Current and Resistance. February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 1

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1 Current and Resistance February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 1

2 Helproom hours! Strosacker learning center, BPS 1248! Mo: 10am noon, 1pm 9pm! Tue: noon 6pm! We: noon 2pm! Th: 10am 1pm, 2pm 7pm! Fri: noon to 2pm February 12, 2014 Physics for Scientists & Engineers 2, Chapter 21 2

3 Resistance and resistivity! Resistance R of a resistor is given by R = ΔV i i = ΔV R or ΔV = ir! Units are Ohms 1 Ω = 1 V 1 A! Resistivity is a property of the material with current density ρ = E J J = i A! Resistance depends on resistivity and length and cross section area of the resistor R = ρ L A February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 3

An empirical relationship for the temperature dependence of the resistivity of metals is given by!

4 Temperature Dependence of Resistivity! The resistivity and resistance vary with temperature! For metals, this dependence on temperature is linear over a broad range of temperatures! An empirical relationship for the temperature dependence of the resistivity of metals is given by! where ( ) ρ ρ 0 = ρ 0 α T T 0 ρ is the resistivity at temperature T ρ 0 is the resistivity at temperature T 0 α is the temperature coefficient of electric resistivity February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 4

Temperature Dependence of Resistance! In everyday applications we are interested in the temperature dependence of the resistance of various devices!

5 Temperature Dependence of Resistance! In everyday applications we are interested in the temperature dependence of the resistance of various devices! The resistance of a device depends on the length and the cross sectional area! These quantities depend on temperature! However, the temperature dependence of linear expansion is much smaller than the temperature dependence of resistivity of a particular conductor! The temperature dependence of the resistance of a conductor is, to a good approximation, ( ) R R 0 = R 0 α T T 0 February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 5

6 Temperature Dependence! Our equations for temperature dependence deal with temperature differences so that one can use C as well as K (T-T 0 in K is equal to T-T 0 in C)! Values of α for representative metals are shown below (more can be found in Table 25.1) February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 6

7 Example: Which Metal is it?! A metal wire of 2mm diameter and length 300m has a resistance of Ω at 20 o C and Ω at 150 o C. Find the values of α, R(0 o C), ρ(0 o C) and identify the metal!! Solution: R(150 o C)=2.415Ω=R(0 o C)(1+α(150-0)) R(20 o C)=1.6424Ω=R(0 o C)(1+α(20-0)) First equation: R(0 o C)=2.451Ω/(1+α(150-0)), substitute in second equation, solve for α: α= o C -1 With α known, use any of the above equations to get R(0 o C)=1.5236Ω. Then use R(0 o C)=ρ(0 o C)L/A Ω = ρ(0 C) 300m 0.25π( m) 2 ρ(0 C) = Ωm ρ(20 C) = ρ(0 C)(1+ α 20) = Ωm Table 25.1: Copper! February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 7

Other Temperature Dependence! Most materials have a resistivity that varies linearly with the temperature under ordinary circumstances! However, some materials do not follow this!

8 Other Temperature Dependence! Most materials have a resistivity that varies linearly with the temperature under ordinary circumstances! However, some materials do not follow this! At very low temperatures the resistivity of some materials goes to exactly zero! These materials are called superconductors Many applications, including MRI! The resistance of some semiconducting materials actually decreases with increasing temperature! These materials are often found in high-resolution detection devices for optical measurements or particle detectors February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 8

9 Electromotive Force and Ohm s Law! To make current flow through a resistor one must establish a potential difference across the resistor! This potential difference is termed an electromotive force or emf! A device that maintains a potential difference is called an emf device and does work on the charge carriers! The emf device not only produces a potential difference but supplies current! The potential difference created by the emf device is termed V emf! We will assume that emf devices have terminals that we can connect and the emf device is assumed to maintain V emf between these terminals February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 9

convert energy from the Sun to electric energy! We will often use DC (direct current) power supplies, which supply emf just like a battery!

10 Circuit! Examples of emf devices are Batteries that produce emf through chemical reactions Electric generators that create emf from electromagnetic induction Solar cells that convert energy from the Sun to electric energy! We will often use DC (direct current) power supplies, which supply emf just like a battery! A circuit is an arrangement of electrical components connected together with ideal conducting wires (i.e., having no resistance)! Electrical components can be sources of emf, capacitors, resistors, or other electrical devices! We will begin with simple circuits that consist of resistors and sources of emf February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 10

11 Ohm s Law! Here a source of emf provides a potential difference V emf across a resistor with resistance R! The relationship between the potential difference and the resistance is given by Ohm s Law V emf = ir! The current in the circuit flows through the resistor, the source of emf, and the wires! The change in potential of the current in the circuit must occur in the resistor! The change is called the potential drop across the resistor February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 11

12 Ohm s Law! We can represent the previous circuit in a different way, making it clearer where the potential drop happens and showing which parts of the circuit are at which potential! On the next slide, the top part of the figure shows the previous circuit while the bottom part shows the same circuit but with the vertical dimension representing the value of the electric potential at different points around the circuit! The potential difference is supplied by the source of emf, and the entire potential drop occurs across the single resistor! Ohm s Law applies for the potential drop across the resistor February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 12

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14 Resistors in Series! Circuits can contain more than one resistor and/or more than one source of emf! The analysis of circuits with multiple resistors requires different techniques! Resistors connected such that all the current in a circuit must flow through each of the resistors are connected in series! For example, two resistors R 1 and R 2 in series with one source of emf with potential difference V emf are shown in this circuit February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 14

15 Resistors in Series! The potential drop across resistor R 1 is ΔV 1! The potential drop across resistor R 2 is ΔV 2! The potential drops must sum to the potential difference V emf = ΔV 1 + ΔV 2! The current flowing through each resistor is the same ( ) = ir eq V emf = ir 1 + ir 2 = i R 1 + R 2 R eq = R 1 + R 2! The two resistors in series can be replaced with an equivalent resistance equal to the sum of the two resistances! Generalized for n resistors in series: R eq = n R i i=1 February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 15

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17 Internal Resistance of a Battery! When a battery is not connected in a circuit, the voltage across its terminals is V t! When the battery is connected in series with a resistor with resistance R, current i flows through the circuit! When current is flowing, the potential difference, V emf, across the terminals of the battery is less than V t! This drop occurs because the battery has an internal resistance R i that can be thought of as being in series with the external resistor ( ) V t = ir eq = i R + R i! The battery terminals are points A and B February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 18

18 Internal Resistance of a Battery PROBLEM! Consider a battery that has V t = 12.0 V when it is not connected to a circuit! When a 10.0 Ω resistor is connected with the battery, the potential difference across the battery s terminals drops to 10.9 V! What is the internal resistance of the battery? SOLUTION! The current flowing through the external resistor is i = ΔV R = 10.9 V 10.0 Ω = 1.09 A February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 19

19 Internal Resistance of a Battery! The current flowing through the complete circuit must be the same as the current flowing through the external resistor V t = ir eq = i R + R i R + R i ( ) = V t i ( ) R i = V t i R = 12.0 V 1.09 A 10.0 Ω = 1.0 Ω! The internal resistance of the battery is 1.0 Ω! You cannot determine if a battery is still functional by simply measuring the potential difference across the terminals! You must connect a resistance across the terminals and then measure the potential difference February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 20

20 Resistors in Parallel! Instead of being connected in series so that all the current must pass through both resistors, two resistors can be connected in parallel, which divides the current between them! The potential drop across each resistor is equal to the potential difference provided by the source of emf! We can better visualize the potential drops, we can look at the same circuit in 3D February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 22

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22 Resistors in Parallel! The voltage drop across each resistor is equal to the potential difference provided by the source of emf! Using Ohm s Law we can write the current in each resistor i 1 = V emf R 1 i 2 = V emf R 2! The total current in the circuit must equal the sum of these currents i = i 1 + i 2! Which we can rewrite as i = i 1 + i 2 = V emf R 1 + V emf 1 = V emf + 1 R 2 R 1 R 2 February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 24

23 Resistors in Parallel! We can then rewrite Ohm s Law for the complete circuit as i = V emf 1 R eq!.. where 1 R eq = 1 R R 2! We can generalize this result for two parallel resistors to n parallel resistors 1 R eq = n i=1 1 R i February 12, 2014 Physics for Scientists & Engineers 2, Chapter 25 25

Physics for Scientists & Engineers 2

Review The resistance R of a device is given by Physics for Scientists & Engineers 2 Spring Semester 2005 Lecture 8 R =! L A ρ is resistivity of the material from which the device is constructed L is the