Chapter 27 Current Resistance And Resistor. Electric Current, the definition Assume charges are moving perpendicular to a surface of area A If ΔQ is the.

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Presentation transcript:

Chapter 27 Current Resistance And Resistor

Electric Current, the definition Assume charges are moving perpendicular to a surface of area A If ΔQ is the amount of charge that passes through A in time Δt, then the average current is or I A Anyone notices a difference of this figure compared with the one in the book? If yes, and explain why I draw it this way. Correct answer = 1 bonus point How many of you preview, review, do homework within 2 days of class, 2 days toward due date?

Electric Current, definition and unit Electric current is the rate of flow of charge through some region of space The SI unit of current is the ampere (A) 1 A = 1 C / s And ampere is a base unit. The unit for time, second, is also a base unit. The unit for charge is then defined as 1C=1A/1s The symbol for electric current is I

Direction of Current The charges passing through the area could be positive or negative or both. This area may or may not be an actual physical surface and the charges can flow in a conductor or in vacuum. It is conventional to assign to the current the same direction as the flow of positive charges The direction of current flow is opposite the direction of the flow of electrons It is common to refer to any moving charge as a charge carrier

Current in a conductor and the drift speed Charged particles move through a conductor under the drive of an electric field inside. Wait! There should be no electric field inside a conductor. Explanation please! E Assume a cross-sectional area A that is perpendicular to and the number of charge carriers per unit volume n. Then nAΔx is the total number of charge carriers

Current linearly proportional to drift speed The total charge is the number of carriers times the charge per carrier, q ΔQ = (nAΔx)q The drift speed, v d, is the speed at which the carriers move v d = Δx / Δt and  x = v d  t Rewritten: ΔQ = (nAv d Δt)q Finally, current, I ave = ΔQ/Δt = nqv d A This is to say that current is linearly proportional to the drift speed v d

A typical value of the drift speed Assume a copper wire, with one free electron per atom contributed to the current The drift speed for a 12-gauge copper wire carrying a current of 10.0 A is 2.23 x m/s This is a typical order of magnitude for drift speeds This is very slow, how come when a switch is closed, the light comes on from a light bulb ~ 10m away? It should take ~10/ 2.23 x sec which is about 12 hours. What is wrong?

Motion of the charge carrier, the electrons, in a conductor The actual charge carrier in conductor is the electron The zigzag black lines represents the motion of a charge carrier in a conductor The net drift speed is small The sharp changes in direction are due to collisions The net motion of electrons is opposite the direction of the electric field The current direction is conventionally defined to be the positive carrier motion direction, or the electric field direction. PLAY ACTIVE FIGURE

Motion of Charge Carriers, final discussion The electric field exerts forces on the electrons in the wire at the same time (almost). These forces cause the electrons to move in the wire and create a current. So the current starts to flow anywhere in the circuit when the switch is closed. In the presence of an electric field, like the one set up by a battery, in spite of all the collisions, the charge carriers slowly move along the conductor with a drift velocity, The battery does not supply the electrons, it only establishes the electric field

Current Density J, the definition Current density is a vector and is in the direction of the positive charge carriers The current density J of the current I in a conductor is defined as the current per unit area J has SI units of A/m 2 The relationship to the current is

Conductivity, the definition A current density and an electric field are established in a conductor whenever a potential difference is maintained across the conductor For some materials, the current density is directly proportional to the field, that is The constant of proportionality, σ, is called the conductivity of the conductor