Week 3 Gravitational Lensing & Polarisation Flashcards

1
Q

briefly describe the snellian approach to gravitational lensing

A

mass bends light so positions are calculated by finding bending angles

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2
Q

briefly describe the fermattian approach to gravitational lensing

A

light suffers from a delay called shapiro delay so find a compromise minimum path between most direct and most bent

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3
Q

what are the four key properties of Linear Polarisation

A

> E remains in the same plane as the wave propagates
plane containing E is at angle arctan[Ey/Ez] to x axis
max E is SQRT[Ex^2 + Ey^2]
no phase shift between x and y

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4
Q

what are the two key properties of circular polarisation

A

> E remains same size but rotates around direction of propagation
phase shift of +-90 between x and y

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5
Q

what is the elliptical polarisation equation

A

XExcos[kx-ωt+φ1] + YEycos[kx-ωt+φ2]

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6
Q

what are the 3 key properties of the elliptical polarisation equation

A

> linear if φ1 = φ2
circular is φ2 - φ1 = +-90
E describes an ellipse with time at any point

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7
Q

what is the condition for full polarisation by reflection

A

if the reflected ray is orthogonal to refracted ray then reflected ray is fully polarised

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8
Q

what is the Brewster angle equation

A

tanθi = nr / ni

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9
Q

what do the Fresnel coefficients do

A

they give the degree of polarisation for arbitrary angles

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10
Q

what are the two Fresnel coefficients equations

A
|b|^2 = [sin(θi-θr)]^2 / [sin(θi+θr)]^2
|B|^2 = [tan(θi-θr)]^2 / [tan(θi+θr)]^2
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11
Q

what is the degree of polarisation equation

A

|b|^2 - |B|^2 / |b|^2 + |B|^2

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12
Q

briefly describe how polarising by scattering works

A

light passes through a scattering medium
depending on the position of the observer relative to the scattering medium the observer will see different amounts of polarisation

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