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Polarization Physics 102 Professor Lee Carkner Lecture 28
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Page 1: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Polarization

Physics 102Professor Lee

CarknerLecture 28

Page 2: Polarization Physics 102 Professor Lee Carkner Lecture 28.

PAL #27 EM Spectrum

Acceleration of lightsail craft I = Ps/4r2 = (3.9X1026)/((1.5X1011)2)

= pr = 2I/c

pr = (2)(1379)/(3X108) =

F = ma = prA a = prA/m a = (9.2X10-6)(2.25X108)/5000 =

Page 3: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Polarization

The plane containing the E vectors is called the plane of oscillation

Most light sources are unpolarized, any given wave has a random plane of oscillation

Page 4: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Plane of Oscillation

x

y

z

y

z

E

E

Page 5: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Direction of Polarization

Page 6: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Unpolarized Light

Page 7: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Polaroid

Polaroid is a sheet of material that will only pass through the components of the E vectors in a certain direction

If you put a horizontal Polaroid sheet on top of a vertical Polaroid sheet no light gets through

Page 8: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Polarizing Sheet

Page 9: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Polarization and Intensity

The sum of all of the y components should be equal to the sum of all of the z components

I = ½ I0 This is true only when the incident

light is completed unpolarized

Page 10: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Angle of Polarization

Page 11: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Incident Polarized Light For polarized light incident on a sheet of

Polaroid, the resultant intensity depends on the angle between the original direction of polarization and the sheet

E = E0 cos

I = I0 cos2

The angle can be the angle between two

adjacent polarizing sheets

Page 12: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Multiple Sheets

Page 13: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Sheet Angles

Page 14: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Today’s PAL

Consider unpolarized light incident on a stack of 3 polarizing sheets. The first sheet is aligned in the vertical direction. The second sheet is aligned 45 degrees from the vertical, and the third sheet is aligned in the horizontal direction. What fraction of the original intensity do you see if you look at the light after it passes through the third sheet?

What would you see if you remove the second sheet?

Page 15: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Means of Polarization

This alignment permits only the components in that direction to pass

The dust grains are partially aligned by the galactic magnetic field and so the light is partially polarized

Light can also be polarized by reflection

Page 16: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Interstellar Polarization

Page 17: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Reflection Polarization

Page 18: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Polarization By Reflection Light reflected off of a surface is

generally polarized This is why polarized sunglasses

reduce glare

Page 19: Polarization Physics 102 Professor Lee Carkner Lecture 28.

Next Time

Final: Section 1, Tuesday, February 22, 9am Section 2, Thursday, February 24, noon

Covers Chapters 21-22, 24.10 (2/3) and Chapters 13-20 (1/3) About 15 multiple choice, 6 problems Structured like previous tests

Practice problems online