Presentation on theme: "Chapter 18. Electric Charges and Forces"— Presentation transcript:
1Chapter 18. Electric Charges and Forces The electric force is one of the fundamental forces of nature. Controlled electricity is the cornerstone of our modern, technological society.Chapter Goal: To develop a basic understanding of electric phenomena in terms of charges, forces, and fields.
2Learning objectivesTo become familiar with basic electric phenomenaTo understand and use Coulomb’s Law for point chargesTo begin the process of understanding the field model and the concept of the electric field
3Electric charge is a fundamental conserved property of some subatomic particles, which determines how they interact (i.e. attraction/repulsion)Substantial experimentation supports the existence of only 2 different types of charge.Benjamin Franklin introduced the modern nomenclature of positive/negative for the 2 types of charge. These terms have nothing to do with greater or less than (as in math) or direction (as in vectors).Electric charge is a conserved quantity. If a system becomes negatively charged, the rest of the universe acquires a positive charge of the same magnitude and vice versa.
4Familiar charged particles include the proton and the electron. The SI unit of electric charge is the Coulomb (C).A Coulomb is a lot of charge! The charge of one proton or electron is:Objects become charged when they have an excess or a deficit of electrons, which are mobile.Like charges (pos/pos or neg/neg) repel each otherUnlike charges attract.Neutral objects are attracted to both kinds of charge. That will be explained later in the chapter.
5Each of three objects carries a charge Each of three objects carries a charge. As the drawing shows, objects A and B attract each other, and objects C and A also attract each other. Which one of the following statements concerning objects B and C is true?They attract each other. They repel each other. They neither attract nor repel each other. This question cannot be answered without additional information.Charged particlesEach of three objects carries a charge. As the drawing shows, objects A and B attract each other, and objects C and A also attract each other. Which one of the following statements concerning objects B and C is true?They attract each otherThey repel each otherMore information needed to answer the question.
6Conservation of Charge The rod carries a charge of -3.0 μC, while the conducting sphere carries a charge of +2.0 μC. The two charged objects touch.What is the final charge state of both rod and sphere?b. How many electrons travel from the rod to the sphere to produce the final charge state?
7Conservation of Charge The rod carries a charge of -3.0 μC, while the conducting sphere carries a charge of +2.0 μC. The two charged objects touch.What is the final charge state of both rod and sphere? -0.5 µC (-3 + 2)/2How many electrons travel from the rod to the sphere to produce the final charge state?(1electron/-1.6x10-19C) (-2.5x 10-6 C) = 1.6 x electrons
8Four spheres-AFour identical metal spheres have charges of qA = −8.0 µC, qB = −2.0 µC, qC = +5.0 µC, and qD = µC. Two of the spheres are brought together so they touch, and then they are separated. Which spheres are they, if the final charge on each of those two is +5.0 µC?A. AB B. AC C. AD D. BD
9Which diagram best represents the charge distribution on three neutral conducting spheres when a positively charged rod is brought near sphere x, but does not touch it?1234None of the diagrams
10InsulatorsThe electrons in the insulator are all tightly bound to the positive nuclei and not free to move around.Charging an insulator by friction leaves patches of molecular ions on the surface, but these patches are immobile.Plastic, styrofoam, wool, silk are examples of insulators.
11ConductorsIn conductors, the outer atomic electrons are only weakly bound to the nuclei.These outer electrons become detached from their parent nuclei and are free to wander about through the entire solid.The solid as a whole remains electrically neutral, but the electrons act like a negatively charged liquid permeating an array of positively charged ion cores.Most conductors are metals.
12Insulators and Conductors can both acquire a charge but….
13Charging ObjectsFrictional charging: Some insulators lose or gain surface electrons if rubbed. In a conductor the charge will “diffuse” over the entire object instead of staying near the rubbed area.Charging by contact: Charge can be transferred from one charged object to another. This works for both insulators and conductors, but in the latter case, the charge will travel and spread out over the surface of the conductor.
14John Travoltage http://phet.colorado.edu/en/simulation/travoltage Is John an insulator or a conductor? Justify your answer. Notice how charge transferred from the carpet acts and where it goes when John rubs his foot.Describe what happens when he touches the door handle. Explain why this happens.
15Charging Objects, cont’d Charging by Induction: If the negatively-charged rod is brought close to a conductor, the conductor will become “polarized”, meaning charge will separate (a). If a wire is attached between sphere and the earth (ground), electrons will travel down the wire (b). When first the wire, then the rod, is removed, a positive charge remains on the conductive sphere. This only works for conductors.
16Stop to Think: Is Order Important? What would happen if, in situation (b) below, we took the rod away first, then disconnected the grounding wire?The metal sphere would still have a positive charge, because the order of events doesn’t matterThe metal sphere would remain neutral because with the rod gone, the electrons that went down the wire would travel back up the grounding wireThe metal sphere would become negative because once the rod is gone, too many electrons would travel up the grounding wire.
17Polarization: Why neutral objects are attracted by charged objects The picture below should explain why a neutral conductor is attracted to a charged object.The positive charges (electron holes?) are attracted to the rod while the electrons are repelledThe attractive force is stronger than the repulsive force because the electron holes are closer than the electrons.If there were no frictional force between the stand and the floor, thesphere would slide to the rod.But insulators are attracted too. What about them?
20The air is an insulator, except….. Although air is normally an excellent insulator, when stressed by a sufficiently large electric field, air can begin to ionize, becoming partially conductive. This culminates in an electrical spark or arc that bridges the entire gap.This is the same phenomenon that occurs during a lightning storm.
21COULOMB’S LAW In SI units k = 8.99 × 109 N m2/C2. k = 1/4πε0, where ε0 is called the permittivity of free space and equals 8.85x C2/(N m2).Note: Assume the weight force is negligible unless otherwise specified in problems and diagrams.
23Charges A and B exert repulsive forces on each other. qA = 4qB Charges A and B exert repulsive forces on each other. qA = 4qB. Which statement is true?STT25.4Answer: CFA on B > FB on AFA on B < FB on AFA on B = FB on A
24Example 4 Three Charges on a Line 18.5 Coulomb’s LawExample 4 Three Charges on a LineDetermine the magnitude and direction of the net electrostatic force on q1.
27Charges in a lineThe drawing shows three point charges arranged in three different ways. The charges are +q, -q, and -q; each has the same magnitude, with one positive and the other two negative. In each of the arrangements the distance d is the same. Rank the arrangements in descending order (largest first) according to the magnitude of the net electrostatic force that acts on the positive charge.A. ABC B. BCA C. CAB D. CBA
28Bohr model of the Hydrogen Atom 18.5 Coulomb’s LawBohr model of the Hydrogen AtomIn the Bohr model of the hydrogen atom, the electron is in orbit about thenuclear proton at a radius of 5.29x10-11m. If me = 9.11 x kg, determinea. the speed of the electron, assuming the orbit to be circular.b. the kinetic energy of the electron
2918.5 Coulomb’s Law1. Draw a fbd of the electron (ignore weight force, even though mass is used)2. Use Newton’s 2nd Law: ΣF = ma. In this case, there is only the electrical force, and a is a centripetal acceleration; a = v2/r and
31Now calculate kinetic energy: KE = ½ mv2 K = 2.16 x 10-18 J 18.5 Coulomb’s LawNow calculate kinetic energy: KE = ½ mv2K = 2.16 x J
32The Electric Field Model: Newton vs Faraday In this illustration, consider A to be one or more source charges, in that it is the source of the “alteration of space”.Consider B to be the test charge (q0), a small visitor to the neighborhood.
33The Electric FieldSome charges, which we will call the source charges, alter the space around them by creating an electric field.A test charge in the electric field experiences a force exerted by the field.Suppose test charge q0 experiences an electric force F due to the source charges. The value of the electric field is the force experienced by q0 divided by the value of q0.The units of the electric field are N/C. The magnitude E of the electric field is called the electric field strength.
34The Electric FieldThe electric field vector points in the same directions as that of the electrostatic force on a positive test chargeThe electric field vector points in the opposite direction from the electrostatic force on a negative test chargeThe electric field due to one or more source charges exists in all space whether there is a test charge or not
35An electron in an E field The electron is placed at the position marked by the dot. The force on the electron is:Zero C. To the leftTo the right D. Not enough information
36Electric field strength due to a point charge q Note that the electric field strength does not depend on the test charge; it isdivided outFor a point charge q:
37Example ProblemTwo charges are placed on the x axis. One of the charges (q1 = +9.1 µC) is at x1 = +2.8 cm and the other (q2 = -22 µC) is at x2 = +8.7 cm. Find the net electric field (magnitude and direction) at x = 0 cm. (Use the sign of your answer to indicate the direction along the x-axis.). In SI units k = 8.99 × 109 N m2/C2. 1 cm = 10-2 m
38Example ProblemTwo charges are placed on the x axis. One of the charges (q1 = +9.1 µC) is at x1 = +2.8 cm and the other (q2 = -22 µC) is at x2 = +8.7 cm. Find the net electric field (magnitude and direction) at x = 0 cm. (Use the sign of your answer to indicate the direction along the x-axis.). In SI units k = 8.99 × 109 N m2/C2. 1 cm = 10-2 m Ans: x 107 N/C
39Electric field strength Rank electric field strengths at points a,b,c,d from greatest to least:
40The E field vectorThe electric field vector at 1 can be represented by the arrow shown above. How long are the arrows at 2 and 4? Explain your reasoning.
41c. If the distance between the unseen point charge and the 900 N/C point is r1, and the distance between the unseen point charge and the 400 N/C is r2, by what factor is r2 > r1 ? Explain your reasoning.
42THE PARALLEL PLATE CAPACITOR The capacitor is a charge-storage device used in many electrical appliances and circuits.The simplest type is the parallel plate capacitor, two metal plates of area A.Each plate has an equal amount of charge, with one being positive and the other negative.The electric field inside the capacitor is constant and does not depend on the distance from the plates.σ = q/A = charge density
43Electric field of a cell membrane The membrane surrounding a living cell consists of an inner and an outer wall that are separated by a small space. Assume that the membrane acts like a parallel plate capacitor in which the effective charge density on the inner and outer walls has a magnitude of 7.1x10-6 C/m2. What is the magnitude of the electric field within the cell membrane?
44Electric field of a cell membrane The membrane surrounding a living cell consists of an inner and an outer wall that are separated by a small space. Assume that the membrane acts like a parallel plate capacitor in which the effective charge density on the inner and outer walls has a magnitude of 7.1 x 10-6 C/m2. What is the magnitude of the electric field within the cell membrane? E = σ/ε0 andE = σ/ε0= x 10-6 C/m28.85 x C2 /(N · m2 )E = x 105 N/C
4518.7 Electric Field LinesElectric field lines or lines of force provide a map of the electric field in the space surrounding electric charges. Figure a shows electric field vectors.Figure b shows the electric field lines due to a positive point charge source.
4618.7 Electric Field LinesElectric field lines are always directed away from positive source charges and toward negative source charges.The line spacing indicates the strength of the field. More closely spaced lines indicate a stronger field. Parallel lines indicate a constant field.The number of field lines drawn is proportional to the strength of the field; twice as many lines would emerge from a charge of 2q than from a charge of q.Electric field lines always begin on a positive charge and end on a negative charge and do not stop in midspace.The direction of electric field (force on a positive test charge) is tangent to the field line at that place in space.
47Electric field lines due to a point charge Positive NegativeElectric field lines are always directed away from positive source charges and toward negative source charges. Lines are more closely spaced close to the charge, where the field is stronger.
4818.7 Electric Field LinesField lines for an electric dipole. Note the direction of the electric force vector, tangent to the field line.
49Field lines for 2 like charges. Where is the electric field zero?
5018.7 Electric Field LinesThe parallel plate capacitor has a constant electric field in the interior of the plate, shown by parallel lines. The field strength is the same, regardless of position.
51Which is the correct field line configuration? Why are the other 3 incorrect?
52Focus on ConceptsThe drawing shows some electric field lines. For the points indicated, rank the magnitudes of the electric field in descending order (largest first).BCA C. CAB E. ABCBAC D. ACB