Irregular Webcomic!

Archive     Blog     Cast     Forum     RSS     Books!     Poll Results     About     Search     Fan Art     Podcast     More Stuff     Random     Support on Patreon
New comics Mon-Fri; reruns Sat-Sun
<   No. 3335   2014-06-08   >

Comic #3335

1 {photo of a cathedral under a deep blue sky}
1 Caption: Polarisation

First (1) | Previous (3334) | Next (3336) || Latest Rerun (2608) | Latest New (5242)
First 5 | Previous 5 | Next 5 | Latest 5
Annotations theme: First | Previous | Next | Latest || First 5 | Previous 5 | Next 5 | Latest 5
This strip's permanent URL:
Annotations off: turn on
Annotations on: turn off

Michael Faraday
Michael Faraday, photographed in 1913. Public domain image from Wikimedia Commons.
I've been watching the new series of Cosmos, hosted by Neil deGrasse Tyson. I recall the original series, hosted by Carl Sagan, vividly from my childhood. It was a large part, perhaps the single largest influence, on me choosing a career in science.

Anyway, Tyson's remake has the advantage of new discoveries made since 1980, and more advanced visual effects. Nevertheless, I get the slight nagging feeling that Tyson's script is talking down to the audience a little bit - a feeling I never got with Sagan (and I rewatched Sagan's Cosmos just a few months ago and didn't feel it then). And I got it especially with the latest new episode I watched, which was about electromagnetism and Michael Faraday.[1] Tyson was narrating an experiment which Faraday had performed with polarised light, to see if a magnetic field would affect it. I thought his explanation of polarisation was, well, sloppy and not very informative. What's more, he followed up with a pseudo-apology, saying (paraphrased slightly - I don't recall the exact words), "Don't worry if you didn't quite understand that, it's pretty complicated."

This is the wrong thing to say in an educational program!! I was practically screaming at the TV (not literally, since my wife was watching with me), "I could have written that bit better! You have four sentences to explain polarisation, and that's the best you can do?!"

Now, it is very easy to criticise something for being less than perfect, or even just less than you think it should be. Everyone criticises stuff - just take a look at the Internet any time. What's more difficult, and what most criticisers fail to do, is to do better. Very well, Tyson. Thou hast thrown down the gauntlet, and I hereby pick it up:

Light is an electromagnetic wave, which is to say a propagating wave made of electric and magnetic fields. The electric field, to pick one, can oscillate in any direction perpendicular to the direction the light is travelling, in the same way that a stretched string can vibrate up and down, or side to side, or any angle in between. Normally, light is made up of collections of waves oscillating in all directions, or polarisations, randomly. But it's also possible to generate or filter light so that it is made up of waves all oscillating in the same direction, or polarisation - and we call that polarised light.

There's a lot more you can say about polarisation and polarised light, but those few sentences would have introduced the concept and explained it enough for viewers to understand Faraday's experiment much better.

Linear polarisation
Light waves commonly have electric fields oscillating in all directions (left). Passing through a polarising filter (grid at centre) restricts the transmitted light's electric field to a single plane of oscillation (right). Creative Commons Attribution-Share Alike image by Bob Mellish, from Wikimedia Commons.
But wait! I have more space! So I can say a bit more about polarisation! Let's look a little deeper then.

Much of the light in the natural world is comprised of a random mixture of all polarisations, making what we call unpolarised light. But certain processes can filter out some polarisations, leaving others to continue as more or less polarised light. Polarisation is not an all or nothing thing. If a beam of light is predominantly polarised in one direction, but still contains some light polarised in other directions, we say the beam is partially polarised. The degree of polarisation can be anything from 0 (completely random and unpolarised) to 100% (all light in the beam is polarised in exactly the same direction).

How is polarised light generated? One simple way, which occurs in nature, is to reflect it off something transparent, say a sheet of glass or pool of water. When light hits the surface of a pool of water, some of the light passes into the water, but some is reflected off the surface. Which specific waves of light pass through and which are reflected depend strongly on their polarisations. At a certain specific angle of incidence (which is governed by the refractive index of the material), all of the reflected light will be polarised, with its electric field oscillating parallel to the water surface. All electric field oscillations perpendicular to the surface pass into the water.

This separation of light into different polarisations does not just pick out the tiny tiny fraction of light rays (or photons, if you prefer) which happen to have polarisation parallel to the water surface, and reject all the others. That would leave very little light at all, since almost all of the light is not polarised exactly parallel to the water surface. Rather, the reflection separates all of the light into components parallel and perpendicular to the surface. So if the light already happens to be fully polarised at, say, 45° to the surface, then half the light is reflected and half the light passes into the water.

Brewster angle

Light incident on a surface at the Brewster angle. Most of the polarisation parallel to the surface (dots) is reflected, none of the polarisation perpendicular to the surface (arrows) is reflected. Public domain image by Wikipedia user Pajs, from Wikimedia Commons.
If you know your vector arithmetic, this is just projection into orthogonal components. The electric field component parallel to the water is one divided by the square root of 2 times the strength of the original 45° field, as is the electric field component perpendicular to the water. Approximating with decimals, the polarised reflected light has an electric field strength 0.707.. times the strength of the incident light, and the light entering the water also has an electric field strength 0.707.. times the strength of the incident light. But wait, you may say, that adds up to 1.414.. (or the square root of 2) times the incoming light strength! Yes it does, but we're not talking about the energy or brightness intensity of the light. The amount of energy (or brightness intensity) of a beam of light depends on the square of the electric field strength. So the energy or brightness of the reflected beam is half the incident beam, and so is the energy of the transmitted beam. So all the necessary quantities are conserved.

One wrinkle in this method of polarising light is that the light only becomes fully polarised if it is hitting the water at the specific angle previously mentioned. This specific angle is called the Brewster angle. At other angles, the reflected light is only partially polarised, with the amount of polarisation decreasing as the angle moves away from the Brewster angle.

Another way to produce polarised light is to pass it through a polarising material. One such material is known by the trade name of Polaroid[2], and is commonly used in sunglasses and glare filters. Polaroid works because of its molecular structure. During manufacture, the plastic material is stretched in one direction. This lines up long polymer molecules, forming sort of spaghetti strands within the material, all parallel to one another. These strands have electrical properties that affect the passage of light. An electric field oscillating perpendicular to the strands can pass through, but not one oscillating parallel to them. This means that if light passes through a piece of Polaroid, only the electric vector components perpendicular to the molecules can get through. The component of the field parallel to the strands is blocked, and the Polaroid material absorbs that energy. If you shine a beam of unpolarised light through Polaroid, the light that emerges is polarised in one direction and has energy (or intensity) half that of the incoming light. The other half is absorbed. This is why Polaroid material looks a dark grey colour - it is blocking half the light that enters it.

Polarising glasses
Polarising sunglasses. Reflected glare from the road is greatly reduced. Creative Commons Attribution-NonCommercial-Share Alike image by Ed Flores, from Flickr.
This is also why Polaroid makes a great material for sunglasses. It cuts out half the incoming light, but it does more than that. It lets through light polarised vertically, but completely blocks light that is polarised horizontally. Like much of the light reflected off a water surface. So in many situations, Polaroid sunglasses are more effective than a simple grey filter that blocks half the incoming light. Besides doing that, Polaroid also significantly reduces glare reflected off horizontal surfaces such as lakes, puddles, roads. Because glass panels on the front and back of cars tend to be sloped, Polaroid also helps reduce reflective glare off those too.

This effect of reducing typical glare only works if the Polaroid molecules are aligned horizontally. If the Polaroid is rotated (you can try this if you have polarising sunglasses by simply turning them, or tilting your head while wearing them), it won't be as effective at cutting the reflected glare. Polarising sunglasses won't normally reduce glare reflected sideways off vertical panes of glass, but they will if you turn them by 90°.

Here's where polarised light starts getting really interesting. If you take two pieces of Polaroid and hold them up together, you can see some interesting things. Each piece of Polaroid cuts the brightness of normal unpolarised light by 50%. So if you stack two of them on top of each other and look through them, how bright is the light passing through? The answer is: it depends. If the molecular axes of the two pieces of Polaroid are aligned, then the light hitting the second sheet is already polarised by the first sheet, so all of it passes through and none is absorbed. On the other hand, if the molecular axes are at 90° to one another, all of the light is absorbed by the second sheet and none gets through. So depending on the relative rotations of the two sheets of Polaroid, the resulting brightness can be anywhere from 50% to 0% of the original light. If you have two pairs of polarising sunglasses you can see this effect easily by looking through both pairs at once, and rotating one of them.

Stacked Polarising filters
Stacked linear polarising filters. The two large filters are at 90°, so they block all light. The smaller filter is turned to an intermediate angle, so passes a component of the light from the first filter at that angle, which then provides a component which can get through the second large filter. Creative Commons Attribution-NonCommercial image by Paul, from Flickr.
Polaroid and similar materials are not the only materials that interact with polarisation in interesting ways. Some materials which look transparent actually rotate the plane of polarisation of light passing through them. Several types of plastic do it, clear sticky tape does it, and even a solution of sugar dissolved in water does it. These materials are called optically active. Imagine setting up two sheets of Polaroid with crossed axes so that no light gets through the combination. Let's say light passing through the first sheet is polarised vertically, and the second sheet is oriented with its polarisation axis horizontal. If you put a piece of the right sort of plastic in between, the light passing through the plastic will have its polarisation rotated. If it is rotated by 90°, then all the light passing through the plastic will now pass through the second sheet of Polaroid. By inserting an object in the way, you have made the light look brighter!

The angle by which the plastic rotates the polarisation depends on the molecular properties of the plastic, and the thickness. Put two layers of the same plastic there, and it will rotate the polarisation by twice the angle. The angle can also depend on the wavelength, or colour, of the light. Some colours might be rotated by different angles, resulting in them appearing brighter or darker when seen through the entire setup. This is the source of the rainbow colour effects you sometimes see when wearing polarising sunglasses and looking at glass or transparent plastic surfaces.

This leads to another practical application of polarisation. If you do this with pieces of plastic such as rulers or protractors, you'll see coloured patterns, even though the thickness might be constant. These correspond to regions of the plastic where the molecular structure has been stressed by the manufacturing process. If you bend the plastic, you'll see the patterns change as the stress patterns within the plastic change. So you can use polarisation to examine stress regions in certain materials.

Another application is related to the sugar solution example mentioned above. Sugar (more specifically, common table sugar, or sucrose) is what is known as a chiral molecule, which means that the atoms are bonded together in such a way that the molecule does not have mirror symmetry. If you reflect the structure in a mirror, you get another molecule which cannot be rotated to match the original - like left and right hands. This asymmetry gives rise to the effect of rotating the plane of polarisation of light passing through the sugar.

Optical activity
Optically active plastic (a French curve) between crossed polarising sheets, showing stress patterns. Creative Commons Attribution-NonCommercial-Share Alike image by Tom Paton, from Flickr.
Let's call the two types of sugar molecule left-handed and right-handed. If you have an equal mixture of both, and you pass polarised light through a solution of them, nothing much happens. The light emerges as it went in. But if your solution is made entirely of left-handed sugar, then a curious thing happens - it twists the plane of polarisation to the left (i.e. anticlockwise). Similarly, if you have a solution of right-handed sugar, it twists the plane of polarisation to the right (clockwise). Using a sheet of Polaroid you can detect the plane of polarisation of the emerging light and measure the amount of the twist. And the amount of twist depends on the concentration of the sugar solution - how many sugar molecules there are.

This means two things: (1) If you know beforehand that the sugar is entirely left-handed (or entirely right-handed), you can measure the concentration of the solution by measuring its effect on polarised light. (2) On the other hand, if you know the concentration of the solution, you can determine by the angle of rotation what percentage of the sugar is left-handed and what is right-handed.

Sugar is not the only chiral molecule which affects polarisation. Some molecules found in molecular clouds in space do the same thing. And what's more, some radiation sources in space are polarised, particularly radio sources. (Radio is an electromagnetic wave like light, so can also be polarised.) Here the polarisation is caused by magnetic fields. We can detect polarised radio waves with radiotelescopes. If we could measure how much the plane of polarisation has been rotated, we could measure the amounts of chiral molecules in molecular clouds between us and a radio source. We don't know the original plane of polarisation, however we can work it out, because the rotation angle varies with wavelength. By measuring the polarisation of several radio wavelengths, we can "unrotate" them by different thicknesses of molecules until they all match - and that allows us to measure the concentrations of molecules in deep space.

Polarised reflections
Difference between a scene photographed in normal light (left) and polarised light (right). Creative Commons Attribution-NonCommercial-Share Alike image by Andy Urban, from Flickr.
Another source of polarisation is the sky. Sunlight reflects (or scatters) off molecules in the air, which is why the entire sky is bright, rather than black like it is on the Moon even when the sun is up. (The scattering depends on wavelength, which is why the sky is blue, but that's another story.) This reflection partially polarised the light from the sky. It is least polarised near the sun and most polarised at a point away from the sun. If you wear polarised sunglasses and look up at the sky away from the sun, you can detect the polarisation by the change in brightness as you tilt your head side to side. Photographers know this and use polarising filters on their cameras to darken the sky in photos, to avoid it washing out and being too bright - though it darkens the sky away from the sun much more than it darkens the sky near the sun (see title photo above). Photographers also use such filters to reduce glare from water, or to reduce reflections when shooting through glass.

Some insects, notably bees, can detect the polarisation of light. This allows them to navigate using the position of the sun, even when it's cloudy, since the polarised light of the sky penetrates the clouds. Human eyes cannot easily detect or distinguish polarisation, but we do have a very slight sensitivity to it. There is an experiment you can try to see if you can detect the polarisation of the sky, or a polarised display screen. It is borderline detectable - some people can see it and some can't. (I've tried and I'm not convinced I can detect anything. Maybe you will have better luck.)

Brewster angle
Diagram of linearly polarised light (left) and circularly polarised light (right). The red line shows the electric field strength and direction as the wave propagates along the black axis. The green and blue waves show the components in the horizontal and vertical planes, respectively. Public domain image by Wikipedia user Dave3457, from Wikimedia Commons.
A final wrinkle is that light can be polarised in another way as well. Imagine holding one end of a skipping rope, with the other end tied to something or held by another person. You can send a wave along the rope by wiggling it up and down, or side to side, or any angle in between. You could also wiggle your end in a circle, sending a spiralling wave of motion along the rope. And you can do this either clockwise or anticlockwise. These spiral waves are analogous to what is known as circular polarisation, in which the electric field of a light ray does not simply wiggle up and down or side to side or whatever, but instead rotates around the axis of travel. And just as with the rope, there are two different circular polarisations, clockwise and anticlockwise. To be specific about the other sort of polarisation (the one we've been discussing previously), it is called plane polarisation, because the electric field oscillates in a single plane, or linear polarisation.

Light can be made circularly polarised not by blocking one of the plane polarisation directions, but by slowing it down. Light slows down when it propagates through a material. (The "speed of light" which is constant in Einstein's relativity refers to the speed of light in vacuum.) The ratio of the speed of light in vacuum to the speed of light in a material is called the refractive index of the material. Water, for example, has a refractive index of 1.33, so light travels at only 75% of its normal speed when in water. Some materials have different refractive indices for two different orientations of plane polarisation because of asymmetries in their crystal structure. The most common such materials are the minerals calcite and mica. In general such materials are called birefringent.

Brewster angle
Circularly polarised light (left) passes through a sheet of birefringent material which slows one component of the polarisation by a quarter of a wavelength, resulting in linearly polarised light, which then passes through a linear polariser. Circularly polarised light of the opposite orientation would be linearised at 90° and then blocked by the linear polariser. Public domain image by Wikipedia user Dave3457, from Wikimedia Commons.
If you pass a beam of light through a birefringent material, the component polarised one way is slowed down by the first refractive index, while the perpendicular component is slowed by the second refractive index. The result is that the two components get out of synch. If they emerge from the material exactly a quarter of a wave out of synch (this is controlled by the thickness of the material), then the resulting components combine to form a spiralling electric field, resulting in circular polarisation. If they're half a wave out of synch the wave is flipped over, and if a full wave out of synch they synch up again, since the waves are periodic. If they are some other fraction out of synch, then the emerging electric field spirals in an elliptical shape instead of a circle, and the result is called elliptical polarisation, which can be considered a mixture of circular and plane polarisation.

The thing with circular polarisation is you can undo it again, with another sheet of the same birefringent material of the same thickness. By retarding one of the components by another quarter wavelength, you synch them back up again, and return to what you began with. This effect is used in 3D movie glasses, which use filters made of a layer of birefringent material followed by a layer of Polaroid. These filter out circularly polarised light by converting it to plane polarised light first, then filtering through the Polaroid. The left and right sides of the glasses filter out circularly polarised light of opposite orientations, so you see the movie image intended for your left eye only with your left eye, and similarly for the right eye. This is superior to using plane polarised light for the two images, because if you tilt your head with plane polarised glasses you will partially mix up the images, whereas this doesn't occur with circularly polarised light.

So that's polarisation in a nutshell. A slightly bigger nutshell than the one Neil deGrasse Tyson gave on Cosmos. Like a coconut to his macadamia, baby!

[1] By the time you read this it will have been a few weeks since that episode premiered, because of my buffer and also the fact that we are getting the episodes in Australia a week after they are being shown in the USA.

[2]"Polaroid" is a trademark of the Polaroid Corporation, and so not strictly the correct generic term for such material. You're probably supposed to call it "polarising plastic material" or something, but everyone I know just calls it Polaroid.

LEGO® is a registered trademark of the LEGO Group of companies, which does not sponsor, authorise, or endorse this site.
This material is presented in accordance with the LEGO® Fair Play Guidelines.

My comics: Irregular Webcomic! | Darths & Droids | Eavesdropper | Planet of Hats | The Dinosaur Whiteboard | mezzacotta
My blogs: (daily updates) | 100 Proofs that the Earth is a Globe (science!) | Carpe DMM (long form posts) | Snot Block & Roll (food reviews)
More comics I host: The Prisoner of Monty Hall | Lightning Made of Owls | Square Root of Minus Garfield | iToons | Comments on a Postcard | Awkward Fumbles
Last Modified: Wednesday, 18 June 2014; 02:00:16 PST.
© 2002-2024 Creative Commons License
This work is copyright and is licensed under a Creative Commons Attribution-Noncommercial-Share Alike 4.0 International Licence by David Morgan-Mar.