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A First Course in Linear Algebra, 2017a

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8.2. Spherical and Cyl<strong>in</strong>drical Coord<strong>in</strong>ates 443<br />

8.2 Spherical and Cyl<strong>in</strong>drical Coord<strong>in</strong>ates<br />

Outcomes<br />

A. Understand cyl<strong>in</strong>drical and spherical coord<strong>in</strong>ates.<br />

B. Convert po<strong>in</strong>ts between Cartesian, cyl<strong>in</strong>drical, and spherical coord<strong>in</strong>ates.<br />

Spherical and cyl<strong>in</strong>drical coord<strong>in</strong>ates are two generalizations of polar coord<strong>in</strong>ates to three dimensions.<br />

We will first look at cyl<strong>in</strong>drical coord<strong>in</strong>ates .<br />

When mov<strong>in</strong>g from polar coord<strong>in</strong>ates <strong>in</strong> two dimensions to cyl<strong>in</strong>drical coord<strong>in</strong>ates <strong>in</strong> three dimensions,<br />

we use the polar coord<strong>in</strong>ates <strong>in</strong> the xy plane and add a z coord<strong>in</strong>ate. For this reason, we use the notation<br />

(r,θ,z) to express cyl<strong>in</strong>drical coord<strong>in</strong>ates. The relationship between Cartesian coord<strong>in</strong>ates (x,y,z) and<br />

cyl<strong>in</strong>drical coord<strong>in</strong>ates (r,θ,z) is given by<br />

x = r cos(θ)<br />

y = r s<strong>in</strong>(θ)<br />

z = z<br />

where r ≥ 0, θ ∈ [0,2π), andz is simply the Cartesian coord<strong>in</strong>ate. Notice that x and y are def<strong>in</strong>ed as the<br />

usual polar coord<strong>in</strong>ates <strong>in</strong> the xy-plane. Recall that r is def<strong>in</strong>ed as the length of the ray from the orig<strong>in</strong> to<br />

the po<strong>in</strong>t (x,y,0), whileθ is the angle between the positive x-axis and this same ray.<br />

To illustrate this coord<strong>in</strong>ate system, consider the follow<strong>in</strong>g two pictures. In the first of these, both r<br />

and z are known. The cyl<strong>in</strong>der corresponds to a given value for r. A useful way to th<strong>in</strong>k of r is as the<br />

distance between a po<strong>in</strong>t <strong>in</strong> three dimensions and the z-axis. Every po<strong>in</strong>t on the cyl<strong>in</strong>der shown is at the<br />

same distance from the z-axis. Giv<strong>in</strong>g a value for z results <strong>in</strong> a horizontal circle, or cross section of the<br />

cyl<strong>in</strong>der at the given height on the z axis (shown below as a black l<strong>in</strong>e on the cyl<strong>in</strong>der). In the second<br />

picture, the po<strong>in</strong>t is specified completely by also know<strong>in</strong>g θ as shown.<br />

z<br />

z<br />

z<br />

(x,y,z)<br />

x<br />

y<br />

x<br />

θ<br />

r<br />

(x,y,0)<br />

y<br />

r and z are known<br />

r, θ and z are known<br />

Every po<strong>in</strong>t of three dimensional space other than the z axis has unique cyl<strong>in</strong>drical coord<strong>in</strong>ates. Of<br />

course there are <strong>in</strong>f<strong>in</strong>itely many cyl<strong>in</strong>drical coord<strong>in</strong>ates for the orig<strong>in</strong> and for the z-axis. Any θ will work<br />

if r = 0andz is given.

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