《Electromagnetism, principles and application》教学课件（PPT讲稿）Chapter 5 Direct Currents in Electric Circuits

Chapter 5 Direct Currents in Electric circuits Conduction of Electricity a Ohm's law Non inear resistors Resistors connected Kirchhoff's laws Substitution theorem Mesh current

Chapter 5 Direct Currents in Electric Circuits ◼ Conduction of Electricity ◼ Ohm’s Law ◼ Non-linear Resistors ◼ Resistors Connected ◼ Kirchhoff’s Lawss ◼ Substitution Theorem ◼ Mesh Current

Voltage and current Sources a Thevenin theorem a transient in rc circuits If the electric field e is maintained in conductor by an external source say, a battery, then charges drift in the field and there is an electric current

◼ Voltage and Current Sources ◼ Thevenin Theorem ◼ Transient in RC Circuits If the electric field E is maintained in conductor by an external source, say, a battery, then charges drift in the field and there is an electric current

5.1 Conduction of electricity The current density vector J Its magnitude is the amount of charge flowing thru a surface in unit time. and has unit collom ampere second. meter meter It points in the direction of flow of positive charge If negative charges flow such as conduction electrons in a conductor, then j points in the opposite direction of flow of negative charges. ( See fig5-1 Seme-conductors contain one or two types of mobile charge, namely electrons and holes For ordinary conductors it holds that J=FE

Here o is the conductivity of the material. (see Table 5-1 for various common materials. Microscopically speaking, current in conductor forms due to the drift of conduction electrons =ne, where n--the conduction electron density the magnitude of the electron charge, the drift velocity of the electron charge For example, in copper, n=8.5 x 102elctron/M if =100 A/M, then the drift velocity ==74×10-5M/s~0.26M/h en he drift velocity is low different from thermal motion( 10 M s

Conservation of Charge Now consider a volume t bounded by a surface s inside conducting material. Let da be a small element of area on S J. da is the charge flowing out thru da per unit time Then /J·da is the charge flowing out of s per unit time, which is also the charge lost by the volume T per unit time dt r. Thus, one has the conservation of charge d Is J. da 1分md T di

Using the divergence theorem, the l h s of the equation is written as a volume integration /sJda=V·Jd7, so the conservation equation is V·Jar h pd Since this is valid for an T is arbitrary V·J This is the conservation of charge stated in differential orm

Homogeneous Conductor in Steady state If the system is in steady state, -dtp=0, thus V·J=0 Then by j=oE, one has V·E=0 If the conductor is also homogeneous, o is independent of position one has V·E=0. Thus by v.E=p/∈0, i.e. under steady-state condition the net charge den sity inside a homogeneous conductor carrying a current s zero

5.2 Ohm's Law Given an element of conductor of length l and cross section a If a potential difference v is maintained btwn its two ends there appears a current I From -oE withJ=I/A andE=v/1, one has A so the current is given by the following Where the resistance is 1≡ A --Ohm's Law

Remarks (1)The current thru a resistor is a the voltage across 止t (2 )A resistor satisfying this law is said to be linear (3)The current and voltage are measured as in Fig.5-4 The current thru a voltmeter is usually assumed to be negligible compares with that thru R R Figure 5.4 Measurement of the current I through a resistor R, and of the voltage v across it. A circle marked I represents an ammeter, and a circle marked v,a voltmeter

The heat generated by the joule effect The work done on the carriers is Qv The work done on the carriers in unit time is QV The work done on the carriers in unit time and unit volume is VIV 732 JE=OE This is converted into the heat generated in unit time and unit volume due to the joule effect For a resistor carrying a current 1 the voltage acr ross it is IR, and the heat generated in unit time is IV=I(IR)=R