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).
The angle θ (in radians) is given by θ=radiusarc length. For a pendulum of length 75 cm, the answers are: (i) 152 rad,
(ii) 51 rad,
(iii) 257 rad.
The key idea here is the Arc Length Formula for a circle. When a pendulum swings, its tip moves along a circular arc. The length of that arc is directly proportional to the angle the pendulum sweeps out, measured in radians.
Why radians? Because the radian measure is defined precisely so that the arc length s equals the radius r times the angle θ (in radians). That is:
s=rθ⇒θ=rs
This is the cleanest relationship in circular motion — no conversion factors, no π until you need degrees. Here, the pendulum length 75 cm is the radius r, and the arc lengths s are given. So each part is just a division.