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charateristic impedance of a vacuum |
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E Q U A T I O N S |
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A times B |
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1 |
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elementary charge |
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8 pi squared |
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-0.589878 |
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2 |
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first radiaton cn |
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32 pi |
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0.219921 |
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3 |
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first radiaton sr |
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32 pi squared |
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0.219921 |
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4 |
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light |
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permeability magn |
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0.069229 |
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5 |
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light squared |
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sphere radius 1 |
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0.138505 |
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6 |
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proton spec charg |
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4 pi squared |
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-0.308362 |
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7 |
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wave # /photon en |
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Zeeman / Gauss |
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0.109096 |
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8 |
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9 |
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10 |
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A divided by B |
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1 |
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conductance quntm |
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2 |
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0.069229 |
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2 |
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pi squared |
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von Klitzing |
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1.492496 |
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3 |
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Zeeman / Gauss |
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ion conversion fc |
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0.156684 |
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4 |
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conductance quntm |
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inv Planck |
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-0.012065 |
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5 |
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permeability magn |
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sphere radius 1 |
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0.069229 |
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6 |
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rd surface/ rd vl |
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second radiation |
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-0.374561 |
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7 |
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8 |
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9 |
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10 |
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11 |
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12 |
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13 |
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14 |
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15 |
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16 |
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17 |
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18 |
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19 |
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20 |
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The impedance that, when connected to the
output terminals of a transmission |
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line
of any length, makes the line appear to be infinitely long, for there are
then |
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no
standing waves on the line, and the ratio of voltage to current is the same
for |
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each point on the line.
Also known as surge impedance. |
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highligted |
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derivative |
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nist |
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copyright steve waterman january 2009 |
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