Maxwells equations Plane waves in a vacuum Plane

  • Slides: 46
Download presentation

Maxwell’s equations

Maxwell’s equations

Plane waves in a vacuum

Plane waves in a vacuum

Plane waves in a vacuum

Plane waves in a vacuum

Plane waves in a vacuum

Plane waves in a vacuum

Plane waves in a vacuum

Plane waves in a vacuum

1638 - Galileo attempts to measure the speed of light by a lantern relay

1638 - Galileo attempts to measure the speed of light by a lantern relay between distant hilltops. He gets a very large answer.

Albert Einstein, when asked to describe radio, replied: "You see, wire telegraph is a

Albert Einstein, when asked to describe radio, replied: "You see, wire telegraph is a kind of a very, very long cat. You pull his tail in New York and his head is meowing in Los Angeles. Do you understand this? And radio operates exactly the same way: you send signals here, they receive them there. The only difference is that there is no cat. "

There was a young lady named Bright, Whose speed was far faster than light;

There was a young lady named Bright, Whose speed was far faster than light; She set out one day, In a relative way, And returned home the previous night.

one dimensional wave equation Ey x yz

one dimensional wave equation Ey x yz

one dimensional wave equation Ey x yz

one dimensional wave equation Ey x yz

 • MOST GENERAL SOLUTION!! • Ey = a F(z - ct) + b

• MOST GENERAL SOLUTION!! • Ey = a F(z - ct) + b G(z + ct) • = a F b G • where F & G are arbitrary functions that depend on the excitation

 • Q. E. D. • Ey = a F(z - ct) + b

• Q. E. D. • Ey = a F(z - ct) + b G(z + ct) • = a F b G • is a solution of the wave equation!!!

Ey = a. F(z - ct) + b. G(z + ct) = a. F

Ey = a. F(z - ct) + b. G(z + ct) = a. F b. G Ey Ey t=T z t = 2 T z

Ey = a. F(z - ct) + b. G(z + ct)

Ey = a. F(z - ct) + b. G(z + ct)

Ey = a. F(z - ct) + b. G(z + ct) = a. F

Ey = a. F(z - ct) + b. G(z + ct) = a. F b. G Let c=2 10 z = z - ct = 0 = z + ct = 0 t z z 0 0 0 1 2 -2 2 4 -4 3 6 -6 4 8 -8 0 -10 5 t

Ey = a. F(z - ct) + b. G(z + ct) = a. F

Ey = a. F(z - ct) + b. G(z + ct) = a. F b. G Let c=2 10 z = z - ct = 0 = z + ct = 0 t z z 0 0 0 1 2 -2 2 4 -4 3 6 -6 4 8 -8 0 -10 5 t

perturbation transverse to the direction of propagation “transverse waves”

perturbation transverse to the direction of propagation “transverse waves”

perturbation transverse to the direction of propagation “transverse waves” “trajectory” z * * t

perturbation transverse to the direction of propagation “transverse waves” “trajectory” z * * t

the flood

the flood

whips and chains

whips and chains

F(Z –CT) F(Z +CT)

F(Z –CT) F(Z +CT)

“the slinky wave”

“the slinky wave”

“the slinky wave”

“the slinky wave”

“the slinky wave” perturbation is in the direction of propagation “longitudinal wave” sound waves--compression

“the slinky wave” perturbation is in the direction of propagation “longitudinal wave” sound waves--compression & rarefaction of air

ion acoustic wave in a plasma

ion acoustic wave in a plasma

nerve propagation test for MS

nerve propagation test for MS

nerve propagation test for MS Pulse generator

nerve propagation test for MS Pulse generator

general properties of linear waves

general properties of linear waves

soliton - soliton collision

soliton - soliton collision

Twinkie shortage looms March 21, 2000 PORTLAND, Maine (AP) - A Teamsters strike against

Twinkie shortage looms March 21, 2000 PORTLAND, Maine (AP) - A Teamsters strike against a bakery company is creating shortage of Twinkies across parts of the Northeast. A Philadelphia bakery was shut down after pickets appeared Monday, and Teamsters planned to set up pickets in Buffalo, N. Y. , as well. A New York City bakery also was shut down over the weekend. "It's a wave that's going to go right across the country, " said Richard Volpe, director for the union in the United States and Canada.