Home |
Search |
Today's Posts |
#21
|
|||
|
|||
Derivation of Reflection Coefficient vs SWR
On Jan 26, 9:07*am, Cecil Moore wrote:
Keith Dysart wrote: Computing Pf and Pr will yield 50 W forward and 50 W reflected. And yet no current is flowing anywhere. The voltage on the line is completely static. Why would you compute Pf and Pr when no DC current is flowing? To facilitate learning about how the equations work and what they may mean. It is an invalid thing to do Not at all. The equations don't just stop working at 0 frequency. In their general form F(t), there is no hint at all that F can not be a constant. Or, if you prefer, a square wave with a width several times longer than the length of the line. and unrelated to reality. Anything unreal will also be unreal for the specific case of sinusoids. And yet some will claim that 50 W is flowing forward and 50 W is flowing backwards. I know of no one who will claim that for static DC. There are obviously no photons being emitted and therefore, no waves. You really should try to stop thinking about photons for just a short while. All the behaviours of a transmission line can be understood and characterized without reference to photons. Analysis using classic circuit principles works quite fine and has no difficulty at low frequencies. Your example is unrelated to standing waves on an RF transmission line where energy is in motion, photons are continuously being emitted and absorbed, and current and voltage loops are active. There is no standing wave, but the example is quite valid none-the-less. If you like, consider it as a long pulse. And if you only want sinusoids, Fourier will convert the pulse to sinusoids which you can, using superposition, use to solve the problem. The simplicity of the constant voltage makes it easy to check your results. One must realize the limitations of one's model. The wave model obviously fails where there are no waves. Think of it as a long pulse. That should satisfy your need to have 'waves'. ...Keith |
#22
|
|||
|
|||
Derivation of Reflection Coefficient vs SWR
On Jan 26, 12:15*pm, Roger Sparks wrote:
On Fri, 25 Jan 2008 19:13:31 -0800 (PST) Keith Dysart wrote: On Jan 24, 10:33*pm, Roger Sparks wrote: [snip] By examining this derivation, the reader can see that power and energy is reflected when a wave encounters a discontinuity. *The reader can also see that more power is present on the transmission line than is delivered to the load. This is the conventional phraseology for describing the behaviour at the impedance discontinuity. Allow me to offer a specific example for which this phraseology is inappropriate. Consider a 50 V step function generator with an output impedance of 50 ohms driving a 50 ohm line that is 1 second long terminated in an open circuit. Turn on the generator. A 50 V step propagates down the line. The generator is putting 50 J/s into the line. One second later it reaches the open end and begins propagating backwards. After two seconds it reaches the generator. The voltage at the generator is now 100 V and no current is flowing from the generator into the line. In the 2 seconds, the generator put 100 joules into the line which is now stored in the line. The line is at a constant 100 V and the current is zero everywhere. Computing Pf and Pr will yield 50 W forward and 50 W reflected. And yet no current is flowing anywhere. The voltage on the line is completely static. And yet some will claim that 50 W is flowing forward and 50 W is flowing backwards. Does this seem like a reasonable claim for an open circuited transmission line with constant voltage along its length and no current anywhere? I do not find it so. ...Keith This is a reasonable observation for a static situation where energy is stored on a transmission line. * If the example contained an ongoing consideration, like "Where does the power move to?", then it would be reasonable to consider that the wave continued to move, simply to avoid the complication of what EXACTLY happens when a wave starts and stops. So have you thought about "where does the power go?" When the generator is matched to the line so that the reflected wave does not encounter an impedance discontinuity when it arrives back at the generator (and therefore is not reflected), where does the reflected power go? Does it enter the generator? Is it dissipated somewhere? Answers to these questions will quickly lead to doubts about the *reality* of "reflected power". ...Keith |
#23
|
|||
|
|||
Derivation of Reflection Coefficient vs SWR
Keith Dysart wrote:
Not at all. The equations don't just stop working at 0 frequency. As a matter of fact, EM waves cannot exist without photons. There is zero wave activity at DC. Therefore, the forward power and reflected power is zero at DC steady-state. You really should try to stop thinking about photons for just a short while. Yep, you guys would like to sweep the technical knowledge from the field of optical physics and quantum electro- dynamics under the rug. One wonders why. Think of it as a long pulse. That should satisfy your need to have 'waves'. No, only photons will satisfy the definition of EM waves. There are no photons. There are no waves. There are no forward and reflected powers. There are no changing E-fields or H-fields. There is not even any movement of electrons associated with the source voltage. -- 73, Cecil http://www.w5dxp.com |
#24
|
|||
|
|||
Derivation of Reflection Coefficient vs SWR
Keith Dysart wrote:
When the generator is matched to the line so that the reflected wave does not encounter an impedance discontinuity when it arrives back at the generator (and therefore is not reflected), ... On the contrary, it is redistributed back toward the load in the process of destructive interference and becomes constructive interference associated with the forward wave. Whether you call that a reflection or not, the fact that the forward power equals the source power plus the reflected power tells us that reflected power being dissipated in the source would violate the conservation of energy principle. where does the reflected power go? Power doesn't flow so reflected power doesn't "go" anywhere. It is the reflected energy that is flowing, i.e. going somewhere. If the power were flowing, its dimensions would be joules/sec/sec. Maybe you would like to try to explain the physical meaning of those dimensions? Does it enter the generator? forward power = source power + reflected power A component of the forward energy is equal in magnitude to the reflected energy so no, it doesn't enter the source. Is it dissipated somewhere? Not during steady-state. During steady-state it is being used for impedance transformation. After steady-state, it is dissipated either in the source or in the load as a traveling wave. Answers to these questions will quickly lead to doubts about the *reality* of "reflected power". Reflected power is the Poynting vector associated with the reflected wave. It exists at a point. It's average magnitude (indirectly measured by a Bird) is Re(ExH*)/2. It's direction is the direction of the flow of reflected energy. If you don't believe in reflected energy, let your fingers become the circulator load resistor for an open-circuit stub being driven by a KW source. -- 73, Cecil http://www.w5dxp.com |
#25
|
|||
|
|||
Derivation of Reflection Coefficient vs SWR
On Sat, 26 Jan 2008 19:24:22 -0800 (PST)
Keith Dysart wrote: On Jan 26, 12:15*pm, Roger Sparks wrote: On Fri, 25 Jan 2008 19:13:31 -0800 (PST) Keith Dysart wrote: On Jan 24, 10:33*pm, Roger Sparks wrote: [snip] By examining this derivation, the reader can see that power and energy is reflected when a wave encounters a discontinuity. *The reader can also see that more power is present on the transmission line than is delivered to the load. This is the conventional phraseology for describing the behaviour at the impedance discontinuity. Allow me to offer a specific example for which this phraseology is inappropriate. Consider a 50 V step function generator with an output impedance of 50 ohms driving a 50 ohm line that is 1 second long terminated in an open circuit. Turn on the generator. A 50 V step propagates down the line. The generator is putting 50 J/s into the line. One second later it reaches the open end and begins propagating backwards. After two seconds it reaches the generator. The voltage at the generator is now 100 V and no current is flowing from the generator into the line. In the 2 seconds, the generator put 100 joules into the line which is now stored in the line. The line is at a constant 100 V and the current is zero everywhere. Computing Pf and Pr will yield 50 W forward and 50 W reflected. And yet no current is flowing anywhere. The voltage on the line is completely static. And yet some will claim that 50 W is flowing forward and 50 W is flowing backwards. Does this seem like a reasonable claim for an open circuited transmission line with constant voltage along its length and no current anywhere? I do not find it so. ...Keith This is a reasonable observation for a static situation where energy is stored on a transmission line. * If the example contained an ongoing consideration, like "Where does the power move to?", then it would be reasonable to consider that the wave continued to move, simply to avoid the complication of what EXACTLY happens when a wave starts and stops. So have you thought about "where does the power go?" Yes, only the model I use substitutes a battery for the signal generator that you are using. The returning wave can recharge the battery, but how does the current stop? Or does it ever stop? From a practical aspect, the current must stop, but I can not explain how except by resistance that absorbs the circulating power. We must keep the limitations of our models in mind. When the generator is matched to the line so that the reflected wave does not encounter an impedance discontinuity when it arrives back at the generator (and therefore is not reflected), where does the reflected power go? Does it enter the generator? Is it dissipated somewhere? Answers to these questions will quickly lead to doubts about the *reality* of "reflected power". ...Keith The reflected wave that does not encounter an impedance at the generator must be on an infinitely long line, and therefore the conditions must have changed between the time of launch and return. It makes more sense to think that the reflected voltage of (using your example) 50v meets 50v of forward voltage, and therefore finds an infinite resistance, coming to a stop. If that happens, doesn't the same condition occur as soon as the reflected wave is first generated at the line end? The current really stops as soon as the end is reached, with the energy contained in the magnetic field converted to electric field energy visible as voltage. If this happened, the reflected wave could be better described as an electric "jump", similar to a hydraulic jump found in open channel flow of liquids, where kinetic energy is converted to potential energy. This idea of an electric "jump" requires not a reflection occuring without a discontinuity, but a moving wave front that absorbs the traveling wave, bringing it to a stop (in this case). -- 73, Roger, W7WKB |
#26
|
|||
|
|||
Derivation of Reflection Coefficient vs SWR
Cecil Moore wrote in news:mO0nj.4140$J41.257
@newssvr14.news.prodigy.net: Keith Dysart wrote: Not at all. The equations don't just stop working at 0 frequency. As a matter of fact, EM waves cannot exist without photons. There is zero wave activity at DC. Therefore, the forward power and reflected power is zero at DC steady-state. You really should try to stop thinking about photons for just a short while. Yep, you guys would like to sweep the technical knowledge from the field of optical physics and quantum electro- dynamics under the rug. One wonders why. Think of it as a long pulse. That should satisfy your need to have 'waves'. No, only photons will satisfy the definition of EM waves. There are no photons. There are no waves. There are no forward and reflected powers. There are no changing E-fields or H-fields. There is not even any movement of electrons associated with the source voltage. Food for thought! There is no such thing as DC! How’s that you say? You have to turn it on sometime and someday you may turn it off. There for, DC is just very low frequency AC. As another example of physics over thinking, I once had a physics professor describe in detail how an electric motor works using Quark physics. Very interesting but it has no practical value in using electric motors. Much like this long thread has nothing much to do with antennas. John Passaneau W3JXP |
#27
|
|||
|
|||
Derivation of Reflection Coefficient vs SWR
Roy Lewallen wrote:
"A better reason to avoid "stored" is that power isn`t stored at all, anywhere. Anyone who believes so should be able to tell us how many watts are stored in a 50 Ah, 12 volt battery." The 50 Ah of energy stored in a battery may be withdrawn at a rate determined by the load, so it is a variable. Velocity in a transmission line is a constant determined by constructtion of the line. Thus, energy stored in the line is determined by its length, voltage, current, and phase angle. These predict the rate of energy transfer (power). Best regards, Richard Harrison, KB5WZI |
#28
|
|||
|
|||
Derivation of Reflection Coefficient vs SWR
"JOHN PASSANEAU" wrote in message ... There is no such thing as DC! How's that you say? You have to turn it on sometime and someday you may turn it off. There for, DC is just very low frequency AC. John Passaneau W3JXP That's false reasoning OM! Alternating current is not the same as discontinuous current. In the example you provide, a DC supply is either off or on; it does not reverse polarity! You do not make AC by switching on and off DC, even at 50 Hz (or your 60 Hz) |
#29
|
|||
|
|||
Derivation of Reflection Coefficient vs SWR
Suzy wrote:
"You do not make AC by switching on and off DC, even at 50 Hz (or your 60 Hz)" Not without inductance to provide the missing half cycle. Remember vibrator supplies and their solid-state equivalents? Best regards, Richard Harrison, KB5WZI |
#30
|
|||
|
|||
Derivation of Reflection Coefficient vs SWR
Richard Harrison wrote:
Roy Lewallen wrote: "A better reason to avoid "stored" is that power isn`t stored at all, anywhere. Anyone who believes so should be able to tell us how many watts are stored in a 50 Ah, 12 volt battery." The 50 Ah of energy stored in a battery may be withdrawn at a rate determined by the load, so it is a variable. Ah is a unit of charge, not energy. The battery, making the simplifying (and invalid) assumption of constant voltage during discharge, contains 2.16 Mj of energy. Velocity in a transmission line is a constant determined by constructtion of the line. Thus, energy stored in the line is determined by its length, voltage, current, and phase angle. These predict the rate of energy transfer (power). So the rate at which a transmission line transfers energy depends on its length? If I put 100 watts into a one wavelength cable and get 100 watts out, will I get 200 watts out if I extend the cable to two wavelengths? Roy Lewallen, W7EL |
Reply |
Thread Tools | Search this Thread |
Display Modes | |
|
|
Similar Threads | ||||
Thread | Forum | |||
Convert reflection coefficient to Z | Antenna | |||
Reflection Coefficient | Antenna | |||
Uses of Reflection Coefficient Bridges. | Antenna | |||
Reflection Coefficient Challenge Solved | Antenna | |||
Derivation of the Reflection Coefficient? | Antenna |