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Einstein Coefficients

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Presentation on theme: "Einstein Coefficients"— Presentation transcript:

1 Einstein Coefficients
m Harry Kroto 2004

2 Einstein Coefficients
m Harry Kroto 2004

3 Einstein Coefficients
Bn←m m Harry Kroto 2004

4 Einstein Coefficients
Bn←m m Harry Kroto 2004

5 Einstein Coefficients
Bn←m Bn→m m Harry Kroto 2004

6 Einstein Coefficients
Bn←m Bn→m m Harry Kroto 2004

7 Einstein Coefficients
Bn←m Bn→m An→m m Harry Kroto 2004

8 Einstein Coefficients
Bn←m Bn→m An→m m A = 1.2 x 3 n em2 transitions per sec Harry Kroto 2004

9 Einstein Coefficients
Bn←m Bn→m An→m m A = 1.2 x 3 n em2 transitions per sec Spontaneous emission lifetime  Harry Kroto 2004

10 Einstein Coefficients
Bn←m Bn→m An→m m A = 1.2 x 3 n em2 transitions per sec Spontaneous emission lifetime   (sec) = 1/A = 1037/3 sec Harry Kroto 2004

11 Lifetime (secs)  ~ 1037/3 Harry Kroto 2004

12 e = 1Debye 1yr = 3 x 107 sec * magnetic dipole
  (Hz) 3 (Hz3)  (sec) H (1420 MHz) cm 1.5x x * H2CO rotations cm 3 x x CO2 vibrations  3 x x Na D electronic nm 1.5 x x H Lyman  nm 3 x x e = 1Debye yr = 3 x 107 sec * magnetic dipole Harry Kroto 2004

13 e = 1Debye 1yr = 3 x 107 sec * magnetic dipole
  (Hz) 3 (Hz3)  (sec) H (1420 MHz) cm 1.5x x * H2CO rotations cm 3 x x CO2 vibrations  3 x x Na D electronic nm 1.5 x x H Lyman  nm 3 x x e = 1Debye yr = 3 x 107 sec * magnetic dipole Harry Kroto 2004

14 e = 1Debye 1yr = 3 x 107 sec * magnetic dipole
  (Hz) 3 (Hz3)  (sec) H (1420 MHz) cm 1.5x x * H2CO rotations cm 3 x x CO2 vibrations  3 x x Na D electronic nm 1.5 x x H Lyman  nm 3 x x e = 1Debye yr = 3 x 107 sec * magnetic dipole Harry Kroto 2004

15 e = 1Debye 1yr = 3 x 107 sec * magnetic dipole
  (Hz) 3 (Hz3)  (sec) H (1420 MHz) cm 1.5x x * H2CO rotations cm 3 x x CO2 vibrations  3 x x Na D electronic nm 1.5 x x H Lyman  nm 3 x x e = 1Debye yr = 3 x 107 sec * magnetic dipole Harry Kroto 2004

16 e = 1Debye 1yr = 3 x 107 sec * magnetic dipole
  (Hz) 3 (Hz3)  (sec) H (1420 MHz) cm 1.5x x * H2CO rotations cm 3 x x CO2 vibrations  3 x x Na D electronic nm 1.5 x x H Lyman  nm 3 x x e = 1Debye yr = 3 x 107 sec * magnetic dipole Harry Kroto 2004

17 e = 1Debye 1yr = 3 x 107 sec * magnetic dipole
  (Hz) 3 (Hz3)  (sec) H (1420 MHz) cm 1.5x x * H2CO rotations cm 3 x x CO2 vibrations  3 x x Na D electronic nm 1.5 x x H Lyman  nm 3 x x e = 1Debye yr = 3 x 107 sec * magnetic dipole Harry Kroto 2004

18 Collisions in the Interstellar Medium ISM
In space the pressures are low Very low If n = number of molecules per cc (mainly H) then Harry Kroto 2004

19 Collisions in the Interstellar Medium ISM
In space the pressures are low Very low If n = number of molecules per cc (mainly H) then 2b = 103/n yrs per collision Harry Kroto 2004

20 Collisions in the Interstellar Medium ISM
In space the pressures are low Very low If n = number of molecules per cc (mainly H) then 2b = 103/n yrs per collision 3b = 1023/n2 yrs per collision Harry Kroto 2004

21 Collisions in the Interstellar Medium ISM
In space the pressures are low Very low If n = number of molecules per cc (mainly H) then 2b = 103/n yrs per collision 3b = 1023/n2 yrs per collision Number densities are anything from n = Harry Kroto 2004

22 Harry Kroto 2004


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