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Rydberg constant |
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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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von Klitzing |
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sphere radius 1 |
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1.422283 |
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2 |
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sphere pack squrd |
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2 |
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0.000000 |
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3 |
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4 |
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5 |
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6 |
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7 |
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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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Avogardo's number |
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electron molr mss |
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-2.082090 |
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2 |
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light |
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n u momentum |
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0.105355 |
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3 |
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light squared |
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n u energy |
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0.174657 |
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4 |
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permeability magn |
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36/pi |
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-0.068386 |
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5 |
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Rydberg xhc in eV |
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ion conversion fc |
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0.018950 |
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6 |
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wave # /photon en |
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rd surface/ rd vl |
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-0.068386 |
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7 |
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(1/12) |
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radiation constnt |
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0.348756 |
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8 |
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(16/15) |
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Lyman beta |
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-0.053655 |
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9 |
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(9/8) |
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Lyman alpha |
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-0.063809 |
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10 |
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1 |
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electron mass |
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0.036102 |
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11 |
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8 |
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fine structure |
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-0.098887 |
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12 |
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4/(3) |
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Hydrogen at infty |
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-0.053548 |
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13 |
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pi squared |
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light squared |
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0.070025 |
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14 |
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pi/18 |
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a u charge |
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-0.731219 |
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15 |
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Nccp squared / pi |
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a u charge |
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-0.731219 |
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16 |
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sphere diam 1 |
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elementary charge |
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-0.657860 |
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17 |
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quantum circl x 2 |
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Josephson constnt |
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-0.811862 |
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18 |
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quantum circulutn |
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12 |
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-0.068386 |
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19 |
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4 pi squared |
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Boltzmann |
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2.202052 |
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20 |
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The
most accurately measured of the fundamental constants, which enters into |
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the
formulas for wave numbers of atomic spectra and serves as a universal
scaling |
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factor
for any spectroscopic transition and as an important cornerstone in the |
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determination of other
constants. For any atom, the Rydberg constant |
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For any atom, the Rydberg
constant divided by 1 + m/M,
where m and M are |
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the masses of an electron and of the
nucleus. |
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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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