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PHY-102: Electrostatics – Lecture 4 Electric Potential, Slides of Thermodynamics

A lecture outline on electric potential in the context of electrostatics. It covers topics such as work done in electric fields, electric potential energy, equipotential surfaces, potential due to electric dipole, and potential of a charged conductor. The document also includes examples and problems to solve. The lecture is aimed at students studying physics at the university level.

Typology: Slides

2020/2021

Available from 02/18/2022

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Download PHY-102: Electrostatics – Lecture 4 Electric Potential and more Slides Thermodynamics in PDF only on Docsity! PHY-102: ELECTROSTATICS– LECTURE 4 ELECTRIC POTENTIAL LECTURE OUTLINE • Work Done in Electric Field • Electric Potential Energy • Electric Potential • Equipotential Surfaces • Finding V from E • Potential due to Electric Dipole • Calculating E from V • Potential of a charged conductor POTENTIAL ENERGY AND WORK DONE ➢ Electric field is a conservative field. ➢ Due to work done there is a change in potential energy of the charge field system given by U = 𝑈𝑓 −𝑈𝑖 =−WAB U = −q0Es cos B A s E C  POTENTIAL ENERGY AND WORK DONE : POINT CHARGE Ede 9 or tren : " , . aside P — AE - (VB13 Pty Osieosyal mi Lert — \_\ October 3, 2007 POTENTIAL ENERGY AND WORK DONE • Cases • ∆𝑈 > 0 • ∆𝑈 = 0 • ∆𝑈 < WORK: POSITIVE OR NEGATIVE? 2. In the right figure, we move the proton from point i to point f in a uniform electric field directed as shown. Which statement of the following is true? A. Electric field does positive work on the proton; And Electric potential energy of the proton increases. B. Electric field does negative work on the proton; And Electric potential energy of the proton decreases. C. Our force does positive work on the proton; And Electric potential energy of the proton increases. D. Electric field does negative work on the proton; And Electric potential energy of the proton decreases. Eif ELECTRIC POTENTIAL FROM ELECTRIC FIELD  −=   f i sdE q U V  0 October 3, 2007 ❑ The electric potential energy ◼ Start ◼ Then ◼ So ❑ The electric potential q U V = q U q U q U VVV if if  =−=−= sdFdW  = sdEqdW  = 0 sdEqW f i  = 0  −=−=−= f i if sdEqWUUU  0 ❑ Potential difference depends only on the source charge distribution (Consider points i and f without the presence of the test charge; ❑ The difference in potential energy exists only if a test charge is moved between the points. POTENTIAL DUE TO A POINT CHARGE • Start with (set Vf=0 at  and Vi=V at R) • We have • Then • So • A positively charged particle produces a positive electric potential. • A negatively charged particle produces a negative electric potential 2 04 1 r q E  = 2 04 1 r q E  =    −=−=−=−= f i R f i if EdrdsEsdEVVV )0cos(  r q rV 04 1 )(  = R q r q dr r q V R R 00 2 0 4 11 4 1 4 0  −=      =−=−    END PROBLEMS -6.00 0 Y 3.00 m Ve 3.00 m Hy 2.00 uC 4.00 2.00 U6 1.00 m re * (a) (b) 1-4 2+) Vp eVieVe i , Ve = eM Kee ny b Rz2 -f q - =Aa ID , arto —SNO Ve 5 a 2, =9 +10 (% - “] 29510 cc = ale 40 Volt ) | 2. Derive an expression for the work required by an external agent to put the four charges together as indicated in Fig. 28- 28. Each side of the square has length a. \~) er the charges clockwise E28-2 There are six interaction terms, one for every charge trom the upper left hand corner. Then fe __ Uj2 = —q?/Aneoa, +q | -4 Uox3 = —q ?/ dicoa, Ry Usy = —q?/ anots S Uy = —-@ 2 Ameo, ro Ube U3 = (~q)* eo(V2a) ; =e +@ Add these terms and get The amount of work required el
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