Electricity and magnetism Chapter Six: Current and Resistance

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Electricity and magnetism Chapter Six: Current and Resistance nine week 23/ 2/ 1439 هـ 26/ 2/ 1439 هـ أ / سمر السلمي

Office Hours The sixth Homework Monday and Wednesday from 1 to 2 p.m. you can put any paper or homework in my mailbox in Faculty of Physics Department. my email is smsolamy@uqu.edu.sa for any question. I will put any announcement or apology in my website (https://uqu.edu.sa/smsolamy) , so please check it The sixth Homework I put the sixth homework in my website in the university homework Due Sunday /3 / 1439 هـ 4 in my mailbox in Faculty of Physics Department , I will not accept any homework after that , but if you could not come to university you should sent it to me by email in the same day

Chapter Six: Current and Resistance In the last five chapters we discussed electrostatics (the physics of stationary charges. In this and the next chapter, we discuss the physics of electric currents) that is, charges in motion. Electrical engineers are concerned with countless electrical systems, such as power systems, lightning protection systems, information storage systems, and music systems. Space engineers monitor and study the flow of charged particles from our Sun because that flow can wipe out telecommunication systems in orbit and even power transmission systems on the ground. In this chapter we discuss the basic physics of electric currents and why they can be established in some materials but not in others. We begin with the meaning of electric current.

1) Electric Current : an electric current is a stream of moving charges in time ……(1) The free electrons (conduction electrons) in an isolated length of conductor wire are in random motion at a speeds. The electrons pass through it in both directions at the rate of many electrons per second—but there is no net transport of charge and thus no current through the wire. However, if you connect the ends of the wire to a battery, as in the figure, it flows in one direction. Thus, there now is a net transport of charge and thus an electric current through the wire. as in Fig. we insert a battery in the loop, the wire is no longer at a single potential. Electric fields act inside the material making up the wire, exerting forces on the conduction electrons, causing them to move and thus establishing a current. After a very short time, the electron flow reaches a constant value and the current is in its steady state. The SI unit for current is the coulomb per second, or the ampere (A), which is an SI base unit:

1) Electric Current : Current is a scalar because both charge and time in are scalars Figure shows a conductor with current i0 splitting at a junction into two branches. Because charge is conserved, the magnitudes of the currents in the branches must add to yield the magnitude of the current in the original conductor, so that Current arrows show only a direction (or sense) of flow along a conductor, not a direction in space. A current arrow is drawn in the direction in which positive charge carriers would move, even if the actual charge carriers are negative and move in the opposite direction. as previous figure in previous slid

2) Current Density If we study the flow of charge through a cross section of the conductor at a particular point. To describe this flow, we can use the current density j which has the same direction as the velocity of the moving charges if they are positive and the opposite direction if they are negative. magnitude J is equal to the current per unit area through that element ……(2) ……(3) where A is the total area of the surface. From Eq. 2 or3we see that the SI unit for current density is the ampere per square meter (A/m2). Current density is a vector

2) Current Density Drift Speed When a conductor does not have a current through it, its conduction electrons move randomly, with no net motion in any direction. When the conductor does have a current through it, these electrons actually still move randomly, but now they tend to drift with a drift speed vd . We can use Fig. to relate the drift speed vd of the conduction electrons in a current through a wire to the magnitude J of the current density in the wire. Fig. shows the equivalent drift of positive charge carriers in the direction of the applied electric field E ……(4) SI unit is the coulomb per cubic meter (C/m3). For positive carriers, ne is positive and Eq. 4 predicts that J and vd have the same direction. For negative carriers, ne is negative and J and vd have opposite directions.

2) Current Density Sample Problem 1 Sample Problem 2 One end of an Aluminum wire whose diameter is 2.5 mm is welded to one end of copper wire whose diameter is 1.8 mm. The composite wire carriers a steady current of 1.3 A. What is the current density in each wire? What is the drift speed of conduction electrons in the copper wire if you know number of electrons per unit volume is 8.49 x 10 28 electrons/m3 ? Sample Problem 2 A strip of silicon of width 3.2 mm and thickness 250 µm carries a current of 190 mA. The silicon n-type semiconductor. having been doped with Phosphorus impurity. The doping has effect of greatly increasing n, the number of charge carriers per unit volume 8 x 1021 m-3 What is the current density in the strip? What is the drift speed?

3) Resistance, Resistivity and Conductivity: We determine the resistance between any two points of a conductor by applying a potential difference V between those points and measuring the current i that results. The resistance R is then ….. (5) The SI unit for resistance that follows from Eq.5 is the volt per ampere. The name is ohm (symbol Ω ); that is, A conductor whose function in a circuit is to provide a specified resistance is called a resistor. In a circuit diagram, we represent a resistor and a resistance with the symbol Another symbol is change resistor .

3) Resistance, Resistivity and Conductivity: Related to resistance is the resistivity ρ , which is a characteristic of a material ….. (6) Table lists resistivities of some materials at temp. 20 0C. The SI unit for resistivity that follows from Eq.6 is the ohm meter.(symbol Ω. m); that is, We often speak of the conductivity σ of a material. This is simply the reciprocal of its resistivity, so ….. (7) The SI unit of conductivity is the reciprocal ohm-meter, (Ω. m)-1

3) Resistance, Resistivity and Conductivity From last sild Resistance is a property of an object. Resistivity is a property of a material. We can calculating resistance from resistivity ….. (8) Sample Problem 3 A rectangular block of iron has dimensions 1.2 cm, 1.2 cm, 15 cm. A potential difference is to be applied to the block between parallel sides and in such a way that those sides are equipotential surfaces (as in Fig). What is the resistance of the block if the two parallel sides are (a) the square ends (with dimensions 1.2 cm x 1.2 cm) ? (b) two rectangular sides (with dimensions 1.2 cm x 15 cm)? 𝐽= 𝜎 𝐸= 1 𝜌 𝐸

4) Ohm’s Law: Ohm’s law is an assertion that the current through a device is always directly proportional to the potential difference applied to the device. conducting device obeys Ohm’s law when the resistance of the device is independent of the magnitude and polarity of the applied potential difference. A conducting material obeys Ohm’s law when the resistivity of the material is independent of the magnitude and direction of the applied electric field. V= i R

5) Power in Electric Circuits: Figure shows a circuit consisting of a battery B that is connected by wires, which we assume have negligible resistance, to an unspecified conducting device. The device might be a resistor, a motor, or some other electrical device. the battery maintains a potential difference of magnitude V across of the unspecified device, the electric potential energy to the device given by The principle of conservation of energy tells us that the decrease in electric potential energy from a to b is accompanied by a transfer of energy to some other form. The power P associated with that transfer is the rate of transfer dU/dt, which is given by ….. (9) The unit of power that follows from Eq. 9 is the volt-ampere (V. A). We can write it as

5) Power in Electric Circuits: For a resistor or some other device with resistance R, we can combine Eqs. 5 and 9 to obtain, for the rate of electrical energy dissipation due to a resistance, either Or ….. (10) Sample Problem 4 You are given a length of uniform heating wire made of a nickel–chromium–iron alloy called Nichrome; it has a resistance 72Ω . At what rate is energy dissipated in each of the following situations if A potential difference of 120 V is applied across? a) the full length of the wire? b) the length of each half when the wire is cut in half? Sample Problem 5 a current go through a wire of aluminum with 0.5 A and potential difference of 10 mV is applied across the wire. Find the electric power dissipation is?