Magnetic fields and magnetic forces • Han Christian Oersted/André Ampere – discovered the relationship between moving charges and magnetism • Michael Faraday/Joseph Henry – discovered that moving a magnet near a conducting loop can cause a current in the loop • Magnetic fields are produced by electric currents. • The Lorentz force: F=qvxB • SI unit: Testa (T) • If the charge is moving in a region where E and B fields are present: Magnetic field sources http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html The magnetic field lines around a long wire The magnetic field lines of a current loop http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Soleniod Bar magnet http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html The bar magnet The earth http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html The bar magnet and the earth http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html http://www.timed.jhuapl.edu/WWW/science/objectives.php Imager of Sprites and Upper Atmospheric Lightning (ISUAL) Imager of Sprites and Upper Atmospheric Lightning (ISUAL) The Lorentz force http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Magnetic force on moving charge http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Mass spectrometer http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html e/m experiment http://physics.csustan.edu/GENERAL/Ian/GeneralPhysicsIIlabs/EoverM/movies/Path.htm Magnetic force on a currentcarrying wire http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html What is generated in the wire? http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Magnetic flux • Magnetic flux is the product of the average magnetic field and the perpendicular area that it penetrates. B dA d B dA Magnetic flux density http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Gauss’ law of magnetism The net magnetic flux out of any closed surface is zero. What is the physical significance of this statement? Units: 1. Magnetic field B: 1T=1Ns/Cm 2. Magnetic flux : 1W=1Tm2 Motion of a charged particles in a magnetic field • Two positive ions having the same charge q, but different masses m1 and m2, are accelerated from rest through a potential difference V. They then enter a region where there is a uniform magnetic field B normal to the plane of the trajectory. Show that if the beam entered the magnetic field along the x-axis, the value of the ycoordinate for each ion at any time t is approximately q y Bx 8mV 2 1 2 provided y is remains much smaller than x. • Can this be used for isotope separation? Magnetic force on a currentcarrying conductor The force on all of the moving charges: F nAl qvd B nqvd AlB but J nqvd F IlB In general F Il B dF Idl B differential form A l vd An electromagnetic rail gun • A conducting bar with mass m and length L slides over a horizontal rails that are connected to a voltage source. The voltage source maintains a constant current I in the rails and bar; and a constant, uniform, vertical magnetic field B fills the region between the rails. – Find the magnitude and direction of the net force on the conducting bar. Ignore friction, air resistance and electrical resistance. – If the bar has a mass m, find the distance d that the bar must move along the rails from rest to attain speed v. – It has been suggested that rail guns based on this principle could accelerate payloads into earth orbit or beyond. Find the distance the bar must travel along the rails if it is to reach the escape speed for the earth. Let B=0.5T, I=2000A, m=25kg and L=0.5m. I B Force and torque on a current loop http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Hall effect http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html The magnetic dipole moment (magnetic moment) IA Torque τ μB Where is the direction of the solenoid’s tendency of rotation? I B http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Sources of magnetic field • The magnetic field produced by a moving charge is proportional to the – charge – velocity of the charge – inverse of the square of the distance 0 q v sin B 4 r2 0 qv rˆ B 4 r 2 0 4 10 7 TmA1 (permeability constant) fr q v s i o e u rl d c p e o p i o in t n Magnetic field of a current element dQ nqAdl 0 n q vd Adl sin dB 4 r2 0 Idl sin dB 4 r2 0 Idl rˆ dB 4 r 2 0 Idl rˆ B 4 r 2 source point dl I r̂ field point r dB Biot-Savart law • For an infinitely long straight wire, the magnetic field at a distance x from the wire is given by 0 I B 2x • Ampere’s law B dl I 0 Force between parallel conductors 0 I B 2r 0 II ' l F I ' lB 2r F 0 II ' l 2r r x x I’ I B One ampere is that unvarying current that, if present in each of tow parallel conductors of infinite length and one meter apart in empty space, causes each conductor to experience a force of exactly 2x10-7 Nm-1. Magnetic field of a circular current loop z dl r̂ I dBy dBz dBy x 0 Idl rˆ dB 4 r 2 Let a be the radius of the ring. dB 0 I dl 4 x 2 a 2 2 y 0 I dl sin 2 2 4 x a 0 I dl dBz cos 4 x 2 a 2 I 1 a By 0 4 x 2 a 2 2 2 By 0 Ia 2 2x a 2 x a 1 2 dl 3 2 2 What is B at the center of the ring? If there are N rings, what is B at the center of the rings? The magnetic field at a distance r from a conductor has a magnitude I B . B dl . dl B 0 2r 0 I B dl Bdl B dl 2r 2r 0 I B dl B 1dl B dl I 0 B dl 0 I d 4 c r2 1 .r 3 1 b c d a b c B dl B dl B dl a B dl B dl d b 2 a b c a b b c a b B dl 0dl B dl 0dl d a c d d a c d B3dl 0dl B1dl B3dl 0dl B1dl 0 I 0 I B dl 2r1 2r1 2r2 2r2 0 Take note: Even though there is a magnetic field everywhere along the integration path, the line integral is zero if there is no current passing through the area bounded by the path. Ampere’s law . B dl 0 I enclosed x . x . path of integration x x Curl your fingers of your right hand around the integration path so that they curl in the direction of integration. Then your right thumb indicates the positive current direction. Applications of Ampere’s law A long, straight, solid cylinder, oriented with its axis in the z-direction, carries a current whose current density is J. The current density, although symmetrical about the cylinder axis, is not constant but varies according to the relation 2 2I 0 J 2 a J0 r 1 a kˆ for ra for ra where a is the radius of the cylinder, r is the radial distance from the cylinder axis, and Io is a constant having units of amperes. a) Show that Iois the total current passing through the entire cross section the wire. b) Using Ampere’s law, derive an expression for the magnitude of the magnetic field B in the region ra. c) Obtain and expression for the current I contained in the circular cross section of radius ra and centered at the cylinder axis. d) Using Ampere’s law, derive an expression for the magnitude of the magnetic field B in the region ra. Applications of Ampere’s law The figure below shows an end view of two long, parallel wires perpendicular to the xy-plane, each carrying a current I but in opposite direction. Derive the expression for the magnitude of B at any point on the x-axis. . a P x a x Applications of Ampere’s law A circular loop has radius R and carries current I2 in a clockwise direction. The center of the loop is a distance D above a long, straight wire. What are the magnitude and direction of the current I1 in the wire if the magnetic field at the center of the loop is zero? R I2 D I1 Study the examples in the book! Field inside a long cylindrical conductor B R r I B Amperian loop B dl I 0 enclosed r2 B2r 0 I 2 R B 0 I r 2 R 2 R r Field of a solenoid Let n be the number of turns. B dl I 0 enclosed BL 0 nLI B 0 nI Find the magnetic field of a toroidal solenoid. http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Magnetic materials But I e L IA e ev I T 2r ev evr 2 r 2r 2 L r mv L mvr e L 2m The dipole moment’s component in a particular direction is an integral multiple of h 2 h 6.626 1034 Js When we speak of the magnitude of a magnetic moment, we mean the “maximum component in a given direction”. aligned with B means that has its maximum possible component in the direction of B. The Bohr magneton If L h 2 eh 9.274 10 24 Am 2 4m Magnetization M μ I i i V Paramagnetism The magnetization of the material is proportional to the applied magnetic field in which the material is placed. B B 0 μ 0M Curie’s law B M C T Mmagnetization CCurie’s constant Ttemperature (K) Bmagnetic field For a given ferromagnetic material the long range order abruptly disappears at a certain temperature called the Curie temperature. The relative permeability: K m 0 For common paramagnetic materials, Km varies from 1.00001 to 1.003. The magnetic susceptibility: m Km 1 The magnetic susceptibility is the amount by which the relative permeability differs from unity. Material Curie temperature (K) Fe 1043 Co 1388 Ni 627 Gd 293 Dy 85 CrBr3 37 Au2MnAl 200 Cu2MnAl 630 Cu2MnIn 500 EuO 77 EuS 16.5 MnAs 318 MnBi 670 GdCl3 2.2 Fe2B 1015 MnB 578 Data from F. Keffer, Handbuch der Physik, 18, pt. 2, New York: Springer-Verlag, 1966 and P. Heller, Rep. Progr. Phys., 30, (pt II), 731 (1967) Material m Iron ammonium alum 66 Uranium 40 Platinum 26 Aluminum 2.2 Sodium 0.72 Oxygen gas 0.19 Bismuth -16.6 Mercury -2.9 Silver -2.6 Carbon (diamond) -2.1 Lead -1.8 Sodium chloride -1.4 Copper -1.0 Young &Freedman, University Physics 11th ed., p.1089 Diamagnetism The orbital motion of electrons creates tiny atomic current loops, which produce magnetic fields. When an external magnetic field is applied to a material, these current loops will tend to align in such a way as to oppose the applied field. Diamagnetism is the residual magnetic behavior when materials are neither paramagnetic nor ferromagnetic. Ferromagnetism Strong interactions between magnetic moments cause to line up parallel to each other in regions called magnetic domains. Hysteresis http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Average magnetic dipole moment per atom of iron A piece of iron has a magnetization M=6.5x104 A/m. Find the average magnetic dipole moment per atom in this piece of iron. Express your answer in Bohr magnetons and in Am2. The density of iron is 7.8x103kg/m3. The atomic mass of iron is 55.845g/mol. Electromagnetic induction • Results from experiments S N electromagnet galvanometer – When there is no current in the electromagnet, so that B=0, the galvanometer shows no current. – When the electromagnet is turned on, there is a momentary current through the meter as B increases. – When B levels off at a steady value, the current drops to zero, no matter how large B is. Electromagnetic induction • Results from experiments S N electromagnet galvanometer – With the coil in a horizontal plane, we squeeze it so as to decrease the cross sectional area of the coil. The meter detects current only during the deformation, not before or after. When we increase the area to return the coil to its original shape, there is current in the opposite direction, but only while the area of the coil is changing. Electromagnetic induction • Results from experiments S N electromagnet galvanometer – If we rotate the coil a few degrees about a horizontal axis, the meter detects a current during the rotation, in the same direction as when we decreased the area. When we rotate the coil back, there is a current in the opposite direction during this rotation. – If we jerk the coil out of the magnetic field, there is a current during the motion, in the same direction as when we decreased the area. Electromagnetic induction • Results from experiments S N electromagnet galvanometer – If we decrease the number of turns in the coil by unwinding one or more turns, there is a current during the unwinding, in the same direction as when we decreased the area. If we wind more turns onto the coil, there is a current in the opposite direction during the winding. Electromagnetic induction • Result from experiments S N electromagnet – When the magnet is turned off, there is a momentary current in the direction opposite the current when it was turned on. – The faster we carry out any of these changes, the greater is the current. – If all these experiments are repeated with a coil that has the same shape but different material and different resistance, the current in each case is inversely proportional to the total circuit resistance. galvanometer What is common in these results? Electromagnetic induction Faraday’s law: The induced emf in a closed loop equals the negative of the time rate of change of magnetic flux through the loop. d B dt B B dA Any change in the magnetic environment of a coil of wire will cause a voltage (emf) to be "induced" in the coil. No matter how the change is produced, the voltage will be generated. The change could be produced by changing the magnetic field strength, moving a magnet toward or away from the coil, moving the coil into or out of the magnetic field, rotating the coil relative to the magnet, etc. For N turns, d B N dt Direction of induced emf Increasing B A <0 Decreasing B A >0 • Define the direction of the vector area A. • From the directions of A and the magnetic field B, determine the sign of the magnetic flux B and its rate of change. • Determine the sign of the induced emf or current. If the flux is increasing, so dB/dt is positive, then the induced emf or current is negative. • If the flux is decreasing, dB/dt is negative and the induced emf or current is positive. Direction of induced emf A >0 A <0 • Determine the direction of the induced emf or current using your right hand. Curl the fingers of your right hand around the A Increasing vector, with your right thumb in B the direction of A. If the induced emf or current in the circuit is positive, it is in the Decreasing same direction as your curled B fingers. If the induced emf or current is negative, it is in the opposite direction. Faraday’s law http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Faraday’s law Lenz’s law: The direction of any magnetic induction effect is such as to oppose the cause of the effect. http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Examples Two coupled circuits, A and B, are situated as shown below. Use Lenz’s law to determine the direction of the induced current in resistor ab when (a) coil B is R brought closer to coil A with the switch closed, (b) the resistance of R is decreased while the switch remains closed, and (c) switch S is opened. An alternator is a device that generates an emf. A rectangular loop is made to rotate with a constant angular velocity w about the axis shown below. The magnetic field B is uniform and constant. At time t=0, f=0, determine the induced emf. A B S a b Examples Consider a motor with a square coil 10cm on a side with 500 turns of wire. If the magnitude of the B field is 0.2T, at what rotation speed will the average back emf of the motor be 112V? The back emf of a motor is the emf induced by changing magnetic flux through its rotating coil. A conducting disk with radius R lies in the xy-plane and rotates with constant velocity w about the z-axis. The disk is in a uniform, constant B field parallel to the z-axis. Find the induced emf between the center and the rim of the disk. Examples Consider a U-shaped conductor in a uniform Bfield. If a metal with length L is put across the arms xx of the conductor, forming a circuit, and move the xx x rod to the right with constant velocity v, find the magnitude and direction of the resulting emf. x x x x x x x x x x x x x x x x x x x x x x x x x A cardboard tube is wrapped with two windings of insulated wire wound in opposite directions. Terminals a and b of winding A may be connected to a battery through a reversing switch. Where is the direction of the induced current in the resistor R if a) the current in winding A is from a to b and is increasing? b) the current is from b to a and decreasing? c) a b Winding A the current is from b to a and increasing? Winding B v Examples A long wire carries a constant current I. A metal bar with length L is moving at constant velocity v. Calculate the emf induced in the bar? Which point is at higher potential? What is the magnitude of the induced current if the bar is replaced by a rectangular wire loop? I I v v Motional electromotive force a xxxxxxxxxxxxxxxx xI x x x x x x x x x x x x x xvx x x x x x x x x x x x xL x x x x xxxxxxxxxxxxxxxx b Motional electromotive force: vBL d v B dL v B dL This equation can be used for non-stationary conductors in changing magnetic fields. A conducting disk with radius R lies in the xy-plane and rotates with constant angular velocity w about the z-axis. The disk is in a uniform, constant B field parallel to the z-axis. Find the induced emf between the center and the rim of the disk. B Induced electric fields G I, dI/dt If the area vector A points in the same direction as B set up by the solenoid, then B BA 0 nIA d B dI 0 nA dt dt What force makes the charges move around the loop? d B E dl dt Maxwell’s equations: Qenclosed E dA B dA 0 0 d E B dl 0 ic 0 dt d B E d l dt Displacement current Displacement current: iD B dl 0 I enclosed q CV A Ed Ed E d dq d E iC dt dt Conduction current d E dt Generalized Ampere’s law: d E B d l i 0 c 0 dt Electromagnetic properties of superconductors Kammerlingh Onnes (1911) discovered superconductivity. The critical temperature for superconductors is the temperature at which the electrical resistivity of a metal drops to zero. Type 1 semiconductors: Mat. Tc Be 0 Rh 0 W 0.0 15 Ir 0.1 Lu 0.1 Hf 0.1 Ru 0.5 Os 0.7 Mo 0.9 2 Type 2 semiconductors: Ma Zr Tc 0.546 Mat. Tc Al 1.2 Cd 0.56 Pa 1.4 U 0.2 Th 1.4 Ti 0.39 Re 1.4 Zn 0.85 Tl 2.39 Ga 1.083 In 3.40 8 Sn 3.72 2 http://www.physnet.uni-hamburg.de/home/vms/reimer/htc/pt3.html The Meissner Effect “Magnetism and superconductivity are natural enemies”. - Lindenfeld Mixed-State Meissner Effect Macroscopic magnetization depends upon aligning the electron spins parallel to one another, while superconductivity depends upon pairs of electrons with their spins antiparallel. Movies: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/maglev2.html http://hyperphysics.phy-astr.gsu.edu/hbase/solids/maglev.html#c1 The Eddy currents The Eddy currents are induced currents due to masses of metal moving in magnetic fields or located in changing magnetic fields. http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html A “proper” complete circuit is not necessary for currents caused by induced emf’s to flow. Microscopic currents can flow within conductors and they are eddy currents! Some applications of that make use of eddy currents: 1. Electromagnetic damping: eddy currents flow in such a way as to oppose the motion that causes them, acting like a brake on a moving body. 2. Induction heating: current flows cause heating effects and eddy currents are no different. Transformers http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Inductance Inductance is typified by the behavior of a coil of wire in resisting any change of electric current through the coil. A changing current in a coil induces an emf in that same coil! The coil is the inductor and the relationship between the current and the emf is described by inductance (self-inductance). emf L dI dt When there are 2 or more inductors present, the coupling between the coils is described by their mutual inductance. A coil is a reactionary device, not liking any change! The induced voltage will cause a current to flow in the secondary coil which tries to maintain the magnetic field which was there. http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Mutual inductance The induced emf in coil 1 is due to self inductance L. The induced emf in coil 2 is caused by the change in the current I1: 2 emf2 N 2 t Define: N2 B 2 M 21i1 B1 i M 21 1 t t d 2 di N2 M 21 1 dt dt M 21 N 2 B 2 i1 emf 2 N 2 A Show that M12=M21. Unit of inductance: 1H=1Wb/A=1J/A2 B field from coil 1 passing through coil 2 Self-inductance and Consider a single isolatedinductors coil. When a varying current is present in a circuit, it sets up a changing magnetic field that causes a changing magnetic flux through the same circuit. The resulting emf is called a self-induced emf. An inductor (or a choke) is a devise that opposes any current variations throughout the circuit and is designed to have a particular inductance. Inductor: Define: L N B i Self induced emf: (Self inductance) L di dt http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html A general purpose RF chokes suitable for power decoupling in logic circuits, IF tuned circuit applications and filters etc. Offers high resonance frequency; suitable for RF blocking and filtering, interference suppression in small size equipment, decoupling and telecoms and entertainment electronics RF chokes consisting of a ferrite based coil former encapsulated in a polypropylene outer case. Wire ended toroidal RFI suppression chokes designed for use with phase angle control equipment applications operating at 240V ac. http://www.rsphilippines.com/ Magnetic field di P V i energy Li a ab Variable source of emf L dt Pdt dU Lidi 1 b U Li 2 2 What is the potential difference between points a and b? Does energy flow into a resistor whenever a steady current passes through it? Does energy flow into a resistor whenever a varying current passes through it? Does energy flow into an ideal zero-resistance inductor when a steady current through it? Does energy flow into an ideal zero-resistance inductor when an increasing current passes through it? Explain what happens to the bulb when the switch is closed. Show that the self-inductance of an ideal toroidal solenoid of mean radius r and crosssectional area A is: 0 N 2 A L 2r Show that the energy density of an ideal toroidal solenoid is U 1 N 2i 2 u 0 2rA 2 2r 2 The RL circuit Show that for an ideal toroidal solenoid B2 u 20 B2 u 2 (magnetic energy density in a vacuum) (magnetic energy density in a material) In steady state condition, what is the potential difference between the ends of the inductor? The magnetic field H is defined as B H 0 Again, an inductor in a circuit makes it difficult for rapid changes in current to occur! Suppose that the switch is initially open, but is suddenly closed at t=0. di V iR L dt http://farside.ph.utexas.edu/teaching/302l/lectures/node88.html t R di ' 0 V 0 L dt ' i ' R i R t V i 1 e L R The time constant for an RL circuit is L/R. V iR L di 0 dt The current in a coil can not increase (or decrease) much faster than L/R. What is the rate of change of the current at t=0? What is the current at the steady state condition? V iR L di 0 dt di R dt V L i R Note that Vs/R=I0 Current decay in an RL circuit iR L i I 0e di 0 dt R t L http://farside.ph.utexas.edu/teaching/302l/lectures/node88.html i 2 R Li Vs/R=I0 di 0 dt When an RL circuit is decaying, what is the expression of the energy stored in the inductor as a function of time? Suppose you want to send a square wave down a wire. How does the output signal look like? The LC circuit In terms of energy considerations, Vi i 2 R Li di 0 dt Consider a charged capacitor that is connected to an inductor. Assume no resistance and no energy losses to radiation. What happens to the current in the circuit? http://www.sweethaven.com/sweethaven/ModElec/acee/lessonMain.asp?iNum=0402 Kirchoff’s voltage law: L di q 0 dt C d 2q 1 q0 dt 2 LC What is the current in the circuit? What is the stored potential energy in the capacitor? What is the stored potential energy in the inductor? A solution to the 2nd order differential equation is: q Q coswt f The current is i wQ sin wt f What is the physical significance of the proposed solution? Are there any possible solutions? What are they? Can you consider an LC circuit as a conservative system? http://www.greenandwhite.net/~chbut/LC_Oscillator/LC_Oscillator.swf In terms of energy considerations, 2 2 1 2 q Q Li 2 2C 2C 1 i Q2 q2 Lc The RLC circuit Similarities between SHM and LC circuit 1 1 2 KE mv 2 ME Li 2 22 1 2 1 q PE kx EE 2 2C 2 2 1 2 1 2 1 2 1 1 q 1 Q 2 mv kx kA Li 2 2 2 2 2C 2 C v dx k A2 x 2 dt m k w m x A coswt f i w dq 1 Q2 q2 dt Lc 1 LC q Q coswt f Kirchoff’s voltage law: di q 0 dt C di 1 t iR L idt ' 0 dt C 0 d 2 q R dq 1 q0 2 dt L dt LC iR L Auxiliary equation: m2 R 1 m 0 L LC 2 R 1 R 1 m 4 2L 2 L LC 2 2 R 1 R 1 m1 4 2L 2 L LC R 1 R 1 m2 4 2L 2 L LC General solution: 2 q Ae R t R 1 t 4 2L 2 L LC 2 Be R t R 1 t 4 2L 2 L LC When R2<<4/LC, (underdamped case), 2 R ti 1 R R t ti 4 1 R 2 t 4 2 L 2 LC L 2 L 2 LC L q Re Ae Be 2 ti 1 R R t ti 4 1 R 2 R 4 t q Re Ae 2 L e 2 LC L Be 2 L e 2 LC L ei cos i sin Euler’s equation: i e t 1 R 4 2 LC L 2 2 2 t t 1 R 1 R cos 4 i sin 4 2 LC L 2 LC L 2 t 1 R q Ae cos 4 f 2 LC L R 2 t 1 R 2L q Ae cos t 2 f w LC 4 L R t 2L 2 q Ae R t R 1 t 4 2L 2 L LC 2 1 R2 2 LC 4 L 2 Be R t R 1 t 4 2L 2 L LC R 1 4 0 Overdamped: L 2 LC R 1 Critical damping: 4 0 L LC 2 R 1 4 0 Underdamped: L LC Overdamped Critically damped Underdamped Alternating current Symbol: ~ Phasors are rotating vectors. Rectified average value of a sinusoidal current: I rav I wt i I coswt How do we measure sinusoidally varying current? 2 I max Root-mean-square current: -Square the instantaneous current -Take the average of the sum of the squares -Take the square root i I coswt i 2 I 2 cos 2 wt But 1 cos 2 wt 1 cos 2wt 2 1 i 2 I 2 cos 2wt 2 http://www.allaboutcircuits.com/vol_3/chpt_3/4.html cos 2wt 0 I I rms 2 Note that I is the maximum current! Vrms Phasor diagram: V 2 The normal voltage source from local outlets is 220VAC. Is this Vrms? The current and voltage are in phase! What are the maximum and minimum voltages that a TV can have if it is rated at 110VAC? 110VDC? Resistance and reactance I sin wt Inductor in an AC circuit: Resistor in an AC circuit: http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html I sin wt Phasor diagram: Note: The phase of the voltage is defined relative to the current! For a pure resistor, the phase is 0. For a pure inductor, the phase is 90o. di dt d V L I sin wt dt V IwL cos wt L V IwL sin wt 90 The inductive reactance is defined as X L wL The voltage difference between the inductor: o V IX L Capacitor in an AC circuit: The voltage leads the current by 90o in phase! http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html I sin wt The capacitive reactance is defined as 1 XC wC dq I sin wt dt i q I w The voltage difference between the capacitor: cos wt V q I cos wt C Cw V I sin wt 90 o Cw Phasor diagram: V IX C XL R XC The voltage lags the current by 90o in phase! http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Mnemonic for the phase relations of current and voltage: ELI the ICE man! VL IX L VL IX L VR IX R VR IX R VL VC VC IX C VC IX C V VR2 VL VC VR IZ VL VC f 2 VR IX R V I R2 X L X C 2 Define: Z R2 X L X C 2 (Impedance) The impedance is the ratio of the voltage amplitude across the circuit to the current amplitude in the circuit. For an RLC circuit: 1 Z R 2 wL w C 2 The angle f is the phase angle of the source with respect to the current. tan f VL VC VR 1 wC R wL At resonance, the phase becomes 0! Thus, 0 tan w 1 wC R wL 1 LC http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html The power factor: cos f For any sinusoidally varying quantity, the rms value is always 0.707 times the amplitude: V I Z 2 2 Vrms I rms Z Power in AC circuits The instantaneous power delivered to a circuit element is A low power factor (large angle f of lag or lead) means that for a given potential difference, a large current is needed to supply a given amount of power. -high I2R losses in transmission -To correct: connect a capacitor in parallel with the load. WHY? Transformers: p vi p V coswt f I coswt p VI cos f cos 2 wt VI sin f cos wt sin wt 1 Pave VI cos f 2 Pave Vrms I rms cos f http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html Derive and expression for Vout/Vin as a function of the angular frequency w of the source. In an LRC series circuit, the magnitude of the phase angle is 54o, with the source voltage lagging the current. The reactance of the capacitor is 350W and the resistor resistance is 180W. The average power delivered by the source is 140W. Find the reactance of the inductor, the rms current and the rms voltage. Derive and expression for Vout/Vin as a function of the angular frequency w of the source. C ~ R Vout L In the circuit shown below, switch S is closed at time t=0. Find the reading of each meter just after S is closed. What does each meter read long after S is closed? 40W S 5W 10W C ~ 15W 25V 20mH 10mH A1 A2 A3 L R Vout A4 Electromagnetic waves Maxwell’s equations: Qenclosed E dA 0 B dA 0 d E B dl 0 ic 0 dt d B E dl dt Speed of light ≡ 299,792,458 m/s http://hyperphysics.phy-astr.gsu.edu/hbase/hframe.html