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4.6 Cylindrical polar coordinates 169

Examining the z coordinate, we see thatzvaries from 0 to 2. As z varies from

0 to 2, we imagine the curve AB sweeping out the curved surface as shown in Figure4.26.AtC,r

= 1, θ = 0 ◦ ,z = 2;atD,r = 1, θ = 90 ◦ ,z = 2.Thissurfaceis

partof a cylinder.

Iftherangeofvaluesofacoordinateisnotgivenitisunderstoodthatthatvariable

variesacrossallitspossiblevalues.Forexample,acurvemaybedescribedbyr = 1,

z = −2.Herethereisnomentionofthevaluesthat θ canhave.Itisassumedthat θ

can have its fullrange of values, thatis0 ◦ to360 ◦ .

Engineeringapplication4.5

Helicalantennas

The helix is a shape commonly found inengineering. For example, the springs used

inacar’ssuspensionoftenhave ahelicalshape.Helicalantennaswereinvented by

John Kraus in the 1940s and since then have been used extensively in a variety of

applications including space exploration, satellite communications and mobile telephony.

Developing a mathematical definition of a helix is essential to analysing its

electromagnetic properties.

Wecansetupacylindricalpolarcoordinatesystemwiththezaxisalignedwiththe

axis of the helix as shown in Figure 4.27. If we were to look at the helix along the

directionofthezaxis,allwewouldseewouldbeacircle.Wesaythattheprojectionof

the helix onto thex--y plane isacircle.

z

y

x

Figure4.27

Helix along thezaxis.

Suppose a particular helix can be defined parametrically by the Cartesian equations

x(t) =3cos2t, y(t) =3sin2t, z(t) =t

wheret is varied over a particular range in order to generate the finite length helix

required. By specifying a particular value oft these equations enable us to calculate

particular values ofx,yandzcorresponding toapoint on the helix.

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