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Click here for animation. A Classical simulation of the trajectory and angular momentum of the electron in a hydrogen atom in an electric field $\scriptstyle {{\vec {E}}=-3\times 10^{6}{\hat {x}}}$ .	Click here for animation. A Classical simulation of the trajectory and angular momentum of the electron in a hydrogen atom in an electric field $\scriptstyle {{\vec {E}}=-3\times 10^{6}{\hat {x}}}$ .	2004 Indian Ocean earthquake and tsunami	A Classical simulation of the trajectory and angular momentum of the electron in a hydrogen atom in an electric field $\scriptstyle {{\vec {E}}=-3\times 10^{6}{\hat {x}}}$ .

Second order Stark shifts in hydrogen. Each n-level consists of n-1 degenerate sublevels; application of an electric field breaks the degeneracy.	A graphical representation of the complex impedance plane. Note that while reactance $\scriptstyle {\mathrm {X} }$ can be either positive or negative, resistance $\scriptstyle {R}$ is always positive.	An AC supply connected across a device with impedance $\scriptstyle {Z}$ , with an AC voltmeter and ammeter in parallel, and series respectively. An AC supply applying a voltage $\scriptstyle {V}$ across a load $\scriptstyle {Z}$ , driving a current $\scriptstyle {I}$ .	Voltage and current phases for an ideal capacitor and inductor.