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Shielding in Li 1s 2s and Li 1s 2p - Boston University

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Shielding in Li 1s 2 2s and Li 1s 2 2p CH101 Fall 2012 Boston University
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Page 1: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Shielding in Li 1s22s and Li 1s22p 

CH101 Fall 2012Boston University

Page 2: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

The Li atom electron configuration 1s22s is more stable than 1s22p. 

The reason is, the 2s electron feels a greater nuclear charge, Zeff, than does the 2p electron.

The following illustrations show qualitatively why this is so.

Shielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 3: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

1s2 portion of Li electron cloudShielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 4: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

2s portion of Li 1s22s electron cloudShielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 5: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

2s outer loop of Li 1s22s electron cloudShielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 6: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

2s outer loop is shielded by 1s2 cloudShielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 7: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

For ~90% of 2s, Zeff,outer ≈ 0.90 x (3 – 2) = 0.9Shielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 8: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

2s inner loop of Li 1s22s electron cloudShielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 9: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

2s inner loop is not shielded by 1s2 cloudShielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 10: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

For ~10% of 2s, Zeff,inner ≈ 0.10 x 3 = 0.3Shielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 11: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

Zeff,2s = Zeff,outer + Zeff,inner = 0.9 + 0.3 = 1.2Shielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 12: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

Li 1s22s valence electron energy

E2s = −13.6 eV Zeff,2s2/4 = − 13.6eV x 1.22/4 = −4.90 eV

Shielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 13: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

2p portion of Li 1s22p electron cloudShielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 14: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

2p is shielded by 1s2 cloudShielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 15: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

For ~100% of 2p, Zeff,2p ≈ 1 x (3 – 2) = 1Shielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 16: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

Li 1s22p valence electron energy

E2p = −13.6 eV Zeff,2p2/4 = −13.6 eV x 12/4 = −3.40 eV

Shielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]

Page 17: Shielding in Li 1s 2s and Li 1s 2p - Boston University

Boston University Slideshow Title Goes Here

Li 1s22s more stable than Li 1s22p

E2s = −13.6 eV Zeff,2s2/4 = − 13.6eV x 1.22/4 = −4.90 eV

E2p = −13.6 eV Zeff,2p2/4 = −13.6 eV x 12/4 = −3.40 eV

Shielding in Li 1s2 2s and Li 1s2 2p

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Copyright © 2012 Dan Dill [email protected]


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