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Arc Length of Parametric Curves

How long is a curved path? If you walk along a winding trail, the distance on your step counter is longer than the straight-line distance between the start and the finish. For a curve given by parametric equations, one integral measures that curved length. It’s also exactly how you find the total distance travelled by a particle moving in the plane.

Chop the curve into many tiny pieces. Each piece is almost a straight segment, the hypotenuse of a right triangle with legs Δx\Delta x and Δy\Delta y:

Δs≈(Δx)2+(Δy)2=(ΔxΔt)2+(ΔyΔt)2 Δt\Delta s \approx \sqrt{(\Delta x)^2 + (\Delta y)^2} = \sqrt{\left( \frac{\Delta x}{\Delta t} \right)^2 + \left( \frac{\Delta y}{\Delta t} \right)^2}\ \Delta t

Adding up all the pieces and letting Δt→0\Delta t \to 0 turns the sum into an integral.

A curve from t = a to t = b approximated by four straight chords. One chord, of length delta s, is the hypotenuse of a right triangle with legs delta x and delta y. Δx Δy Δs t = b t = a x y
Each short chord has length (Δx)2+(Δy)2\sqrt{(\Delta x)^2 + (\Delta y)^2}. More, shorter chords give a better estimate of the curve’s length.

If x(t)x(t) and y(t)y(t) have continuous derivatives and the curve is traced exactly once as tt goes from aa to bb, its length is

L=∫ab(dxdt)2+(dydt)2 dtL = \int_a^b \sqrt{\left( \frac{dx}{dt} \right)^2 + \left( \frac{dy}{dt} \right)^2}\ dt

The integrand is always ≥0\ge 0, so the length is never negative. (For a graph y=f(x)y = f(x), the same idea gives ∫ab1+(f′(x))2 dx\int_a^b \sqrt{1 + (f'(x))^2}\, dx; see arc length.)

If (x(t),y(t))(x(t), y(t)) is the position of a particle at time tt, then (x′(t))2+(y′(t))2\sqrt{(x'(t))^2 + (y'(t))^2} is its speed. So the same integral is the total distance travelled:

What it measuresHow to find it
Total distance travelledevery bit of the path, as a positive length∫ab(x′(t))2+(y′(t))2 dt\displaystyle\int_a^b \sqrt{(x'(t))^2 + (y'(t))^2}\, dt
Displacementthe change in position, from start to finishthe vector ⟨x(b)−x(a), y(b)−y(a)⟩\langle x(b) - x(a),\ y(b) - y(a) \rangle

The straight-line distance between the start and the finish is the length of the displacement vector, and it’s never more than the distance travelled. If the particle goes around a curve more than once, the distance travelled counts every lap, even though the curve itself has the same length.

The square root makes most arc length integrals impossible to find by hand. On the AP exam, arc length almost always appears on the calculator-active section: write the integral, then evaluate it numerically (in radian mode) and give 33 decimal places. A few curves are designed so that (x′)2+(y′)2(x')^2 + (y')^2 is a perfect square, or so that a u-substitution works. Those can be done exactly.

Example 1: A line segment, checked two ways

Section titled “Example 1: A line segment, checked two ways”

Find the length of x=3tx = 3t, y=4ty = 4t for 0≤t≤20 \le t \le 2.

Solution. dxdt=3\dfrac{dx}{dt} = 3 and dydt=4\dfrac{dy}{dt} = 4, so

L=∫0232+42 dt=∫025 dt=10L = \int_0^2 \sqrt{3^2 + 4^2}\, dt = \int_0^2 5\, dt = 10

Check: the curve is the segment from (0,0)(0, 0) to (6,8)(6, 8), and the distance formula gives 36+64=10\sqrt{36 + 64} = 10.

Find the length of x=2cos⁡tx = 2\cos t, y=2sin⁡ty = 2\sin t for 0≤t≤2π0 \le t \le 2\pi. What changes if 0≤t≤4π0 \le t \le 4\pi?

Solution. (dxdt)2+(dydt)2=4sin⁡2t+4cos⁡2t=4\left( \dfrac{dx}{dt} \right)^2 + \left( \dfrac{dy}{dt} \right)^2 = 4\sin^2 t + 4\cos^2 t = 4, so

L=∫02π4 dt=2(2π)=4πL = \int_0^{2\pi} \sqrt{4}\, dt = 2(2\pi) = 4\pi

That’s the circumference of a circle of radius 22, as it should be.

For 0≤t≤4π0 \le t \le 4\pi, the point goes around the circle twice. The integral gives 8π8\pi: that’s the distance travelled, but the curve itself is still only 4π4\pi long. The arc length formula measures the curve only when it is traced once.

Example 3: An exact answer by u-substitution

Section titled “Example 3: An exact answer by u-substitution”

Find the length of x=t2x = t^2, y=23t3y = \dfrac{2}{3}t^3 for 0≤t≤30 \le t \le \sqrt{3}.

Solution. dxdt=2t\dfrac{dx}{dt} = 2t and dydt=2t2\dfrac{dy}{dt} = 2t^2, so

4t2+4t4=4t2(1+t2)=2t1+t2(t≥0)\sqrt{4t^2 + 4t^4} = \sqrt{4t^2(1 + t^2)} = 2t\sqrt{1 + t^2} \qquad (t \ge 0)

Let u=1+t2u = 1 + t^2, du=2t dtdu = 2t\, dt. When t=0t = 0, u=1u = 1; when t=3t = \sqrt{3}, u=4u = 4.

L=∫032t1+t2 dt=∫14u du=[23u3/2]14=23(8−1)=143L = \int_0^{\sqrt{3}} 2t\sqrt{1 + t^2}\, dt = \int_1^4 \sqrt{u}\, du = \left[ \frac{2}{3}u^{3/2} \right]_1^4 = \frac{2}{3}(8 - 1) = \frac{14}{3}

Check: the straight line from (0,0)(0, 0) to (3,23)(3, 2\sqrt{3}) has length 9+12=21≈4.583\sqrt{9 + 12} = \sqrt{21} \approx 4.583, a little less than 143≈4.667\dfrac{14}{3} \approx 4.667. Good: the curve is slightly longer than the chord.

A particle moves in the plane with x(t)=t2−4tx(t) = t^2 - 4t and y(t)=2sin⁡(1.5t)y(t) = 2\sin(1.5t) for 0≤t≤40 \le t \le 4 (calculator in radian mode). Find the total distance travelled, and the particle’s displacement.

Solution.

distance=∫04(2t−4)2+(3cos⁡(1.5t))2 dt≈11.878\text{distance} = \int_0^4 \sqrt{(2t - 4)^2 + \big( 3\cos(1.5t) \big)^2}\ dt \approx 11.878

Displacement: the particle starts at (0,0)(0, 0) and ends at (16−16, 2sin⁡6)≈(0,−0.559)(16 - 16,\ 2\sin 6) \approx (0, -0.559). The displacement vector is ⟨0, 2sin⁡6⟩≈⟨0,−0.559⟩\langle 0,\ 2\sin 6 \rangle \approx \langle 0, -0.559 \rangle, so the particle ends up only about 0.5590.559 units from where it started, even though it travelled almost 1212 units.

Forgetting to square the derivatives. The integrand is (x′)2+(y′)2\sqrt{(x')^2 + (y')^2}, not x′+y′\sqrt{x' + y'} and not x′+y′x' + y'.

Splitting the square root. a2+b2\sqrt{a^2 + b^2} is not a+ba + b. In Example 1, 9+16=5\sqrt{9 + 16} = 5, not 3+4=73 + 4 = 7.

Using the wrong interval when the curve is retraced. If the curve is traced more than once on [a,b][a, b], the integral gives the distance travelled, not the length of the curve. For a curve’s length, integrate over one trip only.

Confusing distance with displacement. Distance travelled is an integral of speed and is always positive. Displacement is the change in position, ⟨x(b)−x(a), y(b)−y(a)⟩\langle x(b) - x(a),\ y(b) - y(a) \rangle. AP questions often ask for both, so read each part carefully.

Not showing the integral on calculator questions. AP graders need to see the setup, such as ∫04(x′(t))2+(y′(t))2 dt\int_0^4 \sqrt{(x'(t))^2 + (y'(t))^2}\, dt, before the decimal answer. A bare number usually loses the setup point.

Calculator in degree mode. With trig functions in x(t)x(t) or y(t)y(t), degree mode gives a wrong value with no warning.

1. (Warm-up) Find the length of x=1+6tx = 1 + 6t, y=2−8ty = 2 - 8t for 0≤t≤10 \le t \le 1.

SolutionL=∫0162+(−8)2 dt=∫0110 dt=10L = \int_0^1 \sqrt{6^2 + (-8)^2}\, dt = \int_0^1 10\, dt = 10

Check: from (1,2)(1, 2) to (7,−6)(7, -6) is 36+64=10\sqrt{36 + 64} = 10.

2. (Warm-up) Find the length of x=3cos⁡tx = 3\cos t, y=3sin⁡ty = 3\sin t for 0≤t≤π0 \le t \le \pi. What shape is this?

Solution

(x′)2+(y′)2=9sin⁡2t+9cos⁡2t=9(x')^2 + (y')^2 = 9\sin^2 t + 9\cos^2 t = 9, so

L=∫0π3 dt=3πL = \int_0^{\pi} 3\, dt = 3\pi

It’s the top half of a circle of radius 33: half of the circumference 6π6\pi.

3. (Warm-up) Write, but do not evaluate by hand, the integral for the length of x=t2x = t^2, y=sin⁡ty = \sin t for 0≤t≤π0 \le t \le \pi. Then use a calculator to evaluate it.

SolutionL=∫0π4t2+cos⁡2t dt≈10.354L = \int_0^{\pi} \sqrt{4t^2 + \cos^2 t}\ dt \approx 10.354

4. (Core) Find the exact length of x=t2x = t^2, y=t3y = t^3 for 0≤t≤20 \le t \le 2.

Solution

4t2+9t4=t4+9t2\sqrt{4t^2 + 9t^4} = t\sqrt{4 + 9t^2} for t≥0t \ge 0. Let u=4+9t2u = 4 + 9t^2, du=18t dtdu = 18t\, dt; uu runs from 44 to 4040.

L=∫02t4+9t2 dt=118∫440u du=127[u3/2]440=4040−827=8010−827≈9.073L = \int_0^2 t\sqrt{4 + 9t^2}\, dt = \frac{1}{18}\int_4^{40} \sqrt{u}\, du = \frac{1}{27}\Big[ u^{3/2} \Big]_4^{40} = \frac{40\sqrt{40} - 8}{27} = \frac{80\sqrt{10} - 8}{27} \approx 9.073

5. (Core) Find the exact length of x=etcos⁡tx = e^t\cos t, y=etsin⁡ty = e^t\sin t for 0≤t≤10 \le t \le 1.

Solution

By the product rule, x′=et(cos⁡t−sin⁡t)x' = e^t(\cos t - \sin t) and y′=et(sin⁡t+cos⁡t)y' = e^t(\sin t + \cos t).

(x′)2+(y′)2=e2t[(cos⁡t−sin⁡t)2+(sin⁡t+cos⁡t)2]=e2t(2)=2e2t(x')^2 + (y')^2 = e^{2t}\big[ (\cos t - \sin t)^2 + (\sin t + \cos t)^2 \big] = e^{2t}(2) = 2e^{2t}

(The cross terms ∓2sin⁡tcos⁡t\mp 2\sin t\cos t cancel, and sin⁡2t+cos⁡2t=1\sin^2 t + \cos^2 t = 1 in each bracket.)

L=∫012 et dt=2(e−1)≈2.430L = \int_0^1 \sqrt{2}\, e^t\, dt = \sqrt{2}(e - 1) \approx 2.430

6. (Core) Find the exact length of x=t3−3tx = t^3 - 3t, y=3t2y = 3t^2 for 0≤t≤20 \le t \le 2.

Solution

x′=3t2−3x' = 3t^2 - 3 and y′=6ty' = 6t:

(x′)2+(y′)2=9t4−18t2+9+36t2=9t4+18t2+9=9(t2+1)2(x')^2 + (y')^2 = 9t^4 - 18t^2 + 9 + 36t^2 = 9t^4 + 18t^2 + 9 = 9(t^2 + 1)^2

A perfect square, so the root is 3(t2+1)3(t^2 + 1):

L=∫023(t2+1) dt=[t3+3t]02=8+6=14L = \int_0^2 3(t^2 + 1)\, dt = \Big[ t^3 + 3t \Big]_0^2 = 8 + 6 = 14

7. (Core) (Calculator active.) A particle moves with x(t)=t2−3tx(t) = t^2 - 3t and y(t)=ln⁡(1+t2)y(t) = \ln(1 + t^2) for 0≤t≤30 \le t \le 3. Find the total distance travelled, and the distance between the particle’s starting and ending points.

Solution

x′(t)=2t−3x'(t) = 2t - 3 and y′(t)=2t1+t2y'(t) = \dfrac{2t}{1 + t^2}.

distance travelled=∫03(2t−3)2+(2t1+t2)2 dt≈5.377\text{distance travelled} = \int_0^3 \sqrt{(2t - 3)^2 + \left( \frac{2t}{1 + t^2} \right)^2}\ dt \approx 5.377

The particle starts at (0,0)(0, 0) and ends at (9−9, ln⁡10)=(0,ln⁡10)(9 - 9,\ \ln 10) = (0, \ln 10). The distance between them is ln⁡10≈2.303\ln 10 \approx 2.303, much less than the distance travelled, because the particle moves left and then back right.

8. (Challenge) Find the length of one arch of the cycloid x=t−sin⁡tx = t - \sin t, y=1−cos⁡ty = 1 - \cos t, 0≤t≤2π0 \le t \le 2\pi. (Hint: 1−cos⁡t=2sin⁡2t21 - \cos t = 2\sin^2\frac{t}{2}.)

Solution(x′)2+(y′)2=(1−cos⁡t)2+sin⁡2t=1−2cos⁡t+cos⁡2t+sin⁡2t=2−2cos⁡t(x')^2 + (y')^2 = (1 - \cos t)^2 + \sin^2 t = 1 - 2\cos t + \cos^2 t + \sin^2 t = 2 - 2\cos t

Using the hint, 2−2cos⁡t=4sin⁡2t22 - 2\cos t = 4\sin^2\dfrac{t}{2}, so the root is 2∣sin⁡t2∣=2sin⁡t22\left\lvert \sin\dfrac{t}{2} \right\rvert = 2\sin\dfrac{t}{2} (it’s non-negative for 0≤t≤2π0 \le t \le 2\pi).

L=∫02π2sin⁡t2 dt=[−4cos⁡t2]02π=−4(−1)+4(1)=8L = \int_0^{2\pi} 2\sin\frac{t}{2}\, dt = \left[ -4\cos\frac{t}{2} \right]_0^{2\pi} = -4(-1) + 4(1) = 8

9. (Challenge) The astroid x=cos⁡3tx = \cos^3 t, y=sin⁡3ty = \sin^3 t, 0≤t≤2π0 \le t \le 2\pi, is a four-pointed star. Find its total length. (Watch the square root carefully.)

Solution

x′=−3cos⁡2tsin⁡tx' = -3\cos^2 t\sin t and y′=3sin⁡2tcos⁡ty' = 3\sin^2 t\cos t:

(x′)2+(y′)2=9sin⁡2tcos⁡2t(cos⁡2t+sin⁡2t)=9sin⁡2tcos⁡2t(x')^2 + (y')^2 = 9\sin^2 t\cos^2 t(\cos^2 t + \sin^2 t) = 9\sin^2 t\cos^2 t

So the integrand is 3∣sin⁡tcos⁡t∣3\lvert \sin t\cos t \rvert, with absolute value. Integrating 3sin⁡tcos⁡t3\sin t\cos t over [0,2π][0, 2\pi] would wrongly give 00.

By symmetry, the four quarters have equal length. On [0,π2]\left[ 0, \tfrac{\pi}{2} \right], sin⁡tcos⁡t≥0\sin t\cos t \ge 0:

L=4∫0π/23sin⁡tcos⁡t dt=12[sin⁡2t2]0π/2=12⋅12=6L = 4\int_0^{\pi/2} 3\sin t\cos t\, dt = 12\left[ \frac{\sin^2 t}{2} \right]_0^{\pi/2} = 12 \cdot \frac{1}{2} = 6