Not understanding some parts of wave refraction
I am skimming thru the Propagation chapter of the ARRL handbook, and I
am having a difficult time understanding the shortening of wavelength and the retainment of frequency. They have an equation showing that wave velocity is: c = f*w (c = m/s, f = frequency, w = wavelength). It also states that during refraction "the wavelength is simultaneously shortened, but the wave frequency (number of crests that pass a certain point in a given unit of time) remains constant." I don't understand. If the wavelength is shortened, then shouldn't the frequency increase instead of remaining constant? |
Not understanding some parts of wave refraction
On 5 Apr 2007 07:36:49 -0700, "MRW" wrote:
c = f*w (c = m/s, f = frequency, w = wavelength) This frequency is relevant ONLY for vacuum (or with a very, very slight alteration) air. Now, it may seem that all air is air, but no. There are slight variations here too that on the global scale small shifts make large changes. Those small shifts are accounted for by pressure, water content (vapor), and temperature. 73's Richard Clark, KB7QHC |
Not understanding some parts of wave refraction
On Apr 5, 7:36 am, "MRW" wrote:
I am skimming thru the Propagation chapter of the ARRL handbook, and I am having a difficult time understanding the shortening of wavelength and the retainment of frequency. They have an equation showing that wave velocity is: c = f*w (c = m/s, f = frequency, w = wavelength). It also states that during refraction "the wavelength is simultaneously shortened, but the wave frequency (number of crests that pass a certain point in a given unit of time) remains constant." I don't understand. If the wavelength is shortened, then shouldn't the frequency increase instead of remaining constant? Refraction occurs when an EM wave, having frequency f and wavelength w enters a medium in which the speed of propagation (speed of light) is different than vacuum. A medium with an index of refraction greater than one produces a speed of light which is slower than in vacuum (index of refraction is simply the ratio of vacuum speed to speed in that medium). This changes the proportionality between frequency and wavelength. Since w = c / f, the slower speed at a given frequency will now have a correspondingly shorter wavelength. And, as f = c / w, the slower speed at a given wavelength will now have a correspondingly lower frequency. I hope that makes sense. 73, Jim AC6XG |
Not understanding some parts of wave refraction
MRW wrote:
I am skimming thru the Propagation chapter of the ARRL handbook, and I am having a difficult time understanding the shortening of wavelength and the retainment of frequency. They have an equation showing that wave velocity is: c = f*w (c = m/s, f = frequency, w = wavelength). It also states that during refraction "the wavelength is simultaneously shortened, but the wave frequency (number of crests that pass a certain point in a given unit of time) remains constant." I don't understand. If the wavelength is shortened, then shouldn't the frequency increase instead of remaining constant? 'c' decreases because of the fractional velocity factor in a transmission line. The decrease in 'c' compresses the wavelength but doesn't change the frequency. 'c' is less in a transmission line than it is in free space. The speed of light in RG-213, for instance, is 2/3 of the speed of light in free space. -- 73, Cecil, w5dxp.com |
Not understanding some parts of wave refraction
MRW wrote:
I am skimming thru the Propagation chapter of the ARRL handbook, and I am having a difficult time understanding the shortening of wavelength and the retainment of frequency. They have an equation showing that wave velocity is: c = f*w (c = m/s, f = frequency, w = wavelength). It also states that during refraction "the wavelength is simultaneously shortened, but the wave frequency (number of crests that pass a certain point in a given unit of time) remains constant." I don't understand. If the wavelength is shortened, then shouldn't the frequency increase instead of remaining constant? frequency stays the same, but since it's moving slower, c is smaller, so lambda (wavelength) is shorter. Same thing goes on in coaxial cable.. the wave propagates in a dielectric with a propagation speed, say, 66% of the free space speed. In such a case, a one wavelength long piece of coax for 30 MHz is 6.6 meters, not 10 meters (the free space wavelength) The challenge, of course, would be in getting the opposite phenomenon to occur (propagation faster than free space)...but that's a topic for a different day. jim |
Not understanding some parts of wave refraction
On Thu, 05 Apr 2007 09:23:13 -0700, Jim Lux wrote:
MRW wrote: I am skimming thru the Propagation chapter of the ARRL handbook, and I am having a difficult time understanding the shortening of wavelength and the retainment of frequency. They have an equation showing that wave velocity is: c = f*w (c = m/s, f = frequency, w = wavelength). It also states that during refraction "the wavelength is simultaneously shortened, but the wave frequency (number of crests that pass a certain point in a given unit of time) remains constant." I don't understand. If the wavelength is shortened, then shouldn't the frequency increase instead of remaining constant? frequency stays the same, but since it's moving slower, c is smaller, so lambda (wavelength) is shorter. Same thing goes on in coaxial cable.. the wave propagates in a dielectric with a propagation speed, say, 66% of the free space speed. In such a case, a one wavelength long piece of coax for 30 MHz is 6.6 meters, not 10 meters (the free space wavelength) The challenge, of course, would be in getting the opposite phenomenon to occur (propagation faster than free space)...but that's a topic for a different day. jim Speedy Gozales did it, but that's also a topic for a different day. Walt, W2DU |
Not understanding some parts of wave refraction
On Apr 5, 7:36 am, "MRW" wrote:
I am skimming thru the Propagation chapter of the ARRL handbook, and I am having a difficult time understanding the shortening of wavelength and the retainment of frequency. They have an equation showing that wave velocity is: c = f*w (c = m/s, f = frequency, w = wavelength). It also states that during refraction "the wavelength is simultaneously shortened, but the wave frequency (number of crests that pass a certain point in a given unit of time) remains constant." I don't understand. If the wavelength is shortened, then shouldn't the frequency increase instead of remaining constant? Others have posted, correctly, that the propagation velocity is slower in some mediums than in others. I think it's a mistake, though, to say that c changes! c is supposed to be a constant, the speed of electromagnetic wave propagation in a vacuum--in fact, I suppose, in a vacuum with no gravitational fields in it. A description of fields in an electromagnetic wave often used the permittivity, epsilon, and permeability, mu, of the medium through which the wave is travelling. If it's through a vacuum, the values of epsilon and mu have values that are used often and have special notation--epsilon-sub-zero and mu- sub-zero. For convenience here, call them eo and uo. Then note that eo*uo = 1/c^2. As you might suspect, the propagation in a medium with larger values of e and u than eo and uo is slower than c. In fact, it should be velocity = sqrt(1/(e*u)). Note that e has the units of capacitance/length -- commonly farads/ meter -- and u has the units of inductance/length -- commonly henries/ meter. But a farad is an ampere*second/volt, and a henry is a volt*second/amp, so the units of sqrt(1/(e*u)) are sqrt(1/((A*sec/ V*meter)*(V*sec/A*meter))) = sqrt(meter^2/sec^2) = meters/sec. A unit analysis is often useful to insure you haven't made a mistake in your manipulation of equations. So...in summary, c = f*w is actually not quite correct. It should be wave_velocity = f*w. c should be reserved to mean only the speed of light in a vacuum. If you're in a non-vacuum medium, and measure very accurately, you'll measure the same frequency, but a shorter wavelength: the wave doesn't travel as far to push a cycle past you, as compared with in vacuum. It's going slower. If the propagation medium is, for example, solid polyethylene (the dielectric of most inexpensive coax cable), you'll find that w is about 0.66 times as much as it is in a vacuum, and the propagation velocity is similarly 0.66*c. Cheers, Tom |
Not understanding some parts of wave refraction
On Apr 5, 1:44 pm, "K7ITM" wrote:
Others have posted, correctly, that the propagation velocity is slower in some mediums than in others. I think it's a mistake, though, to say that c changes! c is supposed to be a constant, the speed of electromagnetic wave propagation in a vacuum--in fact, I suppose, in a vacuum with no gravitational fields in it. A description of fields in an electromagnetic wave often used the permittivity, epsilon, and permeability, mu, of the medium through which the wave is travelling. If it's through a vacuum, the values of epsilon and mu have values that are used often and have special notation--epsilon-sub-zero and mu- sub-zero. For convenience here, call them eo and uo. Then note that eo*uo = 1/c^2. As you might suspect, the propagation in a medium with larger values of e and u than eo and uo is slower than c. In fact, it should be velocity = sqrt(1/(e*u)). Note that e has the units of capacitance/length -- commonly farads/ meter -- and u has the units of inductance/length -- commonly henries/ meter. But a farad is an ampere*second/volt, and a henry is a volt*second/amp, so the units of sqrt(1/(e*u)) are sqrt(1/((A*sec/ V*meter)*(V*sec/A*meter))) = sqrt(meter^2/sec^2) = meters/sec. A unit analysis is often useful to insure you haven't made a mistake in your manipulation of equations. So...in summary, c = f*w is actually not quite correct. It should be wave_velocity = f*w. c should be reserved to mean only the speed of light in a vacuum. If you're in a non-vacuum medium, and measure very accurately, you'll measure the same frequency, but a shorter wavelength: the wave doesn't travel as far to push a cycle past you, as compared with in vacuum. It's going slower. If the propagation medium is, for example, solid polyethylene (the dielectric of most inexpensive coax cable), you'll find that w is about 0.66 times as much as it is in a vacuum, and the propagation velocity is similarly 0.66*c. Cheers, Tom Thank you everyone! I have a better understanding now. I guess part of my confusion is that on the same chapter thay have a table on the electromagnetic spectrum. In it, they list Radio Waves as having frquencies between 10kHz to 300Ghz and wavelengths of 30,000km to 1mm (I guess the 30,000 km is a typo in the book). Are these wavelength values based in a vacuum then? |
Not understanding some parts of wave refraction
K7ITM wrote: On Apr 5, 7:36 am, "MRW" wrote: I am skimming thru the Propagation chapter of the ARRL handbook, and I am having a difficult time understanding the shortening of wavelength and the retainment of frequency. They have an equation showing that wave velocity is: c = f*w (c = m/s, f = frequency, w = wavelength). It also states that during refraction "the wavelength is simultaneously shortened, but the wave frequency (number of crests that pass a certain point in a given unit of time) remains constant." I don't understand. If the wavelength is shortened, then shouldn't the frequency increase instead of remaining constant? Others have posted, correctly, that the propagation velocity is slower in some mediums than in others. I think it's a mistake, though, to say that c changes! c is supposed to be a constant, the speed of electromagnetic wave propagation in a vacuum--in fact, I suppose, in a vacuum with no gravitational fields in it. A description of fields in an electromagnetic wave often used the permittivity, epsilon, and permeability, mu, of the medium through which the wave is travelling. If it's through a vacuum, the values of epsilon and mu have values that are used often and have special notation--epsilon-sub-zero and mu- sub-zero. For convenience here, call them eo and uo. Then note that eo*uo = 1/c^2. As you might suspect, the propagation in a medium with larger values of e and u than eo and uo is slower than c. In fact, it should be velocity = sqrt(1/(e*u)). Note that e has the units of capacitance/length -- commonly farads/ meter -- and u has the units of inductance/length -- commonly henries/ meter. But a farad is an ampere*second/volt, and a henry is a volt*second/amp, so the units of sqrt(1/(e*u)) are sqrt(1/((A*sec/ V*meter)*(V*sec/A*meter))) = sqrt(meter^2/sec^2) = meters/sec. A unit analysis is often useful to insure you haven't made a mistake in your manipulation of equations. So...in summary, c = f*w is actually not quite correct. It should be wave_velocity = f*w. c should be reserved to mean only the speed of light in a vacuum. If you're in a non-vacuum medium, and measure very accurately, you'll measure the same frequency, but a shorter wavelength: the wave doesn't travel as far to push a cycle past you, as compared with in vacuum. It's going slower. If the propagation medium is, for example, solid polyethylene (the dielectric of most inexpensive coax cable), you'll find that w is about 0.66 times as much as it is in a vacuum, and the propagation velocity is similarly 0.66*c. Cheers, Tom Hi Tom - That's certainly one way to look at it. (Though it is a little like saying there is only one speed of sound.) Another way is to say that c = 1/root(mu*epsilon) for any media. Light does after all, always travel at the speed of light. ;-) Besides, it's more difficult to explain Cherenkov radiation without the expression 'faster than the speed of light in that medium'. I thoroughly enjoyed the discussion you and Owen were (are) having regarding amplifiers. Thank you for that. 73, Jim AC6XG |
Not understanding some parts of wave refraction
On Apr 5, 11:56 am, "Jim Kelley" wrote:
K7ITM wrote: On Apr 5, 7:36 am, "MRW" wrote: I am skimming thru the Propagation chapter of the ARRL handbook, and I am having a difficult time understanding the shortening of wavelength and the retainment of frequency. They have an equation showing that wave velocity is: c = f*w (c = m/s, f = frequency, w = wavelength). It also states that during refraction "the wavelength is simultaneously shortened, but the wave frequency (number of crests that pass a certain point in a given unit of time) remains constant." I don't understand. If the wavelength is shortened, then shouldn't the frequency increase instead of remaining constant? Others have posted, correctly, that the propagation velocity is slower in some mediums than in others. I think it's a mistake, though, to say that c changes! c is supposed to be a constant, the speed of electromagnetic wave propagation in a vacuum--in fact, I suppose, in a vacuum with no gravitational fields in it. A description of fields in an electromagnetic wave often used the permittivity, epsilon, and permeability, mu, of the medium through which the wave is travelling. If it's through a vacuum, the values of epsilon and mu have values that are used often and have special notation--epsilon-sub-zero and mu- sub-zero. For convenience here, call them eo and uo. Then note that eo*uo = 1/c^2. As you might suspect, the propagation in a medium with larger values of e and u than eo and uo is slower than c. In fact, it should be velocity = sqrt(1/(e*u)). Note that e has the units of capacitance/length -- commonly farads/ meter -- and u has the units of inductance/length -- commonly henries/ meter. But a farad is an ampere*second/volt, and a henry is a volt*second/amp, so the units of sqrt(1/(e*u)) are sqrt(1/((A*sec/ V*meter)*(V*sec/A*meter))) = sqrt(meter^2/sec^2) = meters/sec. A unit analysis is often useful to insure you haven't made a mistake in your manipulation of equations. So...in summary, c = f*w is actually not quite correct. It should be wave_velocity = f*w. c should be reserved to mean only the speed of light in a vacuum. If you're in a non-vacuum medium, and measure very accurately, you'll measure the same frequency, but a shorter wavelength: the wave doesn't travel as far to push a cycle past you, as compared with in vacuum. It's going slower. If the propagation medium is, for example, solid polyethylene (the dielectric of most inexpensive coax cable), you'll find that w is about 0.66 times as much as it is in a vacuum, and the propagation velocity is similarly 0.66*c. Cheers, Tom Hi Tom - That's certainly one way to look at it. (Though it is a little like saying there is only one speed of sound.) Another way is to say that c = 1/root(mu*epsilon) for any media. Light does after all, always travel at the speed of light. ;-) Besides, it's more difficult to explain Cherenkov radiation without the expression 'faster than the speed of light in that medium'. I thoroughly enjoyed the discussion you and Owen were (are) having regarding amplifiers. Thank you for that. 73, Jim AC6XG Hi Jim, Some people may use only c-sub-zero for the speed of light in a vacuum, but most commonly I see it simply as c, a fundamental physical constant. To avoid confusion, I would HIGHLY recommend that either you be very explicit that you're using co as the constant, and c as the speed of light in whatever medium you're dealing with -- OR that you're using c as the constant and whatever other notation for the speed elsewhere. NIST lists the constant both ways: c, c-sub-zero. SEVERAL other places I just looked (reference books from my bookshelf; a web survey including US, UK and European sites--mostly physics sites; several university sites) only used c as the constant, except the NIST site and one other, which both listed it as c or c-sub-zero with equal weight. It's clearly a matter only of notation, but I'll elect to stay with the most commonly used notation, and from what I've seen just now, most think c is a constant. Cheers, Tom |
Not understanding some parts of wave refraction
On Apr 5, 11:33 am, "MRW" wrote:
On Apr 5, 1:44 pm, "K7ITM" wrote: Others have posted, correctly, that the propagation velocity is slower in some mediums than in others. I think it's a mistake, though, to say that c changes! c is supposed to be a constant, the speed of electromagnetic wave propagation in a vacuum--in fact, I suppose, in a vacuum with no gravitational fields in it. A description of fields in an electromagnetic wave often used the permittivity, epsilon, and permeability, mu, of the medium through which the wave is travelling. If it's through a vacuum, the values of epsilon and mu have values that are used often and have special notation--epsilon-sub-zero and mu- sub-zero. For convenience here, call them eo and uo. Then note that eo*uo = 1/c^2. As you might suspect, the propagation in a medium with larger values of e and u than eo and uo is slower than c. In fact, it should be velocity = sqrt(1/(e*u)). Note that e has the units of capacitance/length -- commonly farads/ meter -- and u has the units of inductance/length -- commonly henries/ meter. But a farad is an ampere*second/volt, and a henry is a volt*second/amp, so the units of sqrt(1/(e*u)) are sqrt(1/((A*sec/ V*meter)*(V*sec/A*meter))) = sqrt(meter^2/sec^2) = meters/sec. A unit analysis is often useful to insure you haven't made a mistake in your manipulation of equations. So...in summary, c = f*w is actually not quite correct. It should be wave_velocity = f*w. c should be reserved to mean only the speed of light in a vacuum. If you're in a non-vacuum medium, and measure very accurately, you'll measure the same frequency, but a shorter wavelength: the wave doesn't travel as far to push a cycle past you, as compared with in vacuum. It's going slower. If the propagation medium is, for example, solid polyethylene (the dielectric of most inexpensive coax cable), you'll find that w is about 0.66 times as much as it is in a vacuum, and the propagation velocity is similarly 0.66*c. Cheers, Tom Thank you everyone! I have a better understanding now. I guess part of my confusion is that on the same chapter thay have a table on the electromagnetic spectrum. In it, they list Radio Waves as having frquencies between 10kHz to 300Ghz and wavelengths of 30,000km to 1mm (I guess the 30,000 km is a typo in the book). Are these wavelength values based in a vacuum then? Clearly, the definition for the frequency range is somewhat arbitrary. The boundary between infra-red and radio waves will probably continue to be blurred as electronics advances further. Radio waves down to much lower frequencies than 10kHz have been used...the longer wavelengths penetrate water further, and are useful for communicating with submarines. So don't be surprised if you come across references to radio signals at 50Hz or so. Because communications with radio waves is almost always based on propagation through the vacuum of space, or through air which is only very slightly slower, yes, the values for wavelength are based on c being a constant, the speed of light in a vacuum. Once you figure out one wavelength-frequency relationship, decade (power-of-ten) values are easy: 1MHz = 300 meters (actually 299.792458, but almost universally taken to be 300...) 10MHz = 30 meters 100MHz = 3 meters etc... Cheers, Tom |
Not understanding some parts of wave refraction
K7ITM wrote: Hi Jim, Some people may use only c-sub-zero for the speed of light in a vacuum, but most commonly I see it simply as c, a fundamental physical constant. To avoid confusion, I would HIGHLY recommend that either you be very explicit that you're using co as the constant, and c as the speed of light in whatever medium you're dealing with -- OR that you're using c as the constant and whatever other notation for the speed elsewhere. NIST lists the constant both ways: c, c-sub-zero. SEVERAL other places I just looked (reference books from my bookshelf; a web survey including US, UK and European sites--mostly physics sites; several university sites) only used c as the constant, except the NIST site and one other, which both listed it as c or c-sub-zero with equal weight. It's clearly a matter only of notation, but I'll elect to stay with the most commonly used notation, and from what I've seen just now, most think c is a constant. Cheers, Tom Hi Tom - This is becoming circuitous. What you're saying is exactly what led the original correspondent to be confused in the first place. Since the relavant equation doesn't read c = f*w/n, the only way to explain the phenomenon is by using a value of c that varies with medium. That was the entire point. 73. Jim AC6XG |
Not understanding some parts of wave refraction
K7ITM wrote:
It's clearly a matter only of notation, but I'll elect to stay with the most commonly used notation, and from what I've seen just now, most think c is a constant. That's why I put it in quotes - to signify an unusual notation. -- 73, Cecil, w5dxp.com |
Not understanding some parts of wave refraction
MRW wrote:
Thank you everyone! I have a better understanding now. I guess part of my confusion is that on the same chapter thay have a table on the electromagnetic spectrum. In it, they list Radio Waves as having frquencies between 10kHz to 300Ghz and wavelengths of 30,000km to 1mm (I guess the 30,000 km is a typo in the book). Are these wavelength values based in a vacuum then? Yes. And it's very, very nearly the same for air. The 30,000 km would be a typo -- the wavelength in a vacuum at 10 kHz would be 30 km. Roy Lewallen, W7EL |
Not understanding some parts of wave refraction
On Apr 5, 1:14 pm, Jim Kelley wrote:
K7ITM wrote: Hi Jim, Some people may use only c-sub-zero for the speed of light in a vacuum, but most commonly I see it simply as c, a fundamental physical constant. To avoid confusion, I would HIGHLY recommend that either you be very explicit that you're using co as the constant, and c as the speed of light in whatever medium you're dealing with -- OR that you're using c as the constant and whatever other notation for the speed elsewhere. NIST lists the constant both ways: c, c-sub-zero. SEVERAL other places I just looked (reference books from my bookshelf; a web survey including US, UK and European sites--mostly physics sites; several university sites) only used c as the constant, except the NIST site and one other, which both listed it as c or c-sub-zero with equal weight. It's clearly a matter only of notation, but I'll elect to stay with the most commonly used notation, and from what I've seen just now, most think c is a constant. Cheers, Tom Hi Tom - This is becoming circuitous. What you're saying is exactly what led the original correspondent to be confused in the first place. Since the relavant equation doesn't read c = f*w/n, the only way to explain the phenomenon is by using a value of c that varies with medium. That was the entire point. 73. Jim AC6XG Hi Jim, OK, but I still say that, in that case, the equation (c=f*w) uses c in a way that's inconsistent with common usage of c. I don't know if the article quoted by the OP mentions that, or if somewhere it adds other qualification, but if it's not out of context, then it would confuse me, too, if I were trying to understand it for the first time. At the very least, the article should say somewhere that c is the speed of propagation in whatever medium we're dealing with, and if it did, perhaps the OP wouldn't have been confused about it in the first place. His posting makes it very clear to me that HE thought c was a constant, as I would if the author didn't tell me otherwise. Cheers, Tom |
Not understanding some parts of wave refraction
On 5 Apr 2007 18:15:30 -0700, "K7ITM" wrote:
HE thought c was a constant, as I would if the author didn't tell me otherwise. Hi Tom, The speed of light is always constant - within its frame of reference. It is only for those that inhabit a different frame that it "appears" to be different. By Lorentzian laws, there is no time at the speed of light and everything is simultaneous - source and load are inseparable. To illustrate at a slightly slower speed (from Feynman): "A very interesting example of the slowing of time with motion is furnished mu-mesons (muons), which are particles that disintegrate spontaneously after an average lifetime of 2.2 µS. They come to earth in cosmic rays.... It is clear that in its short lifetime a muon cannot travel, even at the speed of light, much more than 600 meters. But although the muons are created at the top of the atmosphere, some 10 kilometers up, yet they are actually found in a laboratory down here, in cosmic rays. How can that be? The answer is that .... While from OUR own point of view they live considerably longer ... time is increased ... by 1/SQRT(1-(u²/v²))." 73's Richard Clark, KB7QHC |
Not understanding some parts of wave refraction
Richard Clark wrote:
While from OUR own point of view they live considerably longer ... time is increased ... by 1/SQRT(1-(u²/v²))." I wonder what that implies about the alleged age of the universe? -- 73, Cecil http://www.w5dxp.com |
Not understanding some parts of wave refraction
On Apr 6, 12:08 am, Richard Clark wrote:
On 5 Apr 2007 18:15:30 -0700, "K7ITM" wrote: HE thought c was a constant, as I would if the author didn't tell me otherwise. Hi Tom, The speed of light is always constant - within its frame of reference. It is only for those that inhabit a different frame that it "appears" to be different. By Lorentzian laws, there is no time at the speed of light and everything is simultaneous - source and load are inseparable. To illustrate at a slightly slower speed (from Feynman): "A very interesting example of the slowing of time with motion is furnished mu-mesons (muons), which are particles that disintegrate spontaneously after an average lifetime of 2.2 µS. They come to earth in cosmic rays.... It is clear that in its short lifetime a muon cannot travel, even at the speed of light, much more than 600 meters. But although the muons are created at the top of the atmosphere, some 10 kilometers up, yet they are actually found in a laboratory down here, in cosmic rays. How can that be? The answer is that .... While from OUR own point of view they live considerably longer ... time is increased ... by 1/SQRT(1-(u²/v²))." 73's Richard Clark, KB7QHC Seems to me you're way off point here, Richard. I'm in my lab, my inertial frame of reference. I send some EM waves through my vacuum chamber and I measure their speed as 2.997...*10^8 meters/second. The same waves continue on through the glass of the bell jar keeping air out of my vacuum, and I happen to notice that their speed through that glass is1.684*10^8 meters/second. I notice that light from my hydrogen light source contains certain well-defined spectral lines, but each of those passes through my vacuum at the same speed. However, I notice that those lines, in a short pulse of light, come out of the glass separated in time slightly, implying that they took different times to get through the glass, and were therefore not even travelling through the glass at the same velocity; I notice no such separation for the light passing through the vacuum. Further, I notice that light from a distant star has apparently the same set of spectral lines, but they are shifted to slightly longer wavelengths. However, they take the same time to pass through the vacuum as my locally-generated hydrogen light. All my measurements are in the same frame of reference, and IN VACUUM the speed of em radiation appears from all my measurements to be the same, no matter its wavelength, even for very long wavelengths, but in other media, still the same inertial reference frame, it's different. I also happen to notice that the light from the distant star was created in a different inertial frame of reference... OK, I'll shut up on this now. Cheers, Tom |
Not understanding some parts of wave refraction
K7ITM wrote:
I also happen to notice that the light from the distant star was created in a different inertial frame of reference... Not to mention being created in a different medium. -- 73, Cecil http://www.w5dxp.com |
Not understanding some parts of wave refraction
On Apr 5, 4:40 pm, Roy Lewallen wrote:
Yes. And it's very, very nearly the same for air. The 30,000 km would be a typo -- the wavelength in a vacuum at 10 kHz would be 30 km. Roy Lewallen, W7EL Thanks again everyone! It makes sense to me to just treat c, in this case, as a relative speed dependent on the medium. |
Not understanding some parts of wave refraction
MRW wrote:
On Apr 5, 4:40 pm, Roy Lewallen wrote: Yes. And it's very, very nearly the same for air. The 30,000 km would be a typo -- the wavelength in a vacuum at 10 kHz would be 30 km. Roy Lewallen, W7EL Thanks again everyone! It makes sense to me to just treat c, in this case, as a relative speed dependent on the medium. As others have pointed out, it's risky to treat c as a variable or medium-dependent speed. That letter is nearly always used to designate the speed of light (or any EM plane wave) in a vacuum. Using that nearly-universal definition, the speed of an EM wave in any other medium is VF * c where VF is the "velocity factor". It's important to realize that while there's a single value for the speed of all EM waves in a vacuum (c), this isn't true in many other media. In many media, the speed of the wave depends on its frequency, a phenomenon called "dispersion". So in many media there's no universal EM velocity equivalent to c, but rather a frequency-dependent velocity factor. In environments where the field is confined such as a waveguide, the velocity can also depend on the mode, that is the orientation of the fields. So there's not even a single value for each frequency. And this can be true even if the waveguide is filled with a vacuum. Roy Lewallen, W7EL |
Not understanding some parts of wave refraction
Roy Lewallen wrote:
Using that nearly-universal definition, the speed of an EM wave in any other medium is VF * c where VF is the "velocity factor". If I remember correctly, at Texas A&M we used an equation like: c' = VF(c) Writing c-prime like that told us that it wasn't the speed of light in free space. -- 73, Cecil http://www.w5dxp.com |
Not understanding some parts of wave refraction
Roy Lewallen wrote:
As others have pointed out, it's risky to treat c as a variable or medium-dependent speed. Roy - The convenient thing about using medium dependent c in that equation is that we can use things such as index of refraction or velocity factor to convert from vacuum 'c' to 'c' in another medium. The fact that it makes the results of the calculation more accurate tends to mitigate any risk that might be encumbered when using it. To require that only vacuum c be used in the equation to me seems overly authoritarian. I wonder how you feel about the speed of sound? :-) 73, Jim AC6XG That letter is nearly always used to designate the speed of light (or any EM plane wave) in a vacuum. Using that nearly-universal definition, the speed of an EM wave in any other medium is VF * c where VF is the "velocity factor". It's important to realize that while there's a single value for the speed of all EM waves in a vacuum (c), this isn't true in many other media. In many media, the speed of the wave depends on its frequency, a phenomenon called "dispersion". So in many media there's no universal EM velocity equivalent to c, but rather a frequency-dependent velocity factor. In environments where the field is confined such as a waveguide, the velocity can also depend on the mode, that is the orientation of the fields. So there's not even a single value for each frequency. And this can be true even if the waveguide is filled with a vacuum. Roy Lewallen, W7EL |
Not understanding some parts of wave refraction
On 6 Apr 2007 09:04:59 -0700, "K7ITM" wrote:
Seems to me you're way off point here, Richard. Hi Tom, Hardly an unfamiliar comment. I'm in my lab, my inertial frame of reference. I send some EM waves through my vacuum chamber and I measure their speed as 2.997...*10^8 meters/second. The same waves continue on through the glass of the bell jar keeping air out of my vacuum, and I happen to notice that their speed through that glass is1.684*10^8 meters/second. I notice that light from my hydrogen light source contains certain well-defined spectral lines, but each of those passes through my vacuum at the same speed. Same as what? However, I notice that those lines, in a short pulse of light, come out of the glass separated in time slightly, implying that they took different times to get through the glass, and were therefore not even travelling through the glass at the same velocity; I notice no such separation for the light passing through the vacuum. Same as what? Different wavelengths respond to different inertial frames of reference, a prism demonstrates this quite dramatically. This happens quite commonly for wideband transmissions through fiber optics. The solution has been to send them as Soliton waves. Another solution is to employ micro channels. Further, I notice that light from a distant star has apparently the same set of spectral lines, but they are shifted to slightly longer wavelengths. A typical frame of reference example. However, they take the same time to pass through the vacuum as my locally-generated hydrogen light. All my measurements are in the same frame of reference, and IN VACUUM the speed of em radiation appears from all my measurements to be the same, no matter its wavelength, even for very long wavelengths, but in other media, still the same inertial reference frame, it's different. I also happen to notice that the light from the distant star was created in a different inertial frame of reference... There are a lot of "same"s here and some are being shown to be different, and others same. I'm wondering what the point is that I'm way off from. 73's Richard Clark, KB7QHC |
Not understanding some parts of wave refraction
Jim Kelley wrote:
Roy Lewallen wrote: As others have pointed out, it's risky to treat c as a variable or medium-dependent speed. Roy - The convenient thing about using medium dependent c in that equation is that we can use things such as index of refraction or velocity factor to convert from vacuum 'c' to 'c' in another medium. The fact that it makes the results of the calculation more accurate tends to mitigate any risk that might be encumbered when using it. To require that only vacuum c be used in the equation to me seems overly authoritarian. I wonder how you feel about the speed of sound? :-) 73, Jim AC6XG What, the speed of sound in a vacuum? I'm afraid you'll have to ask Cecil or Art about that -- I'm not qualified to comment. I'm not trying to be authoritarian about the use of "c", just reporting what I find in my textbooks. Grabbing just one for example, Kraus' _Electromagnetics_, on p. 352 I find that he uses v as the phase velocity, and says, "For free space (vacuum) the velocity is a well-known constant (usually designated by c and usually called the velocity of light)." and shows an equation for c. Then he gives an equation for the "relative phase velocity" p, as v/c. In the back of R.K. Moore's _Traveling-wave Engineering_, c is listed as "Velocity of light in vacuum". He uses v-sub-p for phase velocity. A number of authors avoid using c altogether, but those who do seem to universally use it to mean the speed of light in a vacuum. What texts do you have where it's used to mean the phase velocity in a medium other than air? Of course, you can always go ahead and interpret c any way you want, even if it isn't what the author intended. Then you can progress from there to any number of bizarre conclusions. They'd fit right in with the ones being "debated" over and over on this newsgroup. Roy Lewallen, W7EL |
Not understanding some parts of wave refraction
On Fri, 06 Apr 2007 16:29:07 -0700, Jim Kelley wrote:
Roy Lewallen wrote: As others have pointed out, it's risky to treat c as a variable or medium-dependent speed. Roy - The convenient thing about using medium dependent c in that equation is that we can use things such as index of refraction or velocity factor to convert from vacuum 'c' to 'c' in another medium. The fact that it makes the results of the calculation more accurate tends to mitigate any risk that might be encumbered when using it. To require that only vacuum c be used in the equation to me seems overly authoritarian. I wonder how you feel about the speed of sound? :-) 73, Jim AC6XG The speed of sound in a vacuum is measured using the sound of one hand clapping. Walt |
Not understanding some parts of wave refraction
Roy Lewallen wrote: Jim Kelley wrote: Roy Lewallen wrote: As others have pointed out, it's risky to treat c as a variable or medium-dependent speed. Roy - The convenient thing about using medium dependent c in that equation is that we can use things such as index of refraction or velocity factor to convert from vacuum 'c' to 'c' in another medium. The fact that it makes the results of the calculation more accurate tends to mitigate any risk that might be encumbered when using it. To require that only vacuum c be used in the equation to me seems overly authoritarian. I wonder how you feel about the speed of sound? :-) 73, Jim AC6XG What, the speed of sound in a vacuum? I'm afraid you'll have to ask Cecil or Art about that -- I'm not qualified to comment. I'm not trying to be authoritarian about the use of "c", just reporting what I find in my textbooks. Grabbing just one for example, Kraus' _Electromagnetics_, on p. 352 I find that he uses v as the phase velocity, and says, "For free space (vacuum) the velocity is a well-known constant (usually designated by c and usually called the velocity of light)." and shows an equation for c. Then he gives an equation for the "relative phase velocity" p, as v/c. In the back of R.K. Moore's _Traveling-wave Engineering_, c is listed as "Velocity of light in vacuum". He uses v-sub-p for phase velocity. A number of authors avoid using c altogether, but those who do seem to universally use it to mean the speed of light in a vacuum. What texts do you have where it's used to mean the phase velocity in a medium other than air? Of course, you can always go ahead and interpret c any way you want, even if it isn't what the author intended. Then you can progress from there to any number of bizarre conclusions. They'd fit right in with the ones being "debated" over and over on this newsgroup. Roy Lewallen, W7EL I think we both understand that light travels at a velocity which is dependent on the medium through which it is travelling. You seem to want to continue to argue about that, and to tell you the truth I can't see much difference between that, and the kind of debate going on over and over in this newsgroup. 73, Jim AC6XG |
Not understanding some parts of wave refraction
Jim Kelley wrote:
I think we both understand that light travels at a velocity which is dependent on the medium through which it is travelling. You seem to want to continue to argue about that, and to tell you the truth I can't see much difference between that, and the kind of debate going on over and over in this newsgroup. This isn't the first time I've failed to communicate, and I'm sure it won't be the last. The sole point I was trying to make is that the letter c is just about universally used, as far as I can tell, to mean the velocity of light in a vacuum. That symbol is not generally used to mean the speed of light in any other medium. Roy Lewallen |
Not understanding some parts of wave refraction
Cecil Moore wrote:
Roy Lewallen wrote: Using that nearly-universal definition, the speed of an EM wave in any other medium is VF * c where VF is the "velocity factor". If I remember correctly, at Texas A&M we used an equation like: c' = VF(c) Writing c-prime like that told us that it wasn't the speed of light in free space. my recollection from optics is c/c' = n, index of refraction for the c' medium, (c always used as the constant in a vacuum). |
Not understanding some parts of wave refraction
On Apr 9, 12:20 pm, Roy Lewallen wrote:
Jim Kelley wrote: I think we both understand that light travels at a velocity which is dependent on the medium through which it is travelling. You seem to want to continue to argue about that, and to tell you the truth I can't see much difference between that, and the kind of debate going on over and over in this newsgroup. This isn't the first time I've failed to communicate, and I'm sure it won't be the last. The sole point I was trying to make is that the letter c is just about universally used, as far as I can tell, to mean the velocity of light in a vacuum. That symbol is not generally used to mean the speed of light in any other medium. Roy Lewallen I'm with Roy on this. v is a wonderful symbol for generalized velocity; c is used by far too many--as Roy says, almost universally-- as the velocity of light in vacuum. Speaking of failures to communicate, I think using a symbol that's so well accepted to mean one thing when you mean something else is a wonderful way to precipitate failures of communication. Clear communication is aided by not changing the meaning of well-accepted symbols. "Let's see... e=m*c^2. Now what c is that? Is it 3e8m/s, or is it only 3.4e7m/s because I'm in water? Will the nuclear blast be only 1/78 as energetic because it's conducted in water? Oh, but wait, at higher frequencies c is greater than at low frequencies, in water. Oh, I'm getting soooo confused...." No, c=3e8m/s, nominally. "Let's see... epsilon-zero = 1/(mu-zero * c^2). Now what c is that? ...." Examples of equations where c is taken for granted as the freespace speed of light abound. I think publishing an equation where c is the speed of light, but not necessarily the freespace speed, shows poor technical editing. Cheers, Tom |
Not understanding some parts of wave refraction
K7ITM wrote: "Let's see... e=m*c^2. Now what c is that? I think I know which one, and as far as I know there hasn't been a dispute about that on RRAA. The question posed on the newsgroup, and the one which still seems to be a point of contention is which one should go in *this* equation: f = c / w I maintain the answer is still - it depends on the medium. I am sorry to have gotten so many pairs of panties wadded up about this. Seemed a noncontroversial notion to me at the time. 73, Jim AC6XG |
Not understanding some parts of wave refraction
Jim Kelley wrote in news:eve92l$mip$1
@news.service.uci.edu: K7ITM wrote: "Let's see... e=m*c^2. Now what c is that? I think I know which one, and as far as I know there hasn't been a dispute about that on RRAA. The question posed on the newsgroup, and the one which still seems to be a point of contention is which one should go in *this* equation: f = c / w I maintain the answer is still - it depends on the medium. Jim, I am not a physicist... but I recall when introduced to e=m*c^2 at high school, that "c" was defined as "the velocity of light in a vacuum". If the "in a vacuum" qualification was unnecessary, if wasn't relevant, I wonder why they complicated and restricted the definition? I am with you (until someone presents a convincing argument otherwise). This leaves all those books, software etc giving a value for "c" as not necessarily in need of revision. Owen |
Not understanding some parts of wave refraction
john Wiener wrote:
c/c' = n, index of refraction for the c' medium, (c always used as the constant in a vacuum). That's the convention we used at Texas A&M 50 years ago. -- 73, Cecil http://www.w5dxp.com |
Not understanding some parts of wave refraction
Being that I have zero qualifications as an expert on C I will tell
you how I see it.. pun intended First, C is specified as the speed of photon travel in a vacuum, per definition... Or as our attorney brethern say it, Per Se... Second, C' is the measured speed of the propagation of the wave front we call light through an atomic medium, air, water, glass, diamond, etc.... The thing to keep in mind is that the two, C and C', are not identical physical entities... C is the unimpeded propagation of a photon - i.e. a single entity - through a non atomic medium we call a vacuum - 'aether' if you will... The photon that left Proxima Centauri ~4 years ago is the same photon that slams into the front lens of the Hubble telescope (according to that photon's wrist watch that ~4 years happened instantaneously, but that's another rant)... Now if you were in orbit at the eyepiece of the Hubble the photon that enters your retina is not the same Proxima Centauri photon that slammed into the Hubble's mirror... And that makes all the difference... C' happens when the photon smashes into the Hubble's glass and is caught up in the electrical fields sorrounding the atoms making up the glass, primarily the electrical field of the outer (valence) electrons of the Protons... Like a house fly at full speed hitting a spiders web the photon begins to tumble and veer sideways and rapidly decellerate causing it to dump it's energy, i.e. radiate an electromagnetic field of it's own... The electron's field absorbs the energy radiated off the photon, causing in increase in the electrons energy level, usually forcing it to jump to a higher 'orbit'... Now at this instant the photon has disappeared (eaten by the spider) and the electron has been pumped up (like Hulk Hogan)... After a short interval the electron drops back to a lower energy level emitting a new photon... This photon takes off like a scalded rabbit at C (or very near C) but doesn't get far before another electron field sucks it up again... And so it goes for the passage of the photon (actually information) through the atomic structure of the transparent material... The photon that pops out of the eyepiece and slams into your retina is the lebenty sebenth generation descendent of the original photon that hit your scope... The process of repeated absorption and emission of a photon by multiple electrons is what slows the light (wave front) when it travels through transparent material... (and also what creates refraction, circles of confusion, and a bunch of other phenomena) Clear as mud, eh wot... denny / k8do |
Not understanding some parts of wave refraction
On Apr 5, 11:00 am, Richard Clark wrote:
On 5 Apr 2007 07:36:49 -0700, "MRW" wrote: c = f*w (c = m/s, f = frequency, w = wavelength) This frequency is relevant ONLY for vacuum (or with a very, very slight alteration) air. Now, it may seem that all air is air, but no. There are slight variations here too that on the global scale small shifts make large changes. Those small shifts are accounted for by pressure, water content (vapor), and temperature. 73's Richard Clark, KB7QHC Same thing happens with light through water, the light slows down but doesnt change in color(frequency). Jimmie |
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