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Rutgers - PHYSICS - 104
Gravitation"On the Shoulders of Giants" Newtononce said that his success was based on the fact that he "stood on the shoulders of giants" In other words, his work was based on the great work done by his predecessors. Tycho Brahe 1546-1601 the original
Rutgers - PHYSICS - 104
Electric Forces and Electric FieldsElectric Forces and Electric Fields1 Properties of Electric Charges Electric charge is an intrinsic property of matter, inherent in its atomic structure. electron charge: q = -e proton charge: q = +e with elementary c
Rutgers - PHYSICS - 104
Electrical Potential Energy and Electric Potential1 Potential Energy and Electric PotentialThe Coulomb force law is of the same form as the universal law of gravity the electrostatic force is a conservative force. Example: A small positive test charge,
Rutgers - PHYSICS - 104
Electric Circuits1 Electric Current and Electromotive ForceThe flow of electric charges: Electric currents power light bulbs, TV sets, computers etc. Definition of electric current: The current is the rate at which charge flows through a surface perpend
Rutgers - PHYSICS - 104
Chapter 211Hydrodynamics and Electromagnetism Muchof the terminology is the same Some concepts can be applied between the two fields2Amber3Charging By Induction4Two Things You Already Knew1. Oppositechargesattract 2. "Like" charges repel5Re
Rutgers - PHYSICS - 104
Magnetic Forces and Magnetic Fields1 MagnetsMagnets are metallic objects, mostly made out of iron, which attract other iron containing objects (nails) etc. Magnets orient themselves in roughly a north - south direction if they are allowed to rotate free
Rutgers - PHYSICS - 104
Electromagnetic Induction1 Induced emf and Magnetic FluxWe have seen that electric currents produce magnetic fields. Can magnetic fields produce electric currents? Faraday's experiment: (see micro.magnet.fsu.edu/electromag/java/faraday) When the switch
Rutgers - PHYSICS - 104
Electromagnetic Waves1 Maxwell's PredictionsDuring the early stages of studies of electric and magnetic phenomena, they were thought to be unrelated. In 1865, James Clark Maxwell provided a mathematical theory that showed a close relation between electr
Rutgers - PHYSICS - 104
The Reflection of Light: Mirrors1 Plane MirrorsThe laws of reflection and refraction can be developed using a geometric method proposed by Huygens in 1678. His wave model is adequate for understanding many practical aspects of the propagation of light.
Rutgers - PHYSICS - 104
The Refraction of Light1 The Refraction of Light When a ray of light traveling through a transparent medium encounters a boundary leading into another transparent medium, part of the light is reflected and part enters the second medium. The ray that ent
Rutgers - PHYSICS - 104
The Refraction of Light1 Polarization and the Reflection and Refraction of Light The most common technique to produce polarized light is to use a material that only allows for the transmission of a certain component of the electric field. Polarization c
Rutgers - PHYSICS - 104
The Principle of Linear Superposition1 Conditions for InterferenceWhen two or more light waves meet at a given point, their electric fields combine (interfere) according to the laws of linear superposition: The waves can add together either constructive
Rutgers - PHYSICS - 104
The Nature of the Atom1 Early Models of the Atom Thompson's model: The atom is a volume of positive charge, with electrons embedded throughout the volume. In 1911, Geiger and Marsden (under supervision of Rutherford) directed a beam of alpha particles (
Rutgers - PHYSICS - 104
Radioactivity1 The Structure of the Nucleus The nucleus consists of protons (positively charged particles) and neutrons (electrically neutral). The neutron is slightly heavier than the proton. The total number of protons and neutrons inside a nucleus is
Rutgers - PHYSICS - 104
Inductance and Alternating Current Circuits1 Self-inductance Consider a circuit consisting of a switch, a resistor, and an emf.I S BR When the switch is closed, the current does not change immediately from zero to its maximum value /R but only increa
Rutgers - PHYSICS - 104
Special Relativity and Quantum Physics1 The Principle of Relativity Although Newtonian mechanics works very well at low speeds, it fails when applied to particles whose speeds approach that of light. Experimentally, the predictions of Newtonian mechanic
Rutgers - PHYSICS - 104
Physics Intro &KinematicsQuantitiesVelocityUnitsAccelerationVectorsKinematicsDisplacementGraphing Motion in 1-DSome Physics QuantitiesVector - quantity with both magnitude (size) and directionScalar - quantity with magnitude onlyVectors: Dis
Rutgers - PHYSICS - 104
Forces Newtons Lawsof Motion Weight Free fall Force and motionproblems in 1-D Normal force Tension Free body diagrams Atwood device Static and kinetic friction Coefficients of friction Air resistance Terminal velocityExamples of Forces A f
Rutgers - PHYSICS - 104
Vectors Vector Operations Components Inclined Planes Equilibrium 2-D Force &Motion Problems Trig Applications Relative Velocities Free Body DiagramsVector AdditionSuppose 3 forces act on an objectat the same time. Fnet is not 15 Nbecause thes
Rutgers - PHYSICS - 104
MotioninTwoDimensions:ProjectileMotionCircularMotionAngularSpeedSimpleHarmonicMotionTorqueCenterofMassProjectile MotionA red marble is dropped off a cliff at thesame time a black one is shothorizontally. At any point in time themarbles are at
Rutgers - PHYSICS - 104
GravityNewtonsLawofGravitationKeplersLawsofPlanetaryMotionGravitationalFieldsNewtons Law of Gravitationrm2m1There is a force of gravity between any pair of objectsanywhere. The force is proportional to each mass andinversely proportional to the
Rutgers - PHYSICS - 104
MOMENTUM!MomentumImpulseConservationofMomentumin1DimensionConservationofMomentumin2DimensionsAngularMomentumTorqueMomentofInertiaMomentum Definedp = mvp = momentum vectorm = massv = velocity vectorMomentum Facts p = mv Momentum is a vect
Rutgers - PHYSICS - 104
EnergyWorkForms of EnergyConservation of EnergyGravitational & Elastic Potential EnergyWork - Energy TheoremConservation of Momentum & EnergyPowerSimple MachinesMechanical AdvantageWorkThe simplest definition for the amount of work a force does
Rutgers - PHYSICS - 104
Chapter 1: ReviewIn Physics 6A, we use the MKS/SI System:Length: the meterTime: the secondMass: the kilogramTemperature: the kelvinPlane angle: the radian, but we can still use degrees formost problems. We generally use radians when formulasare de
Rutgers - PHYSICS - 104
Chapter 2 Review: Motion in a Straight LineDisplacement is change in position. For motion along the x direction, displacement is designated x: x = x2x1 where x1 and x2 are the initial and final positions, respectively. Velocity is the rate of change of p
Rutgers - PHYSICS - 104
Chapter 3 Review: Motion in 2DA vector is a quantity that has both magnitude and direction. In two dimensions it takes two numbers to specify a vector. A vector can be represented by an arrow whose length correspondsto the vectors magnitude.Position
Rutgers - PHYSICS - 104
Chapter 4 Review: Newtons Laws of Motion Newtons first law of motion: A body in uniform motionremains in uniform motion, and a body at rest remains atrest, unless acted on by a nonzero net force. Newtons second law of motion: The rate at which abodys
Rutgers - PHYSICS - 104
Chapter 5 Review: Using Newton's Laws Physical diagram: Free-body diagram: Newtons law: Fnet = ma In components: x-component: mg sinO = ma y-component: n mg cosO = 0 2012 Pearson Education, Inc.Slide 5-1Two Body Problems Solve problems involving
Rutgers - PHYSICS - 104
dU/dT = 0d2U/dt2 > 0d2U/dt2 < 0
Rutgers - PHYSICS - 104
CircuitsCurrentResistance&OhmsLawResistorsinSeries,inParallel,andincombinationCapacitorsinSeriesandParallelVoltmeters&AmmetersResistivityPower&PowerLinesFuses&BreakersBulbsinSeries&ParallelElectricityThe term electricity can be used to refer to
Rutgers - PHYSICS - 104
Electric Fields Review of gravitational fields Electric field vector Electric fields for various charge configurations Field strengths for point charges and uniform fields Work done by fields & change in potential energy Potential & equipotential su
Rutgers - PHYSICS - 104
Electrostatics Electric charge Van de Graff generators Conservation of charge Equilibrium problems Insulators & conductors Grounding Charging objects Static electricity Electroscopes Coulombs law Lightning Systems of chargesElectric Charge J
Rutgers - PHYSICS - 104
1. What is the wavelength of 345 Hz sound in air if the speed of sound is 345 m/s?A. B. C. D. E. 0.1 meters 0.345 meters 1.0 meter 3.45 meters sound is not characterized by wavelengthC2. Why is it difficult to localize sound under water?A. B. C. D. so
Rutgers - PHYSICS - 104
FluidsStatesofMatterPhaseChangesDensityPressurePascalsPrincipleBuoyantForceArchimedesPrincipleBernoullisPrincipleTorricellisprincipleViscosityTurbulenceCohesionAdhesionSurfaceTensionStatesofMatterMatter comes in a variety of states: solid,
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The Art of Estimation Physics Thealsoknownas Ph 2239I.Nat ur al Uni t sPatrick Diamond, George M. Fuller, Tom Murphy Department of Physics, University of California, San DiegoRichard Feynman : use sloppy thinking never attempt a physics problem until
Rutgers - PHYSICS - 104
The Art of Estimation Physics Thealsoknownas Ph 2239II.Forces,etc.Patrick Diamond, George M. Fuller, Tom Murphy Department of Physics, University of California, San DiegoHandy Facts: Solar Systemradius of earths orbit around sunHandy Facts: the Univ
Rutgers - PHYSICS - 104
The Art of Estimation Physics Thealsoknownas Ph 239I.Statistical Mechanics for DummiesPatrick Diamond, George M. Fuller, Tom Murphy Department of Physics, University of California, San DiegoHandy Facts: Solar Systemradius of earths orbit around sun
Rutgers - PHYSICS - 104
The Art of Estimation Physics Thealsoknownas Ph 2239I.Statistical Mechanics for DummiesPatrick Diamond, George M. Fuller, Tom Murphy Department of Physics, University of California, San DiegoHandy Facts: Solar Systemradius of earths orbit around sun
Rutgers - PHYSICS - 104
Nucleons & Nucleia quick guide to the real essentials in the subject which particle and nuclear physicists won't tell youThe Paradox~ 1 fmNucleon (www.jlab.org) 3 basic quarks plus a sea of gluons and quarkantiquark pairsDo electron scattering on nuc
Rutgers - PHYSICS - 104
Introduction to Physics 260Dr. Phil Womble womble@wku.edu Applied Physics Institute 270 781 3859 Office Hours: MWF 8-5, TR 1-5 API1Are you in the right place? Thisis University Physics II Pre-requisites:Physics 250 and Math 126 Co-requisites: Math
Rutgers - PHYSICS - 104
Chapter 4 Kinematics in 2 & 3 DimensionsKinematics in 2 & 3 Dim Projectile Motion Circular MotionPosition and Displacement in 3-DAverage Velocity Displacementper unit time r x ^ y ^ z ^ vavg = = i+ j+ k t t t t velocity Instantaneous dr dx ^ dy ^ d
Rutgers - PHYSICS - 104
Chapter 3 Vectors Physics deals with many quantities that have bothSize Direction VECTORS !y r(x,y) (r,)xE.g. Displacement, Velocity, Acceleration, Force, Torquex and y components of motion are independent-"LINEARITY"Componets v x = v cos v y = v
Rutgers - PHYSICS - 104
Physics 211 "Physics" with Calculus Concurrent minimal requirement: Math 140 "First Semester Calculus" Text: Halliday Resnick Walker, Fundamentals of Physics, Extended, 9th EditionPhysics 211Introduction to Mechanics Course Overview Requirements Exp
Rutgers - PHYSICS - 104
Motion in 1-D KINEMATICSThe Major Player Isaac Newton 1642-1727 Develops Calculus to explain the theory of Mechanics F = maKinematics Dynamics We begin here in 1-D Note that vx0 is the same throughout the motion of the objectvx 0 = v0 cos v y 0 = v0
Rutgers - PHYSICS - 104
Lecture 5: Introduction to Physics PHY101Chapter 2: Equations of Kinematics for Constant Acceleration in 1 Dim. (2.4, 2.5, 2.7) Free Fall (2.6) Chapter 3: Equations of Kinematics for Constant Acceleration in 2 Dim. (3.1, 3.2)Physics 101: Lecture 6, Pg 1
Rutgers - PHYSICS - 104
Physics 101: Lecture 8Newton's LawsqToday's lecture will be a review of Newton's Laws and the four types of forces discussed in Chapter 4. Concepts of Mass and Force Newton's Three Laws Gravitational, Normal, Frictional, Tension ForcesPhysics 101: Lec
Rutgers - PHYSICS - 104
Physics 101: Application of Newton's LawsReview of the different types of forces discussed in Chapter 4: Gravitational, Normal, Frictional, Tension Forces Practice Examples qPhysics 101: Lecture 9, Pg 1Solving ProblemsIdentify forces acting on an obj
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Physics 101: Lecture 10 Application of Newton's LawsqNew Material: Textbook Chapter 5 Circular Motion & Centripetal AccelerationPhysics 101: Lecture 10, Pg 1You are twirling a ball on string. What happens if the string breaks ?b a cvAnswer: bPhys
Rutgers - PHYSICS - 104
Physics 101: Lecture 11 Centripetal Forceq qBrie Re w of Chapte 1-4 f vie rs Te xtbook Chapte 5 r Uniformcircular m otion :sate s in circular orbits, appare we llite nt ightle ss and ssne artificial gravityPhysics 101: Lecture 11, Pg 1Centripetal For
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Faraday's Law and Lenz's LawB(t) i~Physics 1304: Lecture 13, Pg 1Overview of Lectureq qInduction Effects Faraday's Law (Lenz' Law) Energy Conservation with induced currents?qFaraday's Law in terms of Electric FieldsText Reference: Chapter 31.1-4
Rutgers - PHYSICS - 104
Physics 101: Lecture 14 Impulse and MomentumqToday's le cturewill cove C r hapte 7.1 - 7.2 rPhysics 101: Lecture 14, Pg 1Impulse and MomentumqC onside a ball hit by a base bat: r ball At t=t 0: ball approache bat with initial ve s locity v0 At t=t f
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Physics 101: Lecture 15 Impulse and MomentumqToday's lecture will be a review of Chapters 7.1 - 7.2 and q New material: Collisions and Center of Mass, Chapters 7.3-7.5 Rotational Motion and Angular Displacement, Chapter 8.1Physics 101: Lecture 15, Pg 1
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Physics 101: Lecture 16 Rotational KinematicsqToday's le cturewill cove Te r xtbook C hapte 8 rPhysics 101: Lecture 16, Pg 1Rotational KinematicsqThe motion of a rigid body about a fixed axis is described by using the same concepts as for linear mot
Rutgers - PHYSICS - 104
Physics 101: Lecture 17 Rotational DynamicsqRe w of thelast le vie ctureon Rotational Kine atics and m Rolling Motion and theVe Natureof Angular Variable ctor s q Today's le cturewill cove Te r xtbook S ctions 9.1 - 9.3 ePhysics 101: Lecture 17, Pg 1B