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Theorem 1: Direction of a Curve at the Origin

Derivatives can be used to measure direction in polar as well as in rectangular coordinates. We begin with two theorems, one about the direction of a curve at the origin (an unusual point in polar coordinates) and the other about the direction of a curve elsewhere. Then we shall use these theorems for sketching curves.

THEOREM 1

At any value θ0 where the curve r = f(θ) passes through the origin, the curve is tangent to the line θ = θ0.

More precisely, if r = 0 at θ = θ0 but r ≠ 0 for all θ ≠ θ0 in some neighborhood of θ0, then

07_trigonometric_functions-453.gif07_trigonometric_functions-454.gif

PROOF

Suppose cos θ0 ≠ 0, so tan θ0 exists. Let Δθ be a nonzero infinitesimal. Then Δr ≠ 0 and r changes from 0 to Δr. We compute Δy/Δx.

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Taking standard parts,

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Similarly, when sin θ0 ≠ 0,

07_trigonometric_functions-457.gif

Both limits were given in the theorem to cover the case where the curve is vertical and tan θ0 is undefined.

The theorem tells us that if r = 0 at θ0, the curve must approach the origin from the θ0 direction. Figure 7.8.1 shows two cases.

(a)    If r has a local maximum or minimum at θ0, then r has the same sign on both sides of θ0. In this case the curve has a cusp at θ0.

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Figure 7.8.1 (a)

(b)    If r has no local maximum or minimum at θ0, then r is positive on one side of θ0 and negative on the other side. In this case the curve crosses the origin at θ0.

 

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Figure 7.8.1 (b)

We now consider points other than the origin. In rectangular coordinates, the slope of a curve y = f(x) at a point P is dyjdx = tan φ where φ is the angle between the x-axis and the line tangent to the curve at P as shown in Figure 7.8.2.

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Figure 7.8.2

When r ≠ 0 in polar coordinates, a useful measure of the direction of the curve at a point P is tan ψ, where ψ is the angle between the radius OP and the tangent line at P (see Figure 7.8.3).

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Figure 7.8.3


Last Update: 2006-11-25