The Arc Length Formula: Measuring the Unmeasurable
You already know how to find the distance between two points on a straight line — that's just the Pythagorean theorem. But what if the path between them isn't straight? What if it curves like a roller coaster track, a river on a map, or the graph of y=sinx?
That curved distance is called arc length, and the formula that gives it is one of the most elegant applications of calculus.
The Intuition: Straight Lines Approximate Curves
Imagine you're walking along a winding path. If you take a single giant step, you'll cut the corner and miss the true distance. But if you take many tiny steps — each one almost perfectly straight — the sum of those tiny straight steps will be very close to the actual curved distance.
This is the core idea: break a curve into infinitely many infinitesimally small straight pieces, add them up, and let the pieces become infinitely small. That's exactly what an integral does.
For a function y=f(x) from x=a to x=b, here's the reasoning:
Take a tiny horizontal step dx.
The corresponding vertical change is dy=f′(x)dx.
The tiny straight piece connecting (x,f(x)) to (x+dx,f(x+dx)) has length, by Pythagoras:
(dx)2+(dy)2=1+(dxdy)2dx
Summing all these tiny lengths from a to b gives the total arc length.
Arc Length=∫ab1+(dxdy)2dx
That's the arc length formula for a curve given as y=f(x).
The Precise Statement
Let f be a function whose derivative f′ is continuous on the closed interval [a,b]. Then the length L of the curve y=f(x) from x=a to x=b is:
L=∫ab1+[f′(x)]2dx
The continuity of f′ guarantees the curve is "smooth" — no sharp corners or jumps — so the tiny straight pieces genuinely approximate the curve.
Watch out
A common mistake is to forget the square root. The expression 1+(dy/dx)2 is not the same as 1+dy/dx. The square root comes directly from the Pythagorean theorem — it's non-negotiable.
What If the Curve Is Given Parametrically?
Sometimes a curve is described by x=g(t), y=h(t) for t from α to β. The same idea applies: a tiny step in t gives dx=g′(t)dt and dy=h′(t)dt, so the tiny straight piece has length:
(dx)2+(dy)2=[g′(t)]2+[h′(t)]2dt
Integrating gives:
L=∫αβ(dtdx)2+(dtdy)2dt
This is the parametric arc length formula. It's actually more fundamental — the y=f(x) version is just a special case where x=t and y=f(t).
When equal arc lengths subtend different angles at the centre, the radii are inversely proportional to those angles. The ratio of the radii is 22 : 13.
The connection between arc length, radius, and central angle is fundamental to circular geometry. An arc of length s on a circle of radius r subtends an angle θ (in radians) at the centre according to the relationship s=rθ. This tells us something powerful: for a fixed arc length, a smaller angle means a larger radius, and vice versa.
Think of it this way. If you walk the same distance along the edge of a small circle versus a large circle, you'll turn through a bigger angle on the small circle. The curvature is tighter, so the same path "wraps around" more of the centre.
Let's denote the two circles with radii r1 and r2, and let the equal arc length be s in both cases.
1. Convert the angles to radians
The first circle has a central angle of 65∘, which in radians is: