21.08.2013 Views

1 Observing the normal Zeeman effect in transverse and longitudinal ...

1 Observing the normal Zeeman effect in transverse and longitudinal ...

1 Observing the normal Zeeman effect in transverse and longitudinal ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

where α is <strong>the</strong> external angle a ray makes with <strong>the</strong> etalon (what you are measur<strong>in</strong>g) <strong>and</strong> β is <strong>the</strong><br />

<strong>in</strong>ternal angle <strong>the</strong> same ray makes <strong>in</strong>side <strong>the</strong> etalon. Equation 9 is derived from equation 8, <strong>and</strong><br />

equation 10 is Snell’s Law.<br />

Us<strong>in</strong>g <strong>the</strong>se equations calculate Δλ/λ as a function of magnetic flux density for your data. F<strong>in</strong>ally<br />

you need to convert Δλ/λ to ΔE. To do this use equation 11.<br />

∆λ<br />

∆λ<br />

∆E = − E = −hc<br />

(11)<br />

2<br />

λ λ<br />

where λ=643.8 nm for <strong>the</strong> cadmium l<strong>in</strong>e. Use your data to calculate <strong>the</strong> value of <strong>the</strong> Bohr<br />

magnetron, μB.<br />

The literature value is 57.9 μeV/T.<br />

Derivation of equation 9<br />

Any given peak has a value of k <strong>and</strong> as λ changes due to <strong>the</strong> magnetic field k rema<strong>in</strong>s constant,<br />

Therefore,<br />

∆λ<br />

2<br />

=<br />

λ<br />

∆λ<br />

=<br />

λ<br />

2 2<br />

2<br />

d n − s<strong>in</strong> α1<br />

− 2d<br />

n −<br />

⎛ n<br />

⎜<br />

⎝ n<br />

From Snell’s law<br />

2<br />

2<br />

2d<br />

n<br />

2<br />

s<strong>in</strong><br />

2<br />

− s<strong>in</strong> α ⎞ 1<br />

−1<br />

2<br />

s<strong>in</strong> ⎟<br />

− α 0 ⎠<br />

2<br />

α<br />

0<br />

s<strong>in</strong><br />

2<br />

α<br />

0<br />

s<strong>in</strong>α = ns<strong>in</strong><br />

β<br />

(14)<br />

2 2 2<br />

2<br />

2 2<br />

n s<strong>in</strong> α = n ( 1−<br />

s<strong>in</strong> β ) = n cos β<br />

(15)<br />

∆λ<br />

=<br />

λ<br />

⎛ n<br />

⎜<br />

⎝ n<br />

2<br />

2<br />

cos<br />

cos<br />

2<br />

2<br />

β ⎞ 1 cos β1<br />

⎟ −1<br />

= −1<br />

β 0 ⎠ cos β 0<br />

8<br />

(12)<br />

(13)<br />

(16)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!