Snell's Law
n 1 Sin [θ 1 ] = n 2 Sin [θ 2 ]
c n = c / n
λ n = λ / n
I θ = I 0 E 2 θ / E 2 0
Where n is the refraction index of the material
c n = c / n
λ n = λ / n
I θ = I 0 E 2 θ / E 2 0
Where n is the refraction index of the material
Lens Equation:
1 / d i + 1 / d o = 1 / f
m = - d i / d o
Where d i is the distance to the image and d o is the distance to the object. m represents the magnification of the object in comparison to the objects actual size.
m = - d i / d o
Where d i is the distance to the image and d o is the distance to the object. m represents the magnification of the object in comparison to the objects actual size.
Lens maker Equation:
1 / f = (n - 1) (1 / R 1 + 1 / R 2 )
r = f / 2
f is the focal length, and r is the radius of curvature. The focal length is the distance at which the parallel rays of light travelling through the lens will converge to a point. The radius of curvature represents the radius of the sphere that the lens could make if it was continued to a sphere.
r = f / 2
f is the focal length, and r is the radius of curvature. The focal length is the distance at which the parallel rays of light travelling through the lens will converge to a point. The radius of curvature represents the radius of the sphere that the lens could make if it was continued to a sphere.
Interference and Diffraction-
Double Slit interference:
I θ = I 0 [Cos(δ / 2)] 2
d Sin[θ] = m λ / Maxima
d Sin[θ] = (m +1/2) λ / Minima
d Sin[θ] = m λ / Maxima
d Sin[θ] = (m +1/2) λ / Minima
Single Slit diffraction:
I θ = I 0 [Sin(Β/2) / (Β / 2)] 2
D Sin[θ] = (m +1/2) λ / Maxima
Note - θ = 0 is the central and highest peak
D Sin[θ] = m λ / Minima
D Sin[θ] = (m +1/2) λ / Maxima
Note - θ = 0 is the central and highest peak
D Sin[θ] = m λ / Minima
Single and double slit effects:
I θ = I 0 [Sin(Β/2) / (Β / 2)] 2 [Cos(δ / 2)] 2
Diffraction grating:
Sin (θ) = m λ / d
R = λ / (Δ λ) = N m
R is the resolving power of the lens
R is the resolving power of the lens
Circular hole diffraction
θ = 1.22 λ / D
Polaroids
I = I 0 (Cos[θ]) 2
Relativity
Minkowski space-This is the setting in which relativistic calculations are done. Points in Minkowski space are represented by a 4-vector which defines position in x, y, z and time, and is represented by the Minkowski metric, which is defined as:
[-1 0 0 0]
| 0 1 0 0|
| 0 0 1 0|
[ 0 0 0 1]
| 0 1 0 0|
| 0 0 1 0|
[ 0 0 0 1]
Invariance of the interval:
(Δs) 2 = (Δx) 2 - (c Δt) 2
(Δs') 2 = (Δs) 2
The invariance of the interval is also known as the line element of the minkowski metric.
(Δs') 2 = (Δs) 2
The invariance of the interval is also known as the line element of the minkowski metric.
Lorentz Transformations-
ct = γ ( v x' / c + c t ' )
x = γ ( x' + v t ' )
y = y'
z = z'
x = γ ( x' + v t ' )
y = y'
z = z'
This is assuming your working in a frame where there is movement in only one direction, however due to the isotropy of space, you can almost always make this assumption.
γ = 1 / [1 - (v / c) 2 ] 1/2
This is known as the lorentz factor, which is used in the lorentz transformation.
This is known as the lorentz factor, which is used in the lorentz transformation.
Velocity addition formulas-
u parallel = (u parallel ' + v) / (1 + (u x ' v / c 2 ))
u perpendicular = (u perpendicular ') / [γ (1 + (u perpendicular ' v / c 2 ))]
u parallel = (u parallel ' + v) / (1 + (u x ' v / c 2 ))
u perpendicular = (u perpendicular ') / [γ (1 + (u perpendicular ' v / c 2 ))]
Contraction
L' = L / γ
Where L' is the length of the moving object as observed by the stationary frame.
Δt' = γ Δt
Where t ' is the length of time experienced by an observer in the stationary frame.
Where L' is the length of the moving object as observed by the stationary frame.
Δt' = γ Δt
Where t ' is the length of time experienced by an observer in the stationary frame.
Stationary frames are described by no acceleration.
Non constant velocity
τ = ∫ [1 - ( v 2 (t) / c 2 )] 1/2 dt
Momentum and Energy
p = γ m v
E = γ m c 2 = [m 2 c 4 + |p| 2 c 2 ]
E 2 = m 2 c 4 + p 2 c 2
KE = E - m 2 c 2 = (γ - 1) m c 2
E = γ m c 2 = [m 2 c 4 + |p| 2 c 2 ]
E 2 = m 2 c 4 + p 2 c 2
KE = E - m 2 c 2 = (γ - 1) m c 2
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