Experiments Proving Electromagnetic Waves are Real

In summary: Kinetic energy when the ball is pushed off the step. The EM wave "ball" sits at the top of a step, at the bottom of the step there is an electron. The EM wave "ball" has no obvious energy (it just sits there), but it has, it has potental energy because it converts to...the energy of motion of the electron when the "ball" falls off the step.In summary, an electromagnetic wave is a type of wave that can be observed through various experiments, such as diffraction patterns and interference. It is a spatial and temporal oscillation of the electric and magnetic fields and can be thought of as a wave of potential energy. This concept was first demonstrated in Young's double slit experiment in
  • #1
Moris526
16
0
Electromagnetic wave?

Hi.
Wich experiments show that an electromagnetic wave is a wave?
And what kind of wave? How i think of it? Sure not like a wave on the ocean, there is no ocean there. So?
thanks
 
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  • #2


I'm not understanding your question here. Surely an electromagnetic wave, by definition, is a wave. This is true by definition without proof!

Do you mean instead:
How do we know that electromagnetic waves exist?
 
  • #3


Yes, that´s right defender, how do we know?
 
  • #4


Because our cellphones work. :rolleyes:

And our wi-fi networks, and our microwave ovens, and our radios, and our TVs (at least the ones that don't use cable)...
 
  • #5


We know that an electromagnetic wave is indeed an 'wave' since it shows diffraction patterns. Slits or crystals(depending on the wavelength) can serve as diffraction gratings.

As for your second question, I would say that an electromagnetic wave is a spatial & temporal oscillation of 'the electric and the magnetic field', just as what we usually call 'wave' is a spatial & temporal oscillation of 'the local displacement of the underlying medium'.
The essence of an 'wave' lies in the 'spatial & temporal oscillation' originated from the equation of motion(the wave equation).
 
  • #6


I recommend you read "Schrödinger's Kittens" by John Gribbin. On page 1 he discusses the most famous experiment that demonstrates the wave properties of light - Young's double slit experiment. Imagine two narrow slits in a board, close together. Shine a light on them and you get a pattern of dark and light lines on the screen beyond that can only be explained by assuming light is a wave. The waves coming from both slits interfere (wave peaks sometime coincide, sometimes clash with troughs, leaving the light-dark-light-dark pattern).

http://physics.about.com/od/lightoptics/a/doubleslit.htm

Faraday thought the universe was filled with a material medium (like the ocean!) that carried the lines of force in the electromagnetic field (he invented those concepts as well). He called this "ocean" the plenum. Think of an olympic* rower; he pushes on the water sending a force through the water and rocketing backwards himself. In that way, Faraday thought of force progressing through the plenum. He thought of the plenum as consisting of microscopic objects, like water molecules, which were the fundamental mechanism of force progression (by action/reaction -- Newton' s third law). He considered light to be due to regular (wave-like) motions in the line-ordered force-carrying particles of the plenum. Phew! Take a pretty picture break:

http://www.kettering.edu/~drussell/Demos/waves/wavemotion.html

Now it gets complicated. There is no plenum. Therefore you cannot visualise directly the reality of what is going on. You can imagine water waves easily because you have experienced the material medium of water and the movements in it.

Notice the above responses to your questions mostly point to the visual effects of EM waves (TV picture, diffraction patterns on the screen...) Visualising these is no problem (you can see them!) But how can you visualise the waves directly? How can they be there when there is nothing material to support the waves, you ask? Gribbin suggest the only way is to visualise what is going on with models and analogies (realising that they are, and can only be, models and analogies) and trust in Maxwell's equations to give you the best account of EM waves because they predict the results of experiments (e.g., the exact position of wave peaks in diffraction patterns). Gribbin (p.66) makes this clear.

He suggests you visualise an EM wave through waves in a stretched rope. Remember that a changing electric field generates a magnetic field, and vice versa. Shake the rope so you get vertical ripples, think of that as the electric field. Because it changes it generates a magnetic field, think of that as at right angle to the changing electric field. That, in turn, generates the electric field. The two changing fields march hand in hand, down the "rope". To improve (?) Gribbin's analogy, take away the rope, but keep the ripples. Voila! Electromagnetic waves propagating through the non-material medium of empty space. David Blaine eat your heart out.

Note, as well as trying to visualise waves in a non-existing plenum you also need to visualise fields of force in empty space:

http://en.wikipedia.org/wiki/Field_(physics )

Not an easy task, visualising this stuff. It occupied the best minds in physics between, and including, Faraday and Einstein, before an acceptable picture was cobbled together. Conveying that picture is not easy, and physics teachers need to try harder in conveying it to the uninitiated (as the drop out rate in physics shows!)

P.S. The double-slit experiment also provides the neatest entry into the even greater mysteries of the quantum world. But that's another story -- with good tellings by Gribbin for the layman, and Feynman in his lectures.

* Go Britain!
 
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  • #7


The first really clear indication that electro-magnatism is a wave was the fact the Maxwell's equation for the electric and magnetic fields imply the wave equation.

Though the old SPSS highscnool physics program had a cute experiment on this: A water wave, moving at an angle into an area of lower depth (so slower wave speed) changes direction closer to the normal, obeying Snell's law. A ball (particle) will do that if moves down a slope (so faster speed). Since we know that light moves slower in glass than in vacuum and obeys Snell's law it follows that light has wave properties.

Of course to say something is a "wave" does not necessarily mean it is a wave in any material medium. Light is a wave in the electro-magnetic field.
 
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  • #8


Why was Young's experiment, performed in 1801, not the first "clear indication"?

If the EM field is not a material medium how would you describe it? Here's something i dreamt up, not sure if it holds water (or plenum:-):

Can the EM wave be thought of as a wave of *potential* energy? Can one use a ball on a step as a metaphor? The ball on the step has no obvious energy (it just sits there), but it has, it has potental energy because it converts to obvious (kinetic) energy on falling off the step. With the EM wave it does nothing until it "hits" the radio mast, so its all potential energy up until that point. Just as the potential energy of the ball obviously needs no material foundation, neither does the EM wave or field.
 
  • #9


mal4mac said:
Why was Young's experiment, performed in 1801, not the first "clear indication"?

Young's experiment indicated that light had to be a wave phenomenon, but it didn't indicate anything about the nature of the wave. At that time the concepts of electric and magnetic fields hadn't even been developed (except perhaps in a very vague sense), let alone been connected to light.

It wasn't until the 1860s that Maxwell derived the wave equation for electric and magnetic fields, calculated the speed of electromagnetic waves from measurements of electric and magnetic constants, and noticed that that speed equals the measured speed of light within experimental accuracy.
 
  • #10


The first real experimental evidence that showed the existence of Maxwell's electromagnetic waves was provided by Heinrich Hertz in 1887.

He set up a coil-driven spark generator to radiate radio waves (which at the time was just considered invisible radiation), and used a circular antenna to receive them. Using Maxwell's theory, he deduced that this radiation consisted of electric and magnetic fields. He also demonstrated that this radiation could be reflected, polarised and produce interference, which are inherent properties of waves. Futhermore, he measured the speed of the radio wave to be similar to what Maxwell had predicted for light.

Wikipedia quote:

"It's of no use whatsoever[...] this is just an experiment that proves Maestro Maxwell was right - we just have these mysterious electromagnetic waves that we cannot see with the naked eye. But they are there."
 
  • #11
jtbell said:
Young's experiment indicated that light had to be a wave phenomenon, but it didn't indicate anything about the nature of the wave. At that time the concepts of electric and magnetic fields hadn't even been developed (except perhaps in a very vague sense), let alone been connected to light.

Good points. But Moris asked "Which experiments show that an electromagnetic wave is a wave?" He didn't say "*all* electromagnetic waves or *except light*. So I think 'Young's experiment' was a valid answer, without more input from Moris.

jtbell said:
It wasn't until the 1860s that Maxwell derived the wave equation for electric and magnetic fields, calculated the speed of electromagnetic waves from measurements of electric and magnetic constants, and noticed that that speed equals the measured speed of light within experimental accuracy.

But that's a theory. Moris was asking for an *experiment*. The following is quite useful on the history:

http://www-gap.dcs.st-and.ac.uk/~history/Projects/Johnson/Chapters/Ch4_4.html

"In 1887, Hertz finally achieved the sought after experimental confirmation."

Found this after a quick Google search:

http://people.seas.harvard.edu/~jones/cscie129/nu_lectures/lecture6/hertz/Hertz_exp.html

It would a good school project to repeat this experiment.
 
  • #12


Yeah, Young's double slit is the answer. Interference and diffraction.

You can also take Maxwell's equations and show that E and B must satisfy the linear wave equation, implying they are waves.
 
  • #13


What is most confusing here, is why electromagnetic waves are transverse, which I cannot understand. Is it really that they are transverse in space, that is, when a light ray beams at my eye, it travels through the air as a wave with a physical extension in the z-direction (if the light ray travels horizontally to me, and z is in the up-direction)?

Also, I cannot sea how any of the experiments here explain why the wave is transverse. The experiment with interference is for me that they could be as well be only longitudinal. At least, it is not explained in a way that is easy to understand... Is there an experiment that proves the transverse nature of the EM waves, with sort of high pedagogical power?
 
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  • #14


Mårten said:
Is there an experiment that proves the transverse nature of the EM waves, with sort of high pedagogical power?

The existence of polarized light proves that EM waves are transverse. Polarization is impossible with a longitudinal wave.
 
  • #15


Thomas Young explained polarisation as well! Got me to thinking if there was a biography about him. Turns out there is, with the longest & most descriptive title I've ever seen!

"The Last Man Who Knew Everything: Thomas Young, the Anonymous Polymath Who Proved Newton Wrong, Explained How We See, Cured the Sick, and Deciphered the Rosetta Stone, Among Other Feats of Genius" by Andrew Robinson

Simon Singh provides a great review of this book (I accessed it from http://en.wikipedia.org/wiki/Thomas_Young_(scientist )), recounting how Young 'might have been' inspired to invent the ripple tank to demonstrate interference in water waves:

"When I was a student at Emmanuel College, Cambridge, where Young also studied, I was told that this demonstration was inspired by the college's famous duck pond. The story goes that Young saw two ducks swimming side by side, leaving behind a complex pattern of interference from the two sets of water waves."
 
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  • #16


jtbell said:
The existence of polarized light proves that EM waves are transverse. Polarization is impossible with a longitudinal wave.

Okey, I'm satisfied with that when it comes to the transverse nature. I'll go and study polarization then.

But still - what kind of transverse are we talking about here? Are the waves really a wave in space, with, as I asked above, a physical extension in z-direction? So that you can say that, if the wave has an amplitude of 1 nm, then the wave actually goes up 1 nm on the hills of the wave, and down 1 nm in the vallyes of the wave?

Interesting about Young however! And the wavemotion link was very useful! :smile:
 
  • #18


Mårten said:
what kind of transverse are we talking about here? Are the waves really a wave in space, with, as I asked above, a physical extension in z-direction? So that you can say that, if the wave has an amplitude of 1 nm, then the wave actually goes up 1 nm on the hills of the wave, and down 1 nm in the vallyes of the wave?

No, what is oscillating are the magnitudes of the electric and magnetic fields at a given point (measured in volts/meter and tesla respectively), not displacements in position. Maybe I can find the diagram I attached to a posting here a couple of years ago... ah, here it is, in this post.
 
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  • #20


jtbell said:
No, what is oscillating are the amplitudes of the electric and magnetic fields at a given point (measured in volts/meter and tesla respectively), not displacements in position. Maybe I can find the diagram I attached to a posting here a couple of years ago... ah, here it is, in this post.

Waoh! This is a revolution for me. :smile: Why have all my physics teachers deceived me on this point? :mad:

Follow-up: Since the E-field describes the force per unit charge in each point, you could say this is just the property that the z-axis describes, just as pressure in air is the property which the z-axis describes when plotting the propagation of sound (but sound is a longitudinal wave). So what's really the difference then in form between a sound wave and an EM wave?
 
  • #22


Mårten said:
Since the E-field describes the force per unit charge in each point, you could say this is just the property that the z-axis describes

Right, except that it's the y-axis in my diagram. If you put a small test charge at some location, it experiences an oscillating electric force parallel to the y-axis.

So what's really the difference then in form between a sound wave and an EM wave?

What do you mean by "difference in form"?
 
  • #23


jtbell said:
What do you mean by "difference in form"?

I meant transverse form or longitudinal form. I mean, a sound wave can be thought of as transverse, if you plot it mathematically with time (or distance) on x-axis, and pressure on y-axis. Same for an EM wave, time (or distance) on x-axis and electric field on y-axis. So that's not much difference really. For every point on the x-axis, we have a property associated: pressure, or electric field strength. So why call one of them longitudinal and one of them transverse?
 
  • #24


The form of the graphs of the two waves are similar as we normally draw them. But those graphs are only abstract representations of the physical phenomena. In an electromagnetic wave the electric and magnetic fields are actually transverse to the direction of propagation of the wave; and in a sound wave in air, the oscillating motion of the molecules is actually parallel (longitudinal) to the direction of propagation of the wave.
 
  • #25


transverse sound waves don't use pressure. the motion of the particles is transverse (90 degrees) to the motion of the wave. it requires a material that resists shear forces. in other words, a solid.
 
  • #26


hdunham said:
Yeah, Young's double slit is the answer. Interference and diffraction.

You can also take Maxwell's equations and show that E and B must satisfy the linear wave equation, implying they are waves.

It's interesting that this is taken as a validation of the wave character of light. Taking one more derivative obtains a longitudinal wave equation in charge and current density.

Yet this nonphysical result is not touted about as an invalidation of Maxwell's equations, and by inheritance, noncomfirmation of the wave equation of light.
 
  • #27


maybe that should be a new thread.
 
  • #28


Mårten said:
Is it really that they are transverse in space...

jtbell said:
No, what is oscillating are the amplitudes of the electric and magnetic fields at a given point (measured in volts/meter and tesla respectively), not displacements in position.

Being pedantic, amplitude is "the maximum displacement of a periodic wave" [Princeton wordnet], therefore you can't strictly define it at a "point", can you? Also the field concept is tricky. In sum might it be better to say, "what is oscillating are the *magnitudes* of the electric and magnetic *forces* at a given point"?

I like this idea of tieing the visualisation down to one point and seeing what the E/B is doing at that point. I find it difficult visualising *clearly* anything that is going on in more than two dimensions. Although I can add time as a third dimension and see the E/B fields going up/ sideways at the point as little arrows that grow and diminish.

Don't be too hard on your teachers Mårten, this concept is often introduced using the wave on a skipping rope metaphor, as that's a more concrete example for people to understand than a regular oscillation of a magnitude at a point. (Gribbin uses it in his "kittens" book).
 
  • #29


jtbell said:
The form of the graphs of the two waves are similar as we normally draw them. But those graphs are only abstract representations of the physical phenomena. In an electromagnetic wave the electric and magnetic fields are actually transverse to the direction of propagation of the wave; and in a sound wave in air, the oscillating motion of the molecules is actually parallel (longitudinal) to the direction of propagation of the wave.

You mean transverse in the meaning - and nothing else - that the vectors of the E-field points 90 degrees in relation to the wave propagation?

My problem here, is that for the sound wave, we have actual molecules oscillating back and forth parallell to the propagation of the wave. But for the EM wave we don't have anything that concrete. The E-field is also abstract (I thought at least). It doesn't really exist until you have a test charge which can be affected by it. In that sense, as I have understodd it so far, your drawing of the EM wave is also just an abstract representation. And as such, it is transverse in the same meaning as a sound wave is, i.e. their abstract representations is transverse, they both form sine waves. I think actually, the EM wave can never be viewed in a non-abstract way as the sound wave can be.

That's just my current understanding of the whole thing - please correct me for all erroneous assumptions I've made...
 
  • #30


why would anybody compare a transverse EM wave to a longitudinal sound wave. why not to a transverse sound wave.

EM waves are considered to be transverse because they can be polarized.
 
  • #31


jtbell said:
But those graphs are only abstract representations of the physical phenomena. In an electromagnetic wave the electric and magnetic fields are actually transverse to the direction of propagation of the wave; and in a sound wave in air, the oscillating motion of the molecules is actually parallel (longitudinal) to the direction of propagation of the wave.

But surely EM waves are less actual than sound waves? Sound waves are waves in physical matter (air molecules). EM waves are ... er... not.
 
  • #32


mal4mac said:
Being pedantic, amplitude is "the maximum displacement of a periodic wave" [Princeton wordnet], therefore you can't strictly define it at a "point", can you? Also the field concept is tricky. In sum might it be better to say, "what is oscillating are the *magnitudes* of the electric and magnetic *forces* at a given point"?
Ah, exactly how I look upon it. Therefore, that magnitude is like any other magnitude of some other property, e.g. pressure.

mal4mac said:
Don't be too hard on your teachers Mårten, this concept is often introduced using the wave on a skipping rope metaphor, as that's a more concrete example for people to understand than a regular oscillation of a magnitude at a point. (Gribbin uses it in his "kittens" book).
Hrm... I think that's just the kind of analogies one should avoid. Better to make an analogy with the sound waves then. And then, in a later stage draw the distinction between transverse and longitudinal waves. A distinction which, when it comes to light, I haven't understood yet, as this is the subject of this thread...

granpa said:
why would anybody compare a transverse EM wave to a longitudinal sound wave. why not to a transverse sound wave.
But the transverse sound wave makes physical extensions in the transverse direction, like waves on water - that's not the case for EM waves, is it?
 
  • #33


Mårten said:
But the transverse sound wave makes physical extensions in the transverse direction, like waves on water - that's not the case for EM waves, is it?

how much of an extension in the transverse direction do you think a transverse sound wave makes when moving through solid rock?
 
  • #34


mal4mac said:
jtbell said:
No, what is oscillating are the amplitudes of the electric and magnetic fields
Being pedantic, amplitude is "the maximum displacement of a periodic wave"

Oops, you're right. I meant "magnitude" as in "magnitude of a vector." I've corrected my original post. Thanks for catching this. :blushing:

(Of course, the directions of [itex]\vec E[/itex] and [itex]\vec B[/itex] also oscillate, or rather, flip-flop.)
 
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  • #35


Mårten said:
jtbell said:
In an electromagnetic wave the electric and magnetic fields are actually transverse to the direction of propagation of the wave;
You mean transverse in the meaning - and nothing else - that the vectors of the E-field points 90 degrees in relation to the wave propagation?

Yes.

Mårten said:
My problem here, is that for the sound wave, we have actual molecules oscillating back and forth parallell to the propagation of the wave. But for the EM wave we don't have anything that concrete. The E-field is also abstract (I thought at least). It doesn't really exist until you have a test charge which can be affected by it.

mal4mac said:
But surely EM waves are less actual than sound waves?

I think most physicists take the view that E- and B- fields are "real" in some sense, and exist independently of the real or imaginary test charges that we use for observing them. It's also possible to take the view that the fields are merely mathematical devices for simplifying the calculation of what is ultimately a complicated "action at a distance" of some kind. It's impossible to distinguish between these two interpretations experimentally, so the choice is a matter of personal preference and philosophy, and depends on exactly what one means by "real." People can and do debate such things endlessly. I get bored with it pretty quickly, myself. :smile:

If you have problems like this with the classical electromagnetic field, just wait until you get to quantum mechanics! In the Quantum Physics forum, people go at each other with hammer and tongs over questions of interpretation. :biggrin:
 
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