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			On Sat, 05 Jun 2004 10:14:09 -0500, Cecil Moore  wrote:
 Walter Maxwell wrote:
 But Cecil, take another look at Fig 6 on page 23-5 to note that those two waves
 arrive 180 out of phase at point A, which means only that the E and H fields
 cancel in the rearward direction only, resulting in a Zo match to the source.
 
 Yes, and that is exactly my point. EXACTLY the same thing happens to the E-fields
 and H-fields. That means exactly the same thing that happens to the rearward-
 traveling voltages also happens to the rearward-traveling currents. Two equal-
 magnitude/opposite-phase voltages cancel. Two equal-magnitude/opposite-phase
 currents cancel. That doesn't happen at either an open or a short. If one
 looks at just the voltages, it looks like a short. If one looks at just the
 currents, it looks like an open.
 
 Snip
 
 J. C. Slater says that's what happens in the above quote. Voltages 1/2WL apart
 in time cancel to zero. Currents 1/2WL apart in time cancel to zero.
 
 Yep, but only in the rearward direction.
 
 The rearward direction is what we are talking about. The point is that EXACTLY
 the same thing happens to the two rearward-traveling current waves as happens
 to the two rearward-traveling voltage waves. A short-circuit doesn't affect
 voltages and currents in the same way. An open-circuit doesn't affect
 voltages and currents in the same way. A match point affects the rearward-
 traveling voltages and rearward-traveling currents in EXACTLY the same way.
 The re-reflection at a match point is a conservation of energy reflection where
 the rearward destructive interference energy supplies energy to constructive
 interference in the opposite direction. For light, the equation a
 
 Destructive Interference Irradiance = I1 + I2 - 2{SQRT[(I1)(I2)]}  (9.16)
 
 Constructive Interference Irradiance = I1 + I2 + 2{SQRT[(I1)(I2)]}   (9.15)
 
 _Optics_, by Hecht, fourth edition, page 388
 
 Note the similarities to equations 13 and 15 in Dr. Best's QEX article,
 Part 3.
 
 PFtotal = P1 + P2 - 2{SQRT[(P1)(P2)]}  (Eq 15)
 
 PFtotal = P1 + P2 + 2{SQRT[(P1)(P2)]}  (Eq 13)
 
 Too bad he didn't label them as Hecht did, as "total destructive interference"
 and "total constructive interference" equations.
 
 Sorry, Cecil, in spite of their similarity with Hecht's, these equations are
 totally invalid. Steve derived them from his Eq 9, which is also totally invalid
 for use with reflected power.  This equation is correct and valid when there are
 two separate and individual sources. But here there is only one source, the
 transceiver. When connecting two batteries in series Eq 9 works, because there
 is enough energy there to support the additional current demanded with the
 increased voltage. But not when the transceiver is the sole source of power.
 
 With the transmission line system Steve's voltage V2 comes from the same source
 as V1. The problem is that when the total forward power resulting from the
 addition of reflected power and source power the total forward power is never
 absorbed in the load, the power resulting from the reflection is subtracted from
 the total power. This limitation does not occur when there are two separate
 sources to maintain the increased current.
 
 Because Steve used Eq 9 in an invalid way to derive Eqs 10 through 15, all of
 these derived equations are also invalid. Try Eq 13 for example. It says 75 w
 plus 8.33 w = 133.33 w, as you well know. This is absurd!
 
 In addition, because the powers don't add up correctly using V1 and V2 at zero
 phase relationship, he concocted the ruse that they must add vectorially, and he
 goes through several values of phase relationships to show what the forward
 power would be with the various phases. This is poppycock, because the phase
 relationship between the source (V1) and re-reflected voltage (V2)  is ALWAYS
 ZERO on lossless lines.
 
 His initial problem is that he misinterpreted Eq 6 in Part 1 to yield the
 forward voltage Vfwd, where it actually yields the voltage E of the standing
 wave at any point on the line, where the point on the line is determined by the
 'L' term in the exponents on the right-hand side of the equation. In other
 words, the summation of terms on the right-hand side of his Eq 6 does not equal
 forward voltage Vfwd, as it indicates incorrectly, but instead equals the
 voltage of the standing wave.
 
 In addition to other errors, the entire right-hand column of page 46 is invalid.
 
 Walt
 
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