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10/27/2014 Electric Field • Force per Unit test charge: A Ratio Electric Field & Potential Physics 115 Eyres E= Fonq0byQ • From Coulomb’s Law q0 kQq0 2 E= r q0 E= Comparing Fields • Electric Fields F= kqby qon 2 r kqby F = 2 qon r F = Eqon kQ r2 Electric field due to a single point-like charged object • Gravitational Fields F= Gmby mon r2 Gmby F = 2 mon r F = gmon © 2014 Pearson Education, Inc. Find Fe Using the superposition principle • Find the Electric Force on q1 caused by the q2 and q3. • q1= q2 = 4 µC 8m • q3 = q4= -3 µC q1 q2 q4 • R12=5 m • R13=8m q3 6m © 2014 Pearson Education, Inc. 1 10/27/2014 Finish the problem F on 1 by 2 @37 degrees W of N F= 8.99 x109 Negative 5.75x10-3 sin 37º= Nm 2 −6 −6 ( 4 x 10 C )( 4 x 10 C ) -3.46x10-3 C2 52 m 2 F on 1 by 3 @ -90 degrees F= 8.99 x109 Zero Nm 2 (4 x10 −6 C )(3 x10 −6 C ) C2 82 m 2 Resultant F on 1 by 2 and 3 = 4.52x10-3N @ 40º above –x axis -3.46x10-3 Positive 5.75x10-3 cos 37º= +4.6x10-3 Negative -1.69x10-3 Find Ee • Find the Electric Field at location p caused by the q2 and q3. • q2 = 4 µC 8m • q3 = q4= -3 µC p q2 q4 2.91x10-3 • R12=5 m • R13=8m q3 6m Finish the problem E at 1 by 2 @37 degrees W of N E= 8.99 x109 Nm 2 ( 4 x10 −6 C ) C2 2 2 5 m E at 1 by 3 @ -90 degrees E= 8.99 x109 Nm 2 (3 x10 −6 C ) C2 82 m 2 Resultant E at 1 by 2 and 3 = E field lines Field Lines Electric Field © 2014 Pearson Education, Inc. Gravitational Field Fig. 15.13, p.399 2 10/27/2014 E field lines Simulations • http://www.vias.org/si mulations/simusoft_efi eld.html • http://phet.colorado.ed u/sims/charges-andfields/charges-andfields_en.html © 2014 Pearson Education, Inc. Electric potential due to a single charged object © 2014 Pearson Education, Inc. Quantitative Exercise 15.6 • Suppose that the heart's dipole charges −Q and +Q are separated by distance d. Write an expression for the V field due to both charges at point A, a distance d to the right of the +Q charge. 1. Simplify and diagram. 2. Represent mathematically. − , = 2 + , = 1 Add: = © 2014 Pearson Education, Inc. + Potential difference • The value of the electric potential depends on the choice of zero level, so we often use the difference in electric potential between two points. = © 2014 Pearson Education, Inc. 3 10/27/2014 Checking Understanding Change in Electric Potential = = ! − = − = − = " ! " = Rank in order, from largest to smallest, the electric potentials at the numbered points. Δ #$ %& '( ! " - − #$ %& ') ! " − =Δ = HINT: Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Example A proton has a speed of 3.5 x 105 m/s at a point where the electrical potential is 600 V. It moves through a point where the electric potential is 1000 V. What is its speed at this second point? Its about Energy! How do you know? Δ =Δ Equipotential surfaces: Representing the V field • The lines represent surfaces of constant electric potential V, called equipotential surfaces. • The surfaces are spheres (they look like circles on a twodimensional page). © 2014 Pearson Education, Inc. Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Contour maps: An analogy for equipotential surfaces A Topographic Map © 2014 Pearson Education, Inc. Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. 4 10/27/2014 Graphical Representations of Electric Potential Δ Connecting Potential and Field =Δ Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Potential and Field for Three Important Cases The Potential Inside a Parallel-Plate Capacitor Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. +,-./ = Δ Δ0 Slope = E Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Example Example A proton is released from rest at point a. It then travels past point b. What is its speed at point b? A proton has a speed of 3.5 x 105 m/s at a point where the electrical potential is 600 V. It moves through a point where the electric potential is 1000 V. What is its speed at this second point? (How is this similar to the previous problem?) Its about Energy! How do you know? Δ Its about Energy! How do you know? =Δ Δ =Δ Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. 5 10/27/2014 Example: (How is this similar to the previous problems?) Example For the situation shown in the figure, find A parallel-plate capacitor is held at a potential difference of 250 V. A proton is fired toward a small hole in the negative plate with a speed of 3.0 x 105 m/s. What is its speed when it emerges through the hole in the positive plate? (Hint: The electric potential outside of a parallel-plate capacitor is zero). A. The potential at points a and b.The potential difference between a and b. B. The potential energy of a proton at a and b. C. The speed at point b of a proton that was moving to the right at point a with a speed of 4.0 x 105 m/s. D. The speed at point a of a proton that was moving to the left at point b with a speed of 4.0 x 105 m/s. Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Example Source charges create the electric potential shown. A. What is the potential at point A? At which point, A, B, or C, does the electric field have its largest magnitude? B. Is the magnitude of the electric field at A greater than, equal to, or less than at point D? C. What is the approximate magnitude of the electric field at point C? D. What is the approximate direction of the electric field at point C? Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. 6