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Material Type: Notes; Class: Radiation Science; Subject: Physics; University: University of Mississippi Main Campus; Term: Unknown 1989;
Typology: Study notes
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E
B
Plane Wave
v = c
a
b
Consider a dipole antenna emitting EM radiation. The E-field follows the charge up and down, The B-field circulates about the current I flow up and down.
E = ( V/d ) k d = length of the antenna B = ( μo I/ 2πR ) i R = radius of the antenna wire
S = ( V /d) ( μo I/ 2πR ) k x i = ( V /d) ( μo I / 2πR ) j
Power emitted from the surface of the antenna P = S x Area P = 1/ μo {(V/d) ( μo I/ 2πR )} 2πR d = I V P =IV (Watts) V = IR (Ohm’s Law)
R
d
V - Oscillator i
j
I k
Hertz Dipole Antenna Waves
E
V
V=
c
V
θ
V
V
7
ETHER HYPOTHESIS BUSTED - NO ETHER!!
Light source 2nd slit
Mirror- 1
Mirror- 2
Beam Splitter - 0 L
Interference Pattern or not? Not?
V Ether Wind
β = V/c Relative speed 0 1
γ = (1- β^2 )-1/^2 Lorentz factor 1
EINSTEIN’s POSTULATES OF RELATIVITY
A
B c
c c +V
Consider light of frequency fo being emitted from a source. An outside Observer will measure a shifted frequency coming from the source
!
f = fo^1 "^ # 1 + #
Source moving away from the Observer with relative speed β. RED SHIFT
!
f = fo^1 +^ " 1 # "
Source moving toward the Observer with relative speed β. BLUE SHIFT
λ = f / c
600nm 500nm 400nm
fo
f <fo (^) f >fo
Einstein used the Lorentz transformation to form a 4-dimensional spacetime.
Let x’ t’ denote the position and time in the laboratory system Let x t denote the position and time in the moving system.
Lorentz Transform Derivative x’ = γ (x + vt) dx’ = γ (dx + v dt) t’ = γ (t + v x/c^2 ) dt’ = γ (dt + v dx/c^2 )
Velocity Transform Vx’ = dx’/dt’ = (dx + β cdt ) / (cdt + β dx )
v= relative velocity Vx = velocity of an object in the moving frame. Vx’ = velocity of the same object as measured in the Lab frame.
Vx << c Vx’ = Vx + v NEWTON Vx = c (flashlight) Vx’ = c EINSTEIN
Lab
Moving β=v /c
x ct
x’ ct’
!
Vx '= Vx^ +^ v 1 + Vx • v / c^2
Lab
Vx=c
Vx’=?
β=v/c