How the parametric length formula turns into the integral of the square root of r squared plus the square of its derivative, and how to choose the angles so a polar curve is measured exactly once.
How long is the edge of a cardioid? There is no ruler for curved lines, but there is the same idea used for parametric curves. Add up the distance covered in tiny steps of θ. In polar form the step has a particularly tidy size, and many classic curves give exact answers.
Key terms
The polar speed
Definition Let f be differentiable on an interval and write the curve r=f(θ) as x=f(θ)cosθ, y=f(θ)sinθ. Then
(dθdx)2+(dθdy)2=f(θ)2+f′(θ)2,
so the point moves along the curve at the rate
dθds=r2+(dθdr)2.
In plain words A small step dθ moves the point rdθ around the pole and dr away from it. These two motions are at right angles, so the step has length r2+(dr/dθ)2dθ.
For the spiral r=θ the speed is θ2+1, so at θ=2π it is about 6.36.
Polar arc length
Definition Let f′ be continuous on [a,b] and suppose the curve r=f(θ) is traced exactly once as θ increases from a to b. Then its length is
L=∫abf(θ)2+f′(θ)2dθ.
In plain words Length equals the integral of the polar speed over an interval that traces the curve once.
Example For the cardioid r=1+cosθ we have f′(θ)=−sinθ and
f2+f′2=1+2cosθ+cos2θ+sin2θ=2+2cosθ=4cos22θ.
The square root is 2cos2θ, and the absolute value matters. On [0,2π],
L=∫0π2cos2θdθ+∫π2π(−2cos2θ)dθ=4+4=8.
Smoothness
Definition The length formula above assumes that f is continuously differentiable on [a,b], that is, f′ exists and is continuous there, with one-sided derivatives at the endpoints. The parametrization is regular where the speed f2+f′2 is positive, which fails only where f(θ)=0 and f′(θ)=0 at once, so only at the pole. Regularity is not needed for the length formula. The integrand f2+f′2 is continuous whenever f′ is, so the integral still gives the length when the point stops for an instant at the pole.
In plain words You need f′ to be continuous. The curve itself may still have a cusp at the pole, where the point comes to rest for an instant, and the integral handles it without trouble.
Example The cardioid r=1+cosθ has f(π)=0 and f′(π)=−sinπ=0, so the speed is 0 at θ=π, which is the cusp at the pole. Since f′(θ)=−sinθ is continuous, the formula applies, and it gave the length 8 above.
Parameter interval
Definition The parameter interval for a length computation must trace each part of the curve exactly once. If an interval runs over the whole curve exactly k times, the integral equals k times the length.
In plain words Find a range of θ that draws the whole curve exactly once, and integrate over that.
Example For the circle r=2cosθ the speed squared is 4cos2θ+4sin2θ=4. The circle is traced once on [0,π], so
L=∫0π2dθ=2π,
the circumference of a circle of radius 1. Integrating over [0,2π] would give 4π, twice the true length.
Piecewise curves
Definition If a path is made of arcs r=fk(θ), θk−1≤θ≤θk, with each fk continuously differentiable on its interval and each arc traced once, then the length of the path is
L=k∑∫θk−1θkfk(θ)2+fk′(θ)2dθ.
The same applies to a single curve r=f(θ) whose derivative has finitely many jumps, by splitting at the jumps.
In plain words Boundaries made of pieces of different curves are measured piece by piece, then added.
Example The region inside both r=sinθ and r=cosθ is bounded by r=sinθ for 0≤θ≤4π and r=cosθ for 4π≤θ≤2π. Each piece has speed sin2θ+cos2θ=1, so the boundary has length 4π+4π=2π.
Check yourself
Find the length of the spiral r=eθ for 0≤θ≤1.
Show the answer
Here f=f′=eθ, so f2+f′2=2e2θ and
L=∫012eθdθ=2(e−1)≈2.43.
Find the length of r=θ2 for 0≤θ≤5.
Show the answer
With f′=2θ the speed is θ4+4θ2=θθ2+4 for θ≥0, so
L=∫05θθ2+4dθ=[31(θ2+4)3/2]05=327−8=319.
Someone finds the length of r=3sinθ by integrating over [0,2π]. What do they get, and what is the right answer?
Show the answer
The speed is 3, so they get 6π. The circle is traced once on [0,π], so its length is 3π.
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