Physics 116. Oct 18, Lecture 12 Electromagnetic waves. R. J. Wilkes

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Physics 116 Lecture 12 Electromagnetic waves Oct 18, 2011 R. J. Wilkes Email: ph116@u.washington.edu

Announcements Exam 1 scores will be posted on WebAssign today Will also appear on Catalyst Gradebook tomorrow Each item was worth 6 points, 15*6=90, so I added 10 to make 100 max possible So, everyone who took the exam got 10 pts just for showing up! Exam statistics: 70.6 avg 12.8 std dev 70 median 94 max 46 min

Lecture Schedule (up to exam 2) Today 3

3.6 m/s

Electromagnetic waves Discoveries about electric and magnetic fields:! H. Ørsted (1820) found electric currents deflected compasses Electric current makes magnetic field: E and B fields are related! M. Faraday (1840) found changing B fields create currents Electric generator! Legislator: What use is this toy, sir?, Faraday: Why, sir, you will soon find a reason to put a tax upon it!! J. Maxwell (1865): unified electricity and magnetism (Maxwell s eqns) Included assumption that changing E field also makes a B field! H. Hertz (1888): first observed E-M waves (radio waves!) Spark in loop of wire produced spark across the room in another G. Marconi (c1900): radiotelegraphy ( spark transmitters ) If you make a time-varying E field, it automatically makes its own time-varying B field (and vice-versa) as described by Maxwell s equations 10

Recall PHYS 115 You learned some background material for this topic last term: Faraday s Law: induced emf around a coil is proportional to rate of change of magnetic flux flux! = BiA B= magnetic field (tesla), A = area of coil, m 2 E (volts) = " #! #t (the minus sign is Lenz's contribution)! Flow of charge (current induced by emf) implies an E field is created by changing B Lenz s Law: the induced emf creates a current that produces a new B field opposing the change in magnetic flux Rather confusing without Maxwell s equations! Which every physics student should at least see once! 11

Cultural supplement not on tests Maxwell s equations: connecting B and E Electric current I makes a magnetic field B, with field lines around the wire! If charges move back and forth (oscillating current ), we get time-varying magnetic fields! Magnetic fields are perpendicular to the electric current direction (field lines are rings around the current) Time varying B fields produce time-varying E fields Maxwell s equations (1865) tell us how they are related: B I Cultural supplement : These symbols represent operations in calculus ( partial derivatives ) which find the rate of change of fields with respect to position and time. (They mean: only B changes) For example, this equation tells us a magnetic field can be produced by either an electric current, OR a changing E field.! 0 and " 0 can be determined by measuring electric and magnetic forces. Maxwell found they were related to c, the speed of light! 12

Facts we already know about EM waves Light waves are a variety of EM wave Light waves propagate through a vacuum (beeper + light demo)! No material medium is required for light to propagate The speed of light is huge, in human terms: ~ 300,000,000 m/s EM waves are produced by changing E or B fields Changing E or B fields are created by accelerated charges (changing currents) We can use changing currents to make radio waves! Example: push charge into and out of a dipole antenna! This produces E fields parallel to the dipole and B fields perpendicular to it B E ~ I 13

E-M wave (from a charge oscillating at center) See this website for many interesting movies illustrating things we have talked about 14

Recall from last week: Doppler effect: If sound source and observer are in relative motion, observed frequency will differ from source s frequency Sound waves require a material medium to propagate Recall: Galilean relativity! If two coordinate systems differ only by a constant v, not by an acceleration, we can simply add velocity vectors to get apparent v in either! Standard example: rowboat in a river that is flowing with speed v rower has speed u relative to water, water has speed v relative to earth, so rower s speed relative to earth is u + v u is + if same direction as river (rowing downstream), negative if opposite (upstream) Coordinate system of medium (air, water, etc) is special for sound waves! Sound waves have speed c, and f and! are related by For an observer moving relative to medium with speed u, apparent propagation speed c will be different:! Wavelength cannot change it s a constant length in the medium, and same length in moving coordinate system (motion does not change lengths) (sign depends on relative direction of u )! Observed frequency has to change, to match apparent speed and fixed wavelength: 15

Doppler effect: So if observer is moving (speed u) relative to source at rest in medium, then apparent frequency f is: + sign if u is toward source, Minus sign if away from source However, if source is moving (speed u) relative to observer at rest in medium, then! Frequency remains constant (same time interval between wavefront emissions)! But source now chases its own waves (or runs away from them): wavelength in the medium is shorter or longer Wave speed = c Time between successive peaks = T Distance between peaks = ct ut = wavelength Frequency of wave in medium (and for observer): Notice the central role of the medium in both cases minus sign if toward observer, + sign if away from observer. Notice: different f for observers on opposite sides of the source! 16

Doppler effect for EM waves (light, radio, etc): For EM waves, there is no material medium! In the 1800s, people assumed there had to be some kind of medium for light -- so maybe it could be massless or otherwise undetectable! If the luminiferous ether exists, it plays the same role as air for sound waves: its rest frame is a special coordinate system for light waves! Fact: no such thing (more on this later this week) Speed of light is the same in all coordinate frames (!)! Does not depend on motion of source or observer! So we only need the Doppler formula for source at rest f ' = f! 1± u $ " # c % & (+ for approaching, - for moving apart) Now u = relative speed between source and observer This formula is accurate only if u << c (Einstein will tell us more ) Example: car 1 moves N at 50 mph, car 2 (ahead of 1) moves N at 25 mph Then they are approaching each other at relative speed 25 mph We have no medium to define a specially significant coordinate frame 17

Any warm object makes E-M waves! Any object s molecules are vibrating in place As long as its temperature is above absolute zero = 270 below zero Celsius! Molecules are made of charged particles! So they emit E-M radiation! Frequency of emission depends on molecular speed! Total radiation from any object covers a broad range of frequencies (wavelengths): random mix of molecular speeds Calculated spectrum (graph of intensity vs wavelength) from an ideal radiator is called blackbody spectrum! Ideal radiator = ideal radiation absorber! Color of an object = color of light it reflects (does not absorb) So, what color would an ideal absorber appear to be? 18

Clicker Quiz 4 Light travels through a vacuum while sound cannot. This is because A)! Sound waves require a material medium, light does not B)! Light waves require a material medium, sound does not C)! Light moves in a mysterious hidden dimension unknown to Man D)! Huh? Sound CAN travel through a vacuum 19