Chapter 23 – Electromagnetic Waves

Chapter 23 – Electromagnetic Waves Electromagnetic Waves

What’s Happ’nin??? • Administrative • Quiz Today • Review Exam Grades • Review Exam • Begin Chapter 23 – Electromagnetic Waves • No 10:30 Office Hours Today. (Sorry) • Next Week … More of the same. • Watch for still another MP Assignment • Will they ever stop??? (No) Electromagnetic Waves

Section 003 Average = 55% Electromagnetic Waves

Section 004 Average*52 Electromagnetic Waves

Electromagnetic Waves

What do we learn from this? • Some of you studied. • Some of you didn’t. • If you didn’t, do. • Or take my Studio Class in the Spring! Electromagnetic Waves

We have studied • Electric Fields and Potential • Magnetic Fields • The interactions between E & M • E&M Oscillations (AC Circuits/Resonance) • James Clerk Maxwell related all of this together is a form called Maxwell’s Equations. Electromagnetic Waves

James Clerk Maxwell • 1831 – 1879 • Electricity and magnetism were originally thought to be unrelated • In 1865, James Clerk Maxwell provided a mathematical theory that showed a close relationship between all electric and magnetic phenomena • Electromagnetic theory of light Electromagnetic Waves

Maxwell Equations closed surface enclosed charge closed surface no mag. charge closed loop linked current + flux closed loop linked flux • Conservation of energy • Conservation of charge Lorentz force law Electromagnetic Waves

Both Maxwell’s Equations and Experimental Evidence Suggested • When an E or B field is changing in time, a wave is created that travels away at a speed c given by: • This is the experimental value for the speed of light. This suggested that Light is an Electromagnetic Disturbance, • In depth experimental substantiation followed. Electromagnetic Waves

Electromagnetic Waves • Can travel through empty space or through some solid materials. • The electric field and the magnetic field are found to be orthogonal to each other and both are orthogonal to the direction of travel of the wave. • EM waves of this sort are sinusoidal in nature. • Picture a sine wave traveling through space. Electromagnetic Waves

Hertz’s Confirmation of Maxwell’s Predictions • 1857 – 1894 • First to generate and detect electromagnetic waves in a laboratory setting • Showed radio waves could be reflected, refracted and diffracted (later) • The unit Hz is named for him Electromagnetic Waves

Hertz’s Experimental Apparatus • An induction coil is connected to two large spheres forming a capacitor • Oscillations are initiated by short voltage pulses • The oscillating current (accelerating charges) generates EM waves

Hertz’s Experiment • Several meters away from the transmitter is the receiver • This consisted of a single loop of wire connected to two spheres • When the oscillation frequency of the transmitter and receiver matched, energy transfer occurred between them

Hertz’s Conclusions • Hertz hypothesized the energy transfer was in the form of waves • These are now known to be electromagnetic waves • Hertz confirmed Maxwell’s theory by showing the waves existed and had all the properties of light waves (e.g., reflection, refraction, diffraction) • They had different frequencies and wavelengths which obeyed the relationship v = f λ for waves • v was very close to 3 x 108 m/s, the known speed of light

EM Waves by an Antenna • Two rods are connected to an oscillating source, charges oscillate between the rods (a) • As oscillations continue, the rods become less charged, the field near the charges decreases and the field produced at t = 0 moves away from the rod (b) • The charges and field reverse (c) – the oscillations continue (d)

EM Waves by an Antenna, final • Because the oscillating charges in the rod produce a current, there is also a magnetic field generated • As the current changes, the magnetic field spreads out from the antenna • The magnetic field is perpendicular to the electric field

Electromagnetic Waves, Summary • A changing magnetic field produces an electric field • A changing electric field produces a magnetic field • These fields are in phase • At any point, both fields reach their maximum value at the same time

Light My Candle Was It Magic? Electromagnetic Waves

DEMO Electromagnetic Waves

Antennas of all kinds

The Electromagnetic Wave

More … • The waves are transverse: electric to magnetic and both to the direction of propagation. • The ratio of electric to magnetic magnitude is E=cB. • The wave(s) travel in vacuum at c. • Unlike other mechanical waves, there is no need for a medium to propagate.

Rules – Don’t try to remember these? • The old RH-Rule • turn E into B and you get the direction of propagation c. • Rotate c into E and get B. • Rotate B into c and get E. Electromagnetic Waves

l Wavelength Electromagnetic Waves

The Electromagnetic Spectrum Electromagnetic Waves

Images at different wavelengthsfor modern astronomy. Electromagnetic Waves

Seeing in the UV, for example, steers insects to pollen that humans could not see. Electromagnetic Waves

X-Rays Electromagnetic Waves

Wave Fronts Electromagnetic Waves

Two types of waves Electromagnetic Waves

Suggestion – Look again at the chapter on sound to solidify this stuff. Electromagnetic Waves

ENERGY How much Energy is in this volume? Electromagnetic Waves

Light carries Energy and Momentum Electromagnetic Waves

MOMENTUM ENERGY & Electromagnetic Waves

Energy stored in the B and B fields are the same! Electromagnetic Waves

Electric and magnetic fields contain energy, potential energy stored in the field: uE and uB • uE: ½ 0 E2electric field energy density • uB: (1/0) B2 magnetic field energy density • The energy is put into the oscillating fields by the sources that generate them. • This energy can then propagate to locations far away, at the velocity of light. Energy in Electromagnetic Waves

Energy in Electromagnetic Waves Energy per unit volume is u = uE + uB Thus the energy, dU, in a box of area A and length dx is Let the length dx equal cdt. Then all of this energy leaves the box in time dt. Thus energy flows at the rate B dx area A E c propagation direction

Energy Flow in Electromagnetic Waves B Rate of energy flow: dx area A E We define the intensityS, as the rate of energy flow per unit area: c propagation direction Rearranging by substituting E=cB and B=E/c, we get,

The Poynting Vector In general, we find: S = (1/0)EB Sis a vector that points in the direction of propagation of the wave and represents the rate of energy flow per unit area. We call this the “Poynting vector”. Units of S are Jm-2 s-1, or Watts/m2. B dx area A E propagation direction

r Source The Inverse-Square Dependence of S A point source of light, or any radiation, spreads out in all directions: Power, P, flowing through sphere is same for any radius. Source

Example:An observer is 1.8 m from a point light source whose average power P= 250 W. Calculate the rms fields in the position of the observer. Intensity of light at a distance r is S= P / 4pr2

Light can exert physical pressure – • When present in large flux, photons can exert measurable force on objects. • Massive photon flux from excimer lasers can slow molecules to a complete stop in a phenomenon called “laser cooling”.

Wave Momentum and Radiation Pressure Momentum and energy of a wave are related by, p = U / c. Now, Force = d p /dt = (dU/dt)/c pressure (radiation) = Force / unit area P = (dU/dt) / (A c) = S / c Radiation Pressure 

Ey Bz x Polarization The direction of polarization of a wave is the direction of the electric field. Most light is randomly polarized, which means it contains a mixture of waves of different polarizations. Polarization direction

Polarization A polarizer lets through light of only one polarization: E Transmitted light has its E in the direction of the polarizer’s transmission axis. E0 E q E = E0 cosq hence, S = S0 cos2q - Malus’s Law

At least of this chapter. Electromagnetic Waves

Chapter 23 – Electromagnetic Waves