 57, page 107 Child 1 throws a snowball horizontally from

More information

Energy Energy Diagrams and Equilibrium Conservation Laws Isolated and Nonisolated Systems

Energy Energy Diagrams and Equilibrium Conservation Laws Isolated and Nonisolated Systems Energy Energy Diagrams and Equilibrium Conservation Laws Isolated and Nonisolated Systems Lana Sheridan De Anza College Oct 30, 2017 Last time gravitational and spring potential energies conservative and

More information

Static Equilibrium. Lana Sheridan. Dec 5, De Anza College

Static Equilibrium. Lana Sheridan. Dec 5, De Anza College tatic Equilibrium Lana heridan De Anza College Dec 5, 2016 Last time simple harmonic motion Overview Introducing static equilibrium center of gravity tatic Equilibrium: ystem in Equilibrium Knowing that

More information

Electricity and Magnetism Coulomb s Law

Electricity and Magnetism Coulomb s Law Electricity and Magnetism Coulomb s Law Lana Sheridan De Anza College Jan 10, 2018 Last time introduced charge conductors insulators induced charge Warm Up. Do both balloons A and B have a charge? ntry

More information

Optics Polarization. Lana Sheridan. June 20, De Anza College

Optics Polarization. Lana Sheridan. June 20, De Anza College Optics Polarization Lana Sheridan De Anza College June 20, 2018 Last time interference from thin films Newton s rings Overview the interferometer and gravitational waves polarization birefringence 7 Michelson

More information

Dynamics: Laws of Motion Newton s 1st & 2nd Laws Forces Fundametally

Dynamics: Laws of Motion Newton s 1st & 2nd Laws Forces Fundametally Dynamics: Laws of Motion Newton s 1st & 2nd Laws Forces Fundametally Lana heridan De Anza College Oct 9, 2017 Last Time nonuniform circular motion Introduced forces Overview Newton s Laws! (1st & 2nd)

More information

Electricity and Magnetism B-Fields from Moving Charges

Electricity and Magnetism B-Fields from Moving Charges Electricity and Magnetism B-Fields from Moving Charges Lana Sheridan De Anza College Feb 28, 2018 Last time force on a curved current carrying wire torque on a wire loop magnetic dipole moment Overview

More information

Energy Power. Lana Sheridan. Nov 1, De Anza College

Energy Power. Lana Sheridan. Nov 1, De Anza College Energy Power Lana heridan De Anza College Nov 1, 2017 Overview Power Practice problems! Power Power the rate of energy transfer to a system. Power Power the rate of energy transfer to a system. The instantaneous

More information

Mechanics Gravity. Lana Sheridan. Nov 29, De Anza College

Mechanics Gravity. Lana Sheridan. Nov 29, De Anza College Mechanics Gravity Lana Sheridan De Anza College Nov 29, 2018 Last time angular momentum of rigid objects conservation of angular momentum examples Overview Newton s law of gravitation gravitational field

More information

2D Motion Projectile Motion

2D Motion Projectile Motion 2D Motion Projectile Motion Lana heridan De Anza College Oct 3, 2017 Last time vectors vector operations 2 dimensional motion Warm Up: Quick review of Vector Expressions Let a, b, and c be (non-null) vectors.

More information

Linear Momentum. Lecture 15. Chapter 9. Physics I Department of Physics and Applied Physics

Linear Momentum. Lecture 15. Chapter 9. Physics I Department of Physics and Applied Physics Lecture 15 Chapter 9 Physics I 10.30.2013 Linear Momentum Course website: http://faculty.uml.edu/ndriy_danylov/teaching/physicsi Lecture Capture: http://echo360.uml.edu/danylov2013/physics1fall.html Outline

More information

Electricity and Magnetism Charge and Conduction Coulomb s Law

Electricity and Magnetism Charge and Conduction Coulomb s Law Electricity and Magnetism Charge and Conduction Coulomb s Law Lana Sheridan De Anza College Jan 9, 2018 Last time course structure introduced charge Overview conductors insulators induced charge quantization

More information

14. Rotational Kinematics and Moment of Inertia

14. Rotational Kinematics and Moment of Inertia 14. Rotational Kinematics and Moment of nertia A) Overview n this unit we will introduce rotational motion. n particular, we will introduce the angular kinematic variables that are used to describe the

More information

Free fall. Lana Sheridan. Oct 3, De Anza College

Free fall. Lana Sheridan. Oct 3, De Anza College Free fall Lana Sheridan De Anza College Oct 3, 2018 2018 Physics Nobel Prize Congratulations to Arthur Ashkin and to Gérard Mourou and Donna Strickland Last time the kinematics equations (constant acceleration)

More information

Introduction to Mechanics Conservative and Nonconservative Forces Potential Energy

Introduction to Mechanics Conservative and Nonconservative Forces Potential Energy Introduction to Mechanics Conservative and Nonconservative Forces Potential Energy Lana Sheridan De Anza College Mar 20, 2018 Last time work of varying force kinetic energy work-kinetic energy theorem

More information

Thermodynamics Second Law Entropy

Thermodynamics Second Law Entropy Thermodynamics Second Law Entropy Lana Sheridan De Anza College May 9, 2018 Last time entropy (macroscopic perspective) Overview entropy (microscopic perspective) Reminder of Example from Last Lecture

More information

2D Kinematics Relative Motion Circular Motion

2D Kinematics Relative Motion Circular Motion 2D Kinematics Relative Motion Circular Motion Lana heridan De Anza College Oct 5, 2017 Last Time range of a projectile trajectory equation projectile example began relative motion Overview relative motion

More information

Electricity and Magnetism Overview of Course Charge and Conduction

Electricity and Magnetism Overview of Course Charge and Conduction Electricity and Magnetism Overview of Course Charge and Conduction Lana Sheridan De Anza College Sept 22, 2015 Overview of the Course Topics charge static electric interactions electric fields electric

More information

PHYS 1441 Section 002 Lecture #17

PHYS 1441 Section 002 Lecture #17 PHYS 1441 Section 002 Lecture #17 Dr. Jaehoon Linear Momentum Linear Momentum and Impulse Linear Momentum and Forces Linear Momentum Conservation Collisions Center of Mass Today s homework is homework

More information

Energy Potential Energy and Force Conservation Laws Isolated and Nonisolated Systems

Energy Potential Energy and Force Conservation Laws Isolated and Nonisolated Systems Energy Potential Energy and Force Conservation Laws Isolated and Nonisolated ystems Lana heridan De Anza College Oct 27, 2017 Last time gravitational and spring potential energies conservative and nonconservative

More information

Fluids, Thermodynamics, Waves, and Optics Fluids

Fluids, Thermodynamics, Waves, and Optics Fluids Fluids, Thermodynamics, Waves, and Optics Fluids Lana Sheridan De Anza College April 10, 2018 Overview static fluids pressure liquid pressure Pascal s law Elastic Properties of Solids We are considering

More information

2D Kinematics: Nonuniform Circular Motion Dynamics: Laws of Motion Newton s 1st & 2nd Laws

2D Kinematics: Nonuniform Circular Motion Dynamics: Laws of Motion Newton s 1st & 2nd Laws 2D Kinematics: Nonuniform Circular Motion Dynamics: Laws of Motion Newton s 1st & 2nd Laws Lana heridan De Anza College Oct 6, 2017 Last Time relative motion uniform circular motion Overview nonuniform

More information

Conceptual Physics Energy Sources Collisions

Conceptual Physics Energy Sources Collisions Conceptual Physics Energy ources Collisions Lana heridan De Anza College July 7, 2015 Last time energy and work kinetic energy potential energy conservation of energy energy transfer simple machines efficiency

More information

Rotational Kinetic Energy

Rotational Kinetic Energy Lecture 17, Chapter 10: Rotational Energy and Angular Momentum 1 Rotational Kinetic Energy Consider a rigid body rotating with an angular velocity ω about an axis. Clearly every point in the rigid body

More information

Kinematics: Circular Motion Mechanics: Forces

Kinematics: Circular Motion Mechanics: Forces Kinematics: Circular Motion Mechanics: Forces Lana heridan De Anza College Oct 11, 2018 Last time projectile trajectory equation projectile examples projectile motion and relative motion Overview circular

More information

Introduction to Mechanics Energy Conservation

Introduction to Mechanics Energy Conservation Introduction to Mechanics Energy Conservation Lana Sheridan De Anza College Mar 22, 2018 Last time conservative forces and potential energy energy diagrams mechanical energy energy conservation Overview

More information

Mechanics Newton s Laws

Mechanics Newton s Laws Mechanics Newton s Laws Lana heridan De Anza College Oct 15, 2018 Last time circular motion force net force Overview net force example Newton s first law Newton s second law mass vs weight force diagrams

More information

Electricity and Magnetism Energy of the Magnetic Field Mutual Inductance

Electricity and Magnetism Energy of the Magnetic Field Mutual Inductance Electricity and Magnetism Energy of the Magnetic Field Mutual Inductance Lana Sheridan De Anza College Mar 14, 2018 Last time inductors resistor-inductor circuits Overview wrap up resistor-inductor circuits

More information

Doppler E ect Bow and Shock Waves

Doppler E ect Bow and Shock Waves Doppler E ect Bow and Shock Waves Lana Sheridan De Anza College May 30, 2018 Last time nonsinusoidal waves intensity of a wave sound level Overview sound level & perception of sound with frequency the

More information

Dynamics Applying Newton s Laws Air Resistance

Dynamics Applying Newton s Laws Air Resistance Dynamics Applying Newton s Laws Air Resistance Lana Sheridan De Anza College Oct 20, 2017 Last Time accelerated frames and rotation Overview resistive forces two models for resistive forces terminal velocities

More information

Quick Questions. 1. Two charges of +1 µc each are separated by 1 cm. What is the force between them?

Quick Questions. 1. Two charges of +1 µc each are separated by 1 cm. What is the force between them? 92 3.10 Quick Questions 3.10 Quick Questions 1. Two charges of +1 µc each are separated by 1 cm. What is the force between them? 0.89 N 90 N 173 N 15 N 2. The electric field inside an isolated conductor

More information

Electricity and Magnetism Implications of Gauss s Law Electric Potential Energy

Electricity and Magnetism Implications of Gauss s Law Electric Potential Energy Electricity and Magnetism Implications of Gauss s Law Electric Potential Energy Lana Sheridan De Anza College Jan 22, 2018 Last time using Gauss s law Overview implications of Gauss law electric potential

More information

Physics 8 Friday, November 4, 2011

Physics 8 Friday, November 4, 2011 Physics 8 Friday, November 4, 2011 Please turn in Homework 7. I will hand out solutions once everyone is here. The handout also includes HW8 and a page or two of updates to the equation sheet needed to

More information

Thermodynamics Molecular Model of a Gas Molar Heat Capacities

Thermodynamics Molecular Model of a Gas Molar Heat Capacities Thermodynamics Molecular Model of a Gas Molar Heat Capacities Lana Sheridan De Anza College May 3, 2018 Last time modeling an ideal gas at the microscopic level rms speed of molecules equipartition of

More information

Introduction to Mechanics Dynamics Forces Newton s Laws

Introduction to Mechanics Dynamics Forces Newton s Laws Introduction to Mechanics Dynamics Forces Newton s Laws Lana heridan De Anza College Nov 1, 2017 Last time Newton s second law mass and weight examples free-body diagrams Overview Newton s second law examples

More information

Energy Practice. Lana Sheridan. Nov 2, De Anza College

Energy Practice. Lana Sheridan. Nov 2, De Anza College Energy Practice Lana heridan De Anza College Nov 2, 2017 Overview Practice problems! a nonconservative force acts. Example: Block pulled across surface g along a freeway at 65 mi/h. Your car has kinetic

More information

Course Instructor. Home Page. Title Page. Page 2 of 33. Go Back. Full Screen. Close. Quit

Course Instructor. Home Page. Title Page. Page 2 of 33. Go Back. Full Screen. Close. Quit Rutgers University Department of Physics & Astronomy 01:750:271 Honors Physics I Lecture 1 Page 1 of 33 Course Instructor Duiliu Emanuel Diaconescu Office: Serrin E358 Phone: 848 445 9054 E-mail: duiliu@physics.rutgers.edu

More information

Systematic Uncertainty Max Bean John Jay College of Criminal Justice, Physics Program

Systematic Uncertainty Max Bean John Jay College of Criminal Justice, Physics Program Systematic Uncertainty Max Bean John Jay College of Criminal Justice, Physics Program When we perform an experiment, there are several reasons why the data we collect will tend to differ from the actual

More information

2D Kinematics: Nonuniform Circular Motion Dynamics: Forces

2D Kinematics: Nonuniform Circular Motion Dynamics: Forces 2D Kinematics: Nonuniform Circular Motion Dynamics: Forces Lana heridan De Anza College Oct 6, 2017 Last Time relative motion uniform circular motion Overview nonuniform circular motion Introduce forces

More information

Concepts in Physics. Friday, October 16th

Concepts in Physics. Friday, October 16th 1206 - Concepts in Physics Friday, October 16th Notes Assignment #4 due Wednesday, October 21 st in class (no later than noon) There are still assignments #1 and #2 in my office to be picked up... If you

More information

Thermodynamics Heat & Internal Energy Heat Capacity

Thermodynamics Heat & Internal Energy Heat Capacity Thermodynamics Heat & Internal Energy Heat Capacity Lana Sheridan De Anza College April 23, 2018 Last time the ideal gas equation moles and molecules Overview finish applying the ideal gas equation thermal

More information

Introduction to Mechanics Potential Energy Energy Conservation

Introduction to Mechanics Potential Energy Energy Conservation Introduction to Mechanics Potential Energy Energy Conservation Lana Sheridan De Anza College Nov 28, 2017 Last time power conservative and nonconservative forces friction Overview conservative forces and

More information

Math 41 Final Exam December 9, 2013

Math 41 Final Exam December 9, 2013 Math 41 Final Exam December 9, 2013 Name: SUID#: Circle your section: Valentin Buciumas Jafar Jafarov Jesse Madnick Alexandra Musat Amy Pang 02 (1:15-2:05pm) 08 (10-10:50am) 03 (11-11:50am) 06 (9-9:50am)

More information

Introduction to Mechanics Motion in 2 Dimensions

Introduction to Mechanics Motion in 2 Dimensions Introduction to Mechanics Motion in 2 Dimensions Lana heridan De Anza College Oct 17, 2017 Last time vectors and trig Overview wrap up vectors introduction to motion in 2 dimensions constant velocity in

More information

APPLICATIONS. CEE 271: Applied Mechanics II, Dynamics Lecture 17: Ch.15, Sec.4 7. IMPACT (Section 15.4) APPLICATIONS (continued) IMPACT READING QUIZ

APPLICATIONS. CEE 271: Applied Mechanics II, Dynamics Lecture 17: Ch.15, Sec.4 7. IMPACT (Section 15.4) APPLICATIONS (continued) IMPACT READING QUIZ APPLICATIONS CEE 271: Applied Mechanics II, Dynamics Lecture 17: Ch.15, Sec.4 7 Prof. Albert S. Kim Civil and Environmental Engineering, University of Hawaii at Manoa Date: The quality of a tennis ball

More information

Note: Each problem is worth 14 points except numbers 5 and 6 which are 15 points. = 3 2

Note: Each problem is worth 14 points except numbers 5 and 6 which are 15 points. = 3 2 Math Prelim II Solutions Spring Note: Each problem is worth points except numbers 5 and 6 which are 5 points. x. Compute x da where is the region in the second quadrant between the + y circles x + y and

More information

Physics 1401V October 28, 2016 Prof. James Kakalios Quiz No. 2

Physics 1401V October 28, 2016 Prof. James Kakalios Quiz No. 2 This is a closed book, closed notes, quiz. Only simple (non-programmable, nongraphing) calculators are permitted. Define all symbols and justify all mathematical expressions used. Make sure to state all

More information

Energy Potential Energy Conservative and Nonconservative Forces

Energy Potential Energy Conservative and Nonconservative Forces Energy Potential Energy Conservative and Nonconservative Forces Lana Sheridan De Anza College Oct 26, 2017 Last time Work as an integral Kinetic Work-Kinetic theorem Potential Overview Gravitational and

More information

PHY131H1F - Class 18. Torque of a quick push

PHY131H1F - Class 18. Torque of a quick push Today: Today, Chapter 11: PHY131H1F - Class 18 Angular velocity and Angular acceleration vectors Torque and the Vector Cross Product Angular Momentum Conservation of Angular Momentum Gyroscopes and Precession

More information

Mechanics More about Impulse Conservation of Momentum

Mechanics More about Impulse Conservation of Momentum Mechanics More about Impulse Conservation of Momentum Lana Sheridan De Anza College Nov 6, 2018 Last time center of mass linear momentum momentum and Newton s second law impulse Overview more about impulse

More information