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Hartree energy |
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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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2 pi |
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k (inv-mtrs/kelv) |
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-0.049938 |
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2 |
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Avogardo's number |
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Nccp density |
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-2.117427 |
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3 |
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molar volume Si |
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quantum circulutn |
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-0.476066 |
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4 |
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Rydbergxhc in J |
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2 |
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0.117271 |
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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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r(sp)d sp vol 1 |
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0.689331 |
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2 |
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first radiaton sr |
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absolute zero |
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0.074942 |
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3 |
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k (inv-mtrs/kelv) |
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a u charge |
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0.021472 |
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4 |
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Wien wve/Wien frq |
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proton ch/ mss qt |
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0.343576 |
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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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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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Douglas Hartree on the left |
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4.35974354 |
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relationship |
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Eh |
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J |
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-0.117143 |
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electron
in the ground state (the lowest-energy state) of the hydrogen atom . |
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When a hydrogen atom is
in this state, an amount of energy equal to 0.5 Hartree |
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is necessary to free the electron and
thereby cause the atom to become an ion |
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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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