Electromagnetic Waves
62 Energy in Electromagnetic Waves
Learning Objectives
- Explain how the energy and amplitude of an electromagnetic wave are related.
- Given its power output and the heating area, calculate the intensity of a microwave oven’s electromagnetic field, as well as its peak electric and magnetic field strengths
Anyone who has used a microwave oven knows there is energy in electromagnetic waves. Sometimes this energy is obvious, such as in the warmth of the summer sun. Other times it is subtle, such as the unfelt energy of gamma rays, which can destroy living cells.
Electromagnetic waves can bring energy into a system by virtue of their electric and magnetic fields. These fields can exert forces and move charges in the system and, thus, do work on them. If the frequency of the electromagnetic wave is the same as the natural frequencies of the system (such as microwaves at the resonant frequency of water molecules), the transfer of energy is much more efficient.
Connections: Waves and Particles
The behavior of electromagnetic radiation clearly exhibits wave characteristics. But we shall find in later modules that at high frequencies, electromagnetic radiation also exhibits particle characteristics. These particle characteristics will be used to explain more of the properties of the electromagnetic spectrum and to introduce the formal study of modern physics.
Another startling discovery of modern physics is that particles, such as electrons and protons, exhibit wave characteristics. This simultaneous sharing of wave and particle properties for all submicroscopic entities is one of the great symmetries in nature.
But there is energy in an electromagnetic wave, whether it is absorbed or not. Once created, the fields carry energy away from a source. If absorbed, the field strengths are diminished and anything left travels on. Clearly, the larger the strength of the electric and magnetic fields, the more work they can do and the greater the energy the electromagnetic wave carries.
A wave’s energy is proportional to its amplitude squared ([latex]{E}^{2}[/latex] or [latex]{B}^{2}[/latex]). This is true for waves on guitar strings, for water waves, and for sound waves, where amplitude is proportional to pressure. In electromagnetic waves, the amplitude is the maximum field strength of the electric and magnetic fields. (See Figure 62.1.)
Thus the energy carried and the intensity [latex]I[/latex] of an electromagnetic wave is proportional to [latex]{E}^{2}[/latex] and [latex]{B}^{2}[/latex]. In fact, for a continuous sinusoidal electromagnetic wave, the average intensity [latex]{I}_{\text{ave}}[/latex] is given by
where [latex]c[/latex] is the speed of light, [latex]{\epsilon }_{0}[/latex] is the permittivity of free space, and [latex]{E}_{0}[/latex] is the maximum electric field strength; intensity, as always, is power per unit area (here in [latex]{\text{W/m}}^{2}[/latex]).
The average intensity of an electromagnetic wave [latex]{I}_{\text