4- Direct Current Circuits

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Presentation transcript:

4- Direct Current Circuits 1- Resistors in series and in parallel 2-Kirchhoff`s Rules سنتعامل فى هذا الفصل مع الدوائر الكهربية التى تحتوى على بطارية ومقاومة . سنتعرف على توصيل المقاومات على التوالى والتوازى ثم نستخدم قاعدتا كيروشوف لحساب التيار الكهربى الما فى كل عنصر من عناصر الدائرة الكهربية

مقاومات

بطاريات Fig 28-CO An assortment of batteries that can be used to provide energy for various devices. Batteries provide a voltage with a fixed polarity, resulting in a direct current in a circuit, that is, a current for which the charges always move in the same direction. (George Semple)

V V V  R

The total resistance R= R1+R2+R3 Resistors in series and in parallel Resistors in series The total resistance R= R1+R2+R3 التيار لا تيجزأ الجهد يتجزأ 1= 2 =  V= V1+V2

Resistors in parallel التيار يتجزأ الجهد لا يتجزأ 1+ 2 =  V= V1=V2 The total resistance R is given by 1+ 2 =  V= V1=V2 التيار يتجزأ الجهد لا يتجزأ

Example: Find the equivalent resistance between points a and c

Calculate the equivalent resistance of the circuit

Calculate the equivalent resistance of the circuits between a and b

تستخدم قاعدتا كيروشوف لتحليل الدوائر الكهربية المكونة من بطارية ومقامة لحساب التيار الكهربى المار فى كل عنصر من عناصر الدائرة

For closed loop abcda -6+8+12+10 = 0 +6+18=0 =-0.333 A