Energy of a magnetic field
Theenergy of the magnetic fieldresults from the excitation of the space permeated by themagnetic field. It can be thought of as the potential energy that would be imparted on a charged particle moving through a region with an external magnetic field present.
Energy stored in an inductor
As a result of the induced magnetic field inside an电感器of inductance \(L\) when a current, \(i,\) flows through, energy is said to be stored in the magnetic field of the inductor.
\[U=\frac12Li^2\]
AnLC oscillatorconsists of an inductor and a capacitor passing energy back and forth without dissipation. A capacitor with capacitance \(C\) is initially charged to \(q_0\) before being attached to an inductor of inductance \(L.\) What is the current when the charge has decreased to half its initial value?
Since energy is not dissipated, employ conservation of energy.
\[U_{L_i} + U_{C_i} = U_{L_f} + U_{C_f}\] \[0 + \frac{q_0^2}{2C} = \frac12Li^2 + \frac{(0.5q_0)^2}{2C}\]
\[\rightarrow i^2 = \frac{3q_0^2}{4LC}\]
Since the natural frequency of an LC oscillator is \(\omega = \frac{1}{\sqrt{LC} },\)
\[i = \frac{\sqrt{3}}{2} q_0 \omega \]
Energy of a magnetic field
The magnetic field component of anelectromagnetic wavecarries a magneticenergydensity\ (u_B \)给出的
\[u_B = \frac{B^2}{2\mu_0}\]
where \(B\) is the amplitude of the magnetic field and \(\mu_0=4\pi \times 10^{-7} \frac{\text{N}}{\text{m}^2}\) is thepermeability of free space.
What is the magnetic energy density of an electromagnetic wave with electric field amplitude \(E = 300,000 \frac{\text{N}}{\text{C}}?\)
First, express the magnetic field amplitude in terms of the electric field amplitude.
\[c=\frac{E}{B}\]
\[\Rightarrow B = \frac{E}{c}\]
Then, calculate the energy density.
\[\begin{align} u_B &= \frac{B^2}{2\mu_0} \\ &= \frac{E^2}{2\mu_0 c^2} \\ &=\frac{(3\times 10^5)^2}{2(4\pi \times 10^{-7})(3\times 10^8)^2} \\ &=\frac{5}{4\pi} \frac{\text{J}}{\text{m}^3} \text{ }_\square \\ \end{align} \]