Current & Resistance - Current and current density - Ohm’s Law - Resistivity - Resistance.

Slides:



Advertisements
Similar presentations
Electricity and Magnetism
Advertisements

Chapter 27 Current And Resistance Electric Current Electric current is the rate of flow of charge through some region of space The SI unit of current.
CH 20-1.
Current and Resistance FCI.  Define the current.  Understand the microscopic description of current.  Discuss the rat at which the power.
Current and Resistance
PHY 2054: Physics II. Calculate the Electric Field at P Calculate the el. potential at P.
UNIT 9 Electrostatics and Currents 1. Thursday March 22 nd 2 Electrostatics and Currents.
Chapter 17 Current and Resistance. Electric Current Let us look at the charges flowing perpendicularly to a surface of area A The electric current is.
Electric Current Whenever electric charges of like signs move, an electric current is said to exist The current is the rate at which the charge flows through.
15/20/2015 General Physics (PHY 2140) Lecture 6  Electrostatics and electrodynamics Capacitance and capacitors capacitors with dielectrics Electric current.
Physics 1402: Lecture 8 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
Current and Resistance
Physics for Scientists and Engineers II, Summer Semester Lecture 8: June 8 th 2009 Physics for Scientists and Engineers II.
1 Chapter 27 Current and Resistance. 2 Electric Current Electric current is the rate of flow of charge through some region of space The SI unit of current.
Current, Resistance, and Electromotive Force
Unit 3, Day 4: Microscopic View of Electric Current Current Density Drift Velocity Speed of an Electron in as Wire Electric Field inside a Current Carrying.
Current and Resistance. Current In our previous discussion all of the charges that were encountered were stationary, not moving. If the charges have a.
Electric (conduction) current I I According to general agreement its direction is chosen to coincide with the direction in which positive.
Today’s agenda: Electric Current. You must know the definition of current, and be able to use it in solving problems. Current Density. You must understand.
Electric Current, Ohm’s Law, and Electric Circuits ISAT 241 Fall 2002 David J. Lawrence.
Electric Current 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 The.
-Electric Current -Resistance -Factors that affect resistance -Microscopic View of Current AP Physics C Mrs. Coyle.
Chapter 24 Electric Current. The electric current I is the rate of flow of charge through some region of space The SI unit of current is Ampere (A): 1.
Current and Direct Current Circuits
Chapter 27 Current Resistance And Resistor. Review The current is defined and its unit is ampere (A), a base unit in the SI system I A The.
1 Electric Current Electric field exerts forces on charges inside it; Charges move under the influence of an electric field. The amount of charge moves.
Chapter 17 Current and Resistance. Electric Current Let us look at the charges flowing perpendicularly to a surface of area A The electric current is.
Copyright © 2009 Pearson Education, Inc. Lecture 6: Electric Currents & Resistance.
 I1I1   R R R I2I2 I3I3 Lecture 11 Current & Resistance.
Electric Current and Resistance Unit 16. Electric Current  The current is the rate at which the charge flows through a surface Look at the charges flowing.
Chapter 27 Current and Resistance. Intro Up until now, our study of electricity has been focused Electrostatics (charges at equilibrium conditions). We.
Current and Resistance
Chapter 17 Current and Resistance. General Physics Current, Resistance, and Power Ch 17, Secs. 1–4, 6–7 (skip Sec. 5)
Current � and � Resistance Electric Current Resistance and Ohm’s Law A Model for Electrical Conduction Resistance and Temperature Superconductor Electrical.
Current Electricity Parallel CircuitSeries Circuit.
Current of Electricity Electric Current Potential Difference Resistance and Resistivity Electromotive Force.
Current and Resistance FCI.  Define the current.  Understand the microscopic description of current.  Discuss the rat at which the power.
Chapter 27 Current and Resistance. Electric Current The electric current I is the rate of flow of charge through some region of space The SI unit of current.
Chapter 17 Current and Resistance. Electric Current Whenever electric charges of like signs move, an electric current is said to exist The current is.
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.
Current and Resistance
Current and Resistance FCI.  Define the current.  Understand the microscopic description of current.  Discuss the rat at which the power.
Chapter 26 Lecture 21: Current: I. Types of Capacitors – Variable Variable capacitors consist of two interwoven sets of metallic plates One plate is fixed.
Chapter 27: Current and Resistance Fig 27-CO, p Electric Current 27.2 Resistance and Ohm’s Law 27.4 Resistance and Temperature 27.6 Electrical.
Electric Charge Atomic ParticleChargeMass Electron –1.6  C9.11  Kg Proton +1.6  C1.673  Kg Neutron  Kg Atomic.
Dr. Jie ZouPHY Chapter 27 Current and Resistance.
Chapter 27 Current Resistance And Resistor. Review The current is defined and its unit is ampere (A), a base unit in the SI system I A The.
Physics Section 17.3 Apply the properties of electric current Electric current is the rate at which charge flows through a conductor. The charges can be.
Chapter 27 Current And Resistance. Electric Current Electric current is the rate of flow of charge through some region of space The SI unit of current.
Electric Current Chapter 27 Electric Current Current Density Resistivity – Conductivity - Resistance Ohm’s Law (microscopic and macroscopic) Power Dissipated.
-Electric Current -Resistance -Factors that affect resistance -Microscopic View of Current AP Physics C Mrs. Coyle.
General Physics 2Current & Resistance1 E5 - Current So far we’ve looked at stationary charges – electrostatics Now we’re ready for moving charges!!!
PHYS219 Fall semester 2014 Lecture 07: Current Flow Dimitrios Giannios Purdue University.
Current and Resistance
Current and Resistance
Announcements Chapter 17 covers current and resistance
Stuff Ya Gotta Know: Current and Resistance Current and Resistance
A Little Capacitance and Current and Resistance
Chapter 24 Electric Current.
Current and Resistance
Announcements Prof. Reitze will be giving this week’s lectures on Ch. 17 Chapter 17 covers current and resistance WebAssign HW Set 4 due this Friday Problems.
General Physics (PHY 2140) Lecture 7
Physics 122B Electricity and Magnetism
Ch 17 Electrical Energy and Current
Microscopic Model of Conduction
Effects of moving charges
Current and Resistance
Current and Resistance
Current and Resistance
Presentation transcript:

Current & Resistance - Current and current density - Ohm’s Law - Resistivity - Resistance

Electrical Current CURRENT I is the amount of positive charge flowing past a fixed point in the wire per unit time : if charge dQ flows in time dt Units: 1 ampere (A) = 1 C/s Direction: by convention, current is the direction of movement of positive charge I I

Electron Velocities Random velocities of electrons are large (several km/s) Drift velocity is a slow, average motion parallel to E start end start end net displacement + E no field

Charge ΔQ in length L of wire passes through the shaded disk of area A in time Δ t : ΔQ = (number of charge carriers/volume) x (charge on each one) x volume L = v d  t E Determining the current

Current: I =  Q/  t = nqAv d  t /  t So,  Charge:  Q = n q V = n q (AL) = n q A v d  t (since L=vt) I = nqAv d v d = average (“drift”) velocity of each charge q = charge on each particle n = number of charge carriers per unit volume A = cross section area L = length AL = volume

Example Take Area = 1 mm 2, assume I = 1 A The mobile charges in most metals are electrons, with about one or two electrons per atom being free to move. So there are about charges per cm 3 (or m -3 ). Which way are the electrons moving?

E = 0 inside ? Note: in electrostatics, we had E=0 inside a conductor, if not, charges would move, the conductor would not be in equilibrium and there would be a current. For a wire to carry a current, we must have an electric field inside the conductor, which is caused by the potential difference between the ends of the wire. This is no longer electrostatics!

Example A copper wire of cross sectional area 3x10 -6 m 2 carries a current of 10A. Find the drift velocity of the electrons in this wire. Copper has a density of 8.95g/cm 3, and atomic weight of 63.5g/mole. Avagadro’s number is 6.02x10 23 atoms. Assume each atom contributes one free electron.

Questions When you turn on a flashlight, how long does it take for the electrons from the battery to reach the bulb? What happens to the wire as the electrons go through it? If you double the electric field in the wire, does the acceleration of the electrons double? If the electric field remains constant, how do the electron kinetic energies change with time?

Current Density J Where  is a constant called the conductivity of the material. The current density J and the electric field E are both established in a conductor as a result of a potential difference across the conductor. The current density is defined as the current per unit area in a conductor, where A is the cross section of conductor. The current density is a vector quantity, units: Amps/m 2. And since I=nqAv d ;

L Uniform E “Resistance”, R Because J is proportional to the field, current in a wire is proportional to the potential difference between the ends of the wire. A E

RESISTIVITY: the inverse of conductivity. where (Uniform wire, Length L, cross-section area A) (this depends on the type of material) Unit of resistance R is: Ohm’s Law

Current density  field: J =  E Current  potential difference: V = IR units,  = “conductivity”  = “resistivity”, has units of  m

ρ (20°C) (Ω·m) Cu1.7 x Al2.8 x Graphite3500 x Si640 Quartz~ Resistivities of a few materials

Example A copper wire, 2 mm in diameter and 30 m in length, has a current of 5A. Find: a) resistance b) potential difference between the ends c) electric field d) current density

Quiz The wire in the previous example is replaced with a wire of the same length and half the diameter, carrying the same current. By what factor will each of the following change? A)resistance B)potential difference between the ends C)electric field D)electron number density E)electron drift speed F)current density

Summary Current Density: Conductivity: Resistivity: Resistance: Ohm’s Law: