ECE 2317 Applied Electricity and Magnetism Prof. D. Wilton ECE Dept. Notes 16 Notes prepared by the EM group, University of Houston. Curl of a Vector V x, y, z arbitrary vector function curl V vector function z S Cz S y S 1 S 0 S 1 y curl V lim S 0 S 1 z curl V lim S 0 S x curl V lim Cx Cy Cz V dr V dr V dr V dr ofcirculation V on C Cx, y , z x, y, z x curl V circulation per unit area about x, etc. Cy x Cx Note: Paths are defined according to the “right-hand rule” Curl of a Vector (cont.) “curl meter” xˆ , yˆ , zˆ Assume that V represents the velocity of a fluid. curl V velocityof rotation (in the sense indicated) Curl Calculation z Path Cx : 4 1 z 2 3 Cx V dr Cx y y y V dx V dy V dz V , 0 z y z z 0, Cx x 2 y Vz 0, , 0 z 2 z Vy 0, 0, y 2 z Vy 0, 0, y 2 (side 1) (side 2) (side 3) (side 4) Curl Calculation (cont.) y y V 0, , 0 V 0, , 0 z z 2 2 V dr y z Cx y z z Vy 0, 0, 2 Vy 0, 0, 2 z y z Vy Vz S S y z Vz Vy C V dr S y z x Though above calculation is for a path about the origin, just add (x,y,z) to all arguments above to obtain the same result for a path about any point (x,y,z) . Curl Calculation (cont.) Vz Vy C V dr S y z x From the curl definition: Hence 1 s 0 S x curl V lim Vz Vy x curl V y z Cx V dr Curl Calculation (cont.) Similarly, Vx Vz V dr S C z x y Vx Vz y curl V z x Vy Vx C V dr S x y z Vy Vx z curl V x y Hence, Vz Vy Vx Vz Vy Vx curl V x y z z x x y z y x Note the cyclic nature of the three terms: y z Del Operator x y z y z x V x y z xVx yVy zVz y z x x y z x Vx y Vy z Vz Vz Vy Vz Vx Vy Vx x y z y z x z x y Del Operator (cont.) Hence, curl V V Example V x 3xy z y 2 x z z 2 xz 2 V 2 3 x y z x y z x Vx y Vy z Vz x 3xy 2 z y 2x2 z3 z 2 xz V x 0 3z 2 y 2 z 3xy z 4 x 6 xyz 2 Example V x y Vz Vy Vz Vx V x y z z x y Vy Vx z y x V z 1 y x Example (cont.) V z 1 V z 1 0 y x Summary of Curl Formulas Vz Vy Vz Vx Vy Vx V x y z y z x z x y 1 Vz V V Vz 1 V V V z z z 1 V sin V V r sin 1 1 Vr rV 1 rV Vr r r sin r r r Stokes’s Theorem S (open) n C n : chosen from “right-hand rule” applied to the surface V n dS V dr S C “The surface integral of circulation per unit area equals the total circulation.” Proof Divide S into rectangular patches that are normal to x, y, or z axes. ni r i n Ci S S n x, y, or z i C Independently consider the left and right hand sides (LHS and RHS) of Stokes’s theorem: LHS : V n dS V S i ri ni S Proof (cont.) S C LHS : V n dS V 1 ni V lim s 0 S ni V ri n i S i S 1 S ri Ci Ci V dr V dr V r ni S V dr i Ci e.g, ni x, y, z Proof (cont.) S C Hence, V i ri n i S V n ds S V dr V dr i Ci C V n ds V dr S C C (Interior edge integrals cancel) Example y CC Verify Stokes’s theorem for V x y = a, z= const V dr V CB C C CA dx V y dy C x x x dy C I C A I CB I CC V x y ICA 0 ( dy = 0 ) I CC 0 (x=0) (dz = 0) Example (cont.) IB x dy a y a y a 2 1 y IB sin 2 2 a y 0 2 CB y =a B CB x a 2 1 sin 1 2 a2 2 2 A a I B a 2 y 2 dy 0 I a2 4 2 Example (cont.) Alternative evaluation (use cylindrical coordinates): B I B V dr A B V d ˆ a d z dz A 2 V a d 0 Now use: V V y x x y x cos , x a cos or V a cos cos a cos 2 Example (cont.) Hence IB 2 a 2 cos 2 d 0 a2 1 cos2 0 2 d 2 2 sin 2 a2 4 0 2 a 4 2 a 2 I 4 Example (cont.) Now Use Stokes’s Theorem: I V dr V z ds C V xy (nˆ z) S Vz Vy Vz Vx Vy Vx V x y z y z x z x y V z 1 1 I z 1 z dS dS A a 2 4 S S I a2 4 Rotation Property of Curl n 1 V dr V n lim S 0 S C (constant) S (planar) C The component of curl in any direction measures the rotation (circulation) about that direction Rotation Property of Curl (cont.) n Proof: Stokes’s Th.: V n ds V dr S But C V n ds V n S S Hence (constant) V n S V dr C Taking the limit: 1 V dr V n lim S 0 S C S (planar) C Vector Identity V 0 Proof: Vz Vy Vz Vx Vy Vx V x y z y z x z x y Ax Ay Az V x y z A 2Vz 2Vy 2Vz 2Vx 2Vy 2Vx x y x z y x y z z x z y 0 Vector Identity V 0 Visualization: V Edge integrals cancel when summed over closed box! nˆ i Si Ci Flux of V out of V 1 V V face i V nˆ i Si 1 V dr Si C i 0 Example Find curl of E: 3 2 1 q s0 Infinite sheet of charge (side view) l0 Infinite line charge Point charge Example (cont.) 1 x s0 E xˆ 2 0 s0 Ez E y Ez Ex E y Ex E x y z z z x y x y E x 0 0 y 0 0 z 0 0 0 Example (cont.) 2 0 E 2 0 l0 1 Ez E E Ez 1 E E E z z z 0 Example (cont.) 3 q 1 E r sin q E r 2 4 0 r E sin E 1 1 Er rE 1 rE Er r r sin r r r 0 By superposition, the result E 0 , must be true for any general charge distribution Faraday’s Law (Differential Form) Stokes’s Th.: E n dS E dr 0 S (in statics) C n Let S S Hence S small planar surface E n dS 0 S Let S 0: n E S 0 n E 0 Faraday’s Law (cont.) n E 0 Let n xˆ , yˆ , zˆ : x E 0 y E 0 z E 0 Hence E 0 n S Faraday’s Law (Summary) E dr 0 Integral form of Faraday’s law C Stokes’s theorem curl definition E 0 Differential (point) form of Faraday’s law Path Independence V 0 Assume A B C1 I1 V d r C2 I2 V d r C1 C2 I1 I 2 Path Independence (cont.) Proof B A C C = C2 - C1 C C2 C1 V d r V n dS 0 S I 2 I1 0 S is any surface that is attached to C. (proof complete) Path Independence (cont.) V 0 Stokes’s theorem Definition of curl path independence V dr 0 C Summary of Electrostatics D v E 0 D 0 E Faraday’s Law: Dynamics In statics, E 0 Experimental Law (dynamics): B E t Faraday’s Law: Dynamics (cont.) B E t Bz zˆ E 0 t (assume that Bz increases with time) y magnetic field Bz (increasing with time) x electric field E Faraday’s Law: Integral Form B E t Apply Stokes’s theorem: E nˆ dS E d r S C B nˆ dS t S Faraday’s Law (Summary) B C E d r S t nˆ dS Integral form of Faraday’s law Stokes’s Theorem B E t Differential (point) form of Faraday’s law Faraday’s Law (Experimental Setup) + y V >0 - x Note: the voltage drop along the wire is zero magnetic field B (increasing with time) Faraday’s Law (Experimental Setup) + A y B C E d r S t nˆ dS Bz dS 0 t S V >0 - B C x S B V E dr A Hence E dr C V 0 (nˆ z) Note: the voltage drop along the wire is zero Differential Form of Maxwell’s Equations D v B E t B 0 D H J t electric Gauss law Faraday’s law magnetic Gauss law Ampere’s law Integral Form of Maxwell’s Equations D nˆ dS dV v S electric Gauss law V d C E d r dt S B nˆ dS B nˆ dS 0 Faraday’s law magnetic Gauss law S d C H d r S J nˆ dS dt S D nˆ dS Ampere’s law