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Direct Energy, 2018a

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6 PHOTOVOLTAICS 103<br />

The human eye can sense light from approximately λ = 400 nm to<br />

λ = 650 nm. Using the expressions above, we can calculate in dierent units<br />

the energy range over which the human eye can respond. An individual<br />

red photon with λ = 650 nm has energy<br />

E red =3.056 · 10 −19 J =1.908 eV =1.538 · 10 4 cm −1 (6.7)<br />

in the dierent units. Similarly, an individual blue photon with λ = 400<br />

nm has energy<br />

E blue =4.966 · 10 −19 J =3.100 eV =2.500 · 10 4 cm −1 . (6.8)<br />

We can calculate the energy of individual photons of electromagnetic<br />

radiation at radio frequencies, at microwave frequencies, or in other frequency<br />

ranges too. For example, the radio station WEAX broadcasts with<br />

a frequency f =88MHz. This corresponds to a wavelength of λ =3.407 m.<br />

An individual photon at this frequency has energy<br />

E =5.831 · 10 −26 J =3.640 · 10 −7 eV. (6.9)<br />

As another example, wi- operates at frequencies near f =2.4 GHz which<br />

corresponds to the wavelength λ =0.125 m. Each photon at this frequency<br />

has energy<br />

E =1.590 · 10 −24 J =9.927 · 10 −6 eV. (6.10)<br />

Ultraviolet light has a wavelength slightly shorter than blue light. A photon<br />

of ultraviolet light with wavelength λ = 350 nm, which corresponds to<br />

frequency f =8.57 · 10 14 Hz, has energy<br />

E =5.676 · 10 −19 J =3.543 eV. (6.11)<br />

X-rays operate at wavelengths near λ =10 −10 m. An x-ray photon with<br />

wavelength λ =10 −10 m has energy<br />

E =1.986 · 10 −15 J =1.240 · 10 4 eV. (6.12)<br />

Why do we talk about radio waves but not radio particles while we treat<br />

light as both wave-like and particle-like? A person is around 1.5 to 2 m<br />

tall. The wavelength of the radio station broadcast in the example above<br />

was λ RF ≈ 3.4 m while the wavelength of blue light was λ blue light ≈ 400<br />

nm. Both radio frequency and optical signals are electromagnetic radiation.<br />

Both are well described by Maxwell's equations. Both have wave-like and<br />

particle-like properties. Humans typically talk about the wave-like nature<br />

of radio waves because they are on a scale we can measure with a meter

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