PHYS 272: Electric and Magnetic Interactions Electric Fields and Circuits Jonathan Nistor Tuesday, July 12th, 2011 Jonathan Nistor (Purdue University) Lecture 16 7/12/2011 1 / 12 Lecture 16 Electric Field and Circuits 19.1 Introduction and Overview 19.2 Current throughout a circuit 19.3 Electric Field and Current 19.4 What charges make the E-field in the wires Jonathan Nistor (Purdue University) Lecture 16 7/12/2011 2 / 12 Lecture 16 Overview – Electron and Conventional Currents Recall that the electron current, i , is defined as the number of electrons per second that enter a section of a conductor For a metal with a cross sectional area A, and density of mobile electrons, n, then: (1) where is the mean (average) drift speed of the electrons Conventional current, , is define as the number of coulombs of charge entering a region per second. Therefore, (2) Conventional current is assumed to consist of positive charges Moving, and therefore flows in the direction of Enet Jonathan Nistor (Purdue University) Lecture 16 7/12/2011 3 / 12 Lecture 16 Overview – Equilibrium and Steady-State A metal is in Equilibium when there is no current flow: i.e. No charges are moving. Does Enet necessarily have to be zero? A conductor is in a steady state if charges are moving, but their drift velocities at any location do not change with time. Furthermore, there is no change in the deposits of excess charge anywhere For a conductor in a steady state, the drift velocities of charges may be different at different locations: Jonathan Nistor (Purdue University) Lecture 16 7/12/2011 4 / 12 Lecture 16 The Current Node Rule Conservation of charge is a fundamental physical principle which guarantees that the total net charge in a system in conserved (constant) i1 = i 2 i2 = i3 + i 4 As such, if a conductor is in the steady state, where no excess deposits of charge occur, then the amount of charge entering a particular region (node), must be equal to the amount of charge leaving that same region in the same amount of time. Written as the current node rule (Kirchhoff 1st Law) In the steady state, the electron current entering a node in a circuit is equal to the electron current leaving that node Jonathan Nistor (Purdue University) Lecture 16 7/12/2011 5 / 12 Lecture 16 Current Node Rule: Example Write the node equation for this circuit. What is the value of I2? I1 + I 4 = I 2 + I 3 I2 = I1 + I4 - I3 = 3A Write the node equations for this circuit? Jonathan Nistor (Purdue University) Lecture 16 7/12/2011 6 / 12 Lecture 16 Electric Field and Current In a current-carrying wire, there must be an electric field to drive the sea of mobile charges What is the relationship between current and the electric field? Why is an electric field require to maintain a flow of charge (current)? i.e. Once current is flowing, why is an electric force required to keep the electrons moving at a constant drift speed ? Do the electrons push each other? Can there be excess charges inside a conductor in the steady state? We already know that there cannot be excess charges inside a conductor in equilibrium! What charges produce the electric field inside the wire? Jonathan Nistor (Purdue University) Lecture 16 7/12/2011 7 / 12 Lecture 16 The Drude Model What is the relationship between current and the electric field? Why is an electric field require to maintain a flow of charge (current)? E Start From the Momentum Principle: p Fnet t The speed of the electron is: The average ‘drift’ speed is: v Jonathan Nistor (Purdue University) p eE t v p me eE t me Lecture 16 p 0 eE t me eE t where t is the average time between collisions 7/12/2011 8 / 12 Lecture 16 Typical E-Field in a wire Drift speed in a copper wire in a typical circuit is 5.10-5 m/s. The mobility of copper is u=4.5.10-3 (m/s)/(N/C). Calculate E. E v u 5 10 5 m/s 4.5 10 3 (m/s)/(N/C) 1.1 10 2 N/C Electric field in a wire in a typical circuit is very small Jonathan Nistor (Purdue University) Lecture 16 7/12/2011 10 / 12 Lecture 16 Electric Field and Drift Speed In steady state current is the same everywhere in a series circuit. Ethick Ethin i i What is the relationship between the drift speeds in the thin and thick wires? i nAv nAthinvthin nAthickvthick Athick vthick Athin vthin Note: density of electrons n cannot change if same metal What about E? v uE uEthin Jonathan Nistor (Purdue University) Athick uEthick Athin Lecture 16 Ethin Athick Ethick Athin 7/12/2011 11 / 12 Lecture 16 Direction of Electric Field in a Wire E must be parallel to the wire, why? E is the same along the wire, how do we know this? Is E uniform across the wire? C D A E1 dl E3 dl E2 dl E3 dl A B C D VAB VCD 0 0 E1 E2 B VABCDA Jonathan Nistor (Purdue University) Lecture 16 0 7/12/2011 12 / 12