SMU PHYS 1304 - Electric Charge and Coulomb’s Law

Unformatted text preview:

Electric Charge and Coulomb’s LawSlide 2Slide 3Slide 4Slide 5Slide 6Slide 7Slide 8Slide 9Slide 10Slide 11Slide 12Slide 13Slide 14Superposition Principle, ExampleZero Resultant Force, ExampleElectrical Force with Other Forces, ExampleElectrical Force with Other Forces, Example cont.1Electric Charge and Coulomb’s LawElectric chargeThe positive charge and negative charge:Matter is made of atoms. Inside an atom, there is the nucleus that is surrounded by electrons.Inside the nucleus, there are two particles called proton and neutron. The smallest nucleus contains only one proton. This is the nucleus inside a hydrogen atom. Proton and electron attract each other. Proton and proton, electron and electron repel each other. This is a property of these matters (proton and electron) and we call it charge. Electric charge is a property of matter that can cause attraction and repulsion. We call the charge carried by electrons “negative (-e) ” and the charge carried by protons “positive (+e)”. Charge is a value, or a scalar, not a vector. It is fully described by a number.2Electric Charge and Coulomb’s LawThe unit of electric chargeThe SI1 unit for charge is the coulomb. An electron or a proton has a charge of magnitude e = 1.602 18×10−19 C (coulombs). Some scientists, chemists in particular, use another unit, the esu or electrostatic unit. One esu equals 3.335 64×10−10 C. To provide you with an idea of the magnitude of a coulomb, approximately 0.8 C of charge flows through a 100 watt light bulb every second. Or about 5 million trillion electrons every second. The rate of charges flowing through a conductor is called a current. We will get to this a few chapters later. No one has ever seen the charge, but we sure all see its effect in everyday life: electrostatic discharge in dry winter days to all the appliances (lights to motors to cell phones) that are powered by electricity.How much more do we know about the charge?1. The International system of Units, more reading: http://physics.nist.gov/cuu/Units/index.html.3Electric Charge and Coulomb’s LawCharge and charge upWhen the numbers of electrons and protons in an object are the same, we say that this object is (electrically) neutral. When they are not, we call it charged. There are many ways to charge up an object. A demo here:In this demo, we rub away or rub in electrons to make anobject positively or negatively charged.4Electric Charge and Coulomb’s LawConservation of electric chargesElectric charge is conserved. Charge can move between objects in the system, but the net charge of the system remains unchanged. Charges cannot be created or destroyed in the system, because charge is just a property of electrons and protons. They both are matter and matter conserves. A remark on anti-matter: matter and anti-matter annihilate into energy. So what’s more fundamental is the conservation of energy, but that’s beyond this class.8 = 10 + (-2), so O-21 decays to Ne-21 plus two electrons.5Electric Charge and Coulomb’s LawMovement of electric charges in matterA conductor: An object or material in which charge can flow relatively freely. Example: metal, carbon, …An insulator: An object or material in which charge does not flow freely. Example: plastic, glass, …To ground: Charge flows from a charged object to the ground, leaving the object neutral. The ground: A neutral object that can accept or supply an essentially unlimited number of charges. The Earth functions as an electric ground. Application based on these physics concepts: the lightning rod on tall buildings.6Electric Charge and Coulomb’s LawElectrostatics – forces between chargesUnlike charges attract; Like charges repel.7Electric Charge and Coulomb’s LawForces between charges – charge inductionThe force between charges provides a second way to charge up an object: This process is call induction.Charging an inductor:Charge rearrangement in insulators:8Electric Charge and Coulomb’s LawTo quantitatively study the forces between charges, we introduce the law of this chapter:The Coulomb’s Law of forces between two point charges in vector form:121212rrF221022141rqqrqqkePLAYACTIVE FIGURE221200022902112mNC 1085428space. free ofty permittivi theis 41CmN 1098768constant. Coulomb thecalled is to from directedr unit vecto theis . of because experience force theis Here/./.kk.qqqqe1212rF9Electric Charge and Coulomb’s LawDiscussions about Coulomb’s LawThe term point charge refers to a particle of zero size that carries an electric chargeThe force is inversely proportional to the square of the separation r between the charges and directed along the line joining themThe force is proportional to the product of the charges, q1 and q2, on the two particlesThe force is attractive if the charges are of opposite signThe force is repulsive if the charges are of like signElectrical forces obey Newton’s Third LawThe force on q1 is equal in magnitude and opposite in direction to the force on q2With like signs for the charges, the product q1q2 is positive and the force is repulsiveWith unlike signs for the charges, the product q1q2 is negative and the force is attractive2112FF10Electric Charge and Coulomb’s LawThe Superposition PrincipleThe resultant force on any one charge equals the vector sum of the forces exerted by the other individual charges that are presentIf there are four charges from q1 to q4, the resultant force on q1 is the vector sum of all the forces exerted on it by other charges: Remember to add forces as vectors: Problem solving template1 21 31 41= + +F F F Fr r r rTemplateStep 1, formulas or related concepts.Step 2, known quantities.Step 3, direct application of the formulas/concept or the condition to form an equation.Step 4, vector involved?Step 5, unit in the final answer correct? Answered all were asked?11Electric Charge and Coulomb’s LawExample 1X axisStep 1, formulaStep 2, known quantities:x Fr F221x221 :axis-X theAlong , Law sCoulomb'rqqkrqqkeeC. 10601electron an of charge theand constant Them 3m 14 m, 6m )5(1 distances536192312321.ekrr,eq,eq,eqe12Electric Charge and Coulomb’s LawStep 3, direct application of the formula twice:Step 4, vector involved? Yes, and the answer


View Full Document

SMU PHYS 1304 - Electric Charge and Coulomb’s Law

Documents in this Course
Force

Force

27 pages

Magnets

Magnets

12 pages

Thin Lens

Thin Lens

19 pages

Load more
Download Electric Charge and Coulomb’s Law
Our administrator received your request to download this document. We will send you the file to your email shortly.
Loading Unlocking...
Login

Join to view Electric Charge and Coulomb’s Law and access 3M+ class-specific study document.

or
We will never post anything without your permission.
Don't have an account?
Sign Up

Join to view Electric Charge and Coulomb’s Law 2 2 and access 3M+ class-specific study document.

or

By creating an account you agree to our Privacy Policy and Terms Of Use

Already a member?