Stigmatic Optics. Rafael G González-Acuña
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Название: Stigmatic Optics

Автор: Rafael G González-Acuña

Издательство: Ingram

Жанр: Физика

Серия: IOP Series in Emerging Technologies in Optics and Photonics

isbn: 9780750334631

isbn:

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      The minus sign of the first cosine means that the wave is travelling to the right of positive z. The plus sign of the second cosine implies that the wave is moving to the right of negative z.

      Also, notice that the time is being multiplied by the angular frequency,

      w=kv.(1.51)

      Notice that image is the speed inside a medium and c is the speed in vacuum. Therefore, if we pick the wave that is traveling to positive z, E⃗(r⃗,t) is given by

      E⃗(r⃗,t)=E0cos(kz−wt)(1.52)

      where we set A→E0. The last expression is the equation of the plane wave.

      Now let’s pay attention to the Helmholtz equation spherical coordinates. First let’s recall the Helmholtz equation,

      ∇2E⃗(r⃗)+k2E⃗(r⃗)=0.(1.53)

      hence, in spherical coordinates the Helmholtz equation is expressed as,

      To solve it assume that E⃗(r⃗) has the following form,

      where E′(r) is a function of r. Thus replacing equation (1.55) in equation (1.54),

      1r2∂∂rr2−E′r2+r∂E′∂r+k2E′r=0(1.56)

      expanding,

      1r2−∂E′∂r+r∂2E′∂r2+∂E′∂r+k2E′r=0(1.57)

      simplify,

      1r∂2E′∂r2+k2E′r=0.(1.58)

      Notice, that is the same equation that we solved in the previous section. Therefore, we can conclude that the solution of the wave equation in spherical coordinates has the following form,

      E⃗(r⃗,t)=E0rcos(kz−wt).(1.59)

      Notice that the amplitude of the wave decreases as r→∞.

      As an exercise to the reader, please study the Helmholtz equation in cylindrical coordinates. The Helmholtz equation in cylindrical coordinates is the following expression,

      1r∂∂rr∂E⃗(r⃗)∂r+k2E⃗(r⃗)=0.(1.60)

      In this chapter, we briefly studied Maxwell’s equations, from which we find the wave equation. From the latter, we obtained some particular solutions and their spatial part—the Helmholtz equation.

      The Helmholtz equation will be of great help to us because through it we will find the eikonal equation and in turn, the ray equation. These last equations lay the foundations of geometric optics. Geometric optics is the playing field of stigmatism which will be presented in-depth in chapter 5 and the following chapters; stigmatic systems will be studied in detail.

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