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أستاذ المادة احمد باقر رضا حمود شربة
21/01/2018 07:50:33
Lecture 4 GAUSS S LAW This law states that the total electric flux ? through any closed surface, or (equivalently) the surface integral over the normal component of the electric field vector E over that closed surface, equals the net charge ?_n?q_n inside the surface: ?=???E.dS?=1/?_o ?_n?q_n =1/?_o ?_V??dV …. (1-8) where dS is the surface element vector at any point p on the surface surrounding the volume V. If the charge is distributed within the volume, ? is the localized charge density within a volume element dV. This law can be expressed in differential form as ??D=? …… (1-9) (how?) This is considered the first of Maxwell s equations. BIOT-SAVART LAW B=?_o/4? ?_V??J(V)×r/|r|^3 dV? …….. (1-10) where J(V) is the current density within volume element dV and r is the position vector from volume element dV to the point of measurement of B. It can be expressed in differential form as: B=?_o/4? ?×???(J(V))/|r| dV? …….. (1-11) which leads directly to: ??B=0 ………. (1-12) (How?) (Prove it) since B is the curl of another vector. This is considered the second of Maxwell s equations.
GAUSS S LAW This law states that the total electric flux ? through any closed surface, or (equivalently) the surface integral over the normal component of the electric field vector E over that closed surface, equals the net charge ?_n?q_n inside the surface: ?=???E.dS?=1/?_o ?_n?q_n =1/?_o ?_V??dV …. (1-8) where dS is the surface element vector at any point p on the surface surrounding the volume V. If the charge is distributed within the volume, ? is the localized charge density within a volume element dV. This law can be expressed in differential form as ??D=? …… (1-9) (how?) This is considered the first of Maxwell s equations. BIOT-SAVART LAW B=?_o/4? ?_V??J(V)×r/|r|^3 dV? …….. (1-10) where J(V) is the current density within volume element dV and r is the position vector from volume element dV to the point of measurement of B. It can be expressed in differential form as: B=?_o/4? ?×???(J(V))/|r| dV? …….. (1-11) which leads directly to: ??B=0 ………. (1-12) (How?) (Prove it) since B is the curl of another vector. This is considered the second of Maxwell s equations.
المادة المعروضة اعلاه هي مدخل الى المحاضرة المرفوعة بواسطة استاذ(ة) المادة . وقد تبدو لك غير متكاملة . حيث يضع استاذ المادة في بعض الاحيان فقط الجزء الاول من المحاضرة من اجل الاطلاع على ما ستقوم بتحميله لاحقا . في نظام التعليم الالكتروني نوفر هذه الخدمة لكي نبقيك على اطلاع حول محتوى الملف الذي ستقوم بتحميله .
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