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| What happens if we add two spherical harmonic functions? For example ($/ell = 1$, $m = 1$) and ($\ell = 1$ $m = -1$). Discuss the constructive and destructive interference of complex numbers. | What happens if we add two spherical harmonic functions? For example ($/ell = 1$, $m = 1$) and ($\ell = 1$ $m = -1$). Discuss the constructive and destructive interference of complex numbers. | ||
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| *What linear combination of the $\ell = 0$ and $\ell = 1$ spherical harmonics would describe a probability density that is big in the $x$direction but and small in $-x$ direction? | *What linear combination of the $\ell = 0$ and $\ell = 1$ spherical harmonics would describe a probability density that is big in the $x$direction but and small in $-x$ direction? | ||
| - | An alternative activity only asks students to show how the phase (not the magnitude) changes about the equator. Have one group at each table show $e^{i\phi}$ and one group show $e^{-i\phi}$ around the equator. By asking them to then add their functions together, you can use this as a way of introducing the superposition of states and to talk about how physicists' counting of states ($p_1$, p_0$, $p_{-1}$) differs from chemists' counting of states ($p_x$, $p_y$, $p_z$). | + | An alternative activity only asks students to show how the phase (not the magnitude) changes about the equator. Have one group at each table show $e^{i\phi}$ and one group show $e^{-i\phi}$ around the equator. By asking them to then add their functions together, you can use this as a way of introducing the superposition of states and to talk about how physicists' counting of states ($p_1$, $p_0$, $p_{-1}$) differs from chemists' counting of states ($p_x$, $p_y$, $p_z$). |