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 tip of the minute hand moves along a circular arc. In 60 minutes it covers the full circumference, so in 40 minutes it covers 6040=32 of the circle.
The arc length is given by s=rθ, where θ is the angle in radians. For 32 of a full circle, θ=32×2π=34π radians.
The tip of the minute hand traces a circular arc. In 40 minutes, it sweeps 32 of a full circle. Using the arc length formula s=rθ, the distance is 1.5×34π=2π≈6.28 cm.
The minute hand of a watch is a rigid rod that rotates about the centre. Its tip moves along the circumference of a circle of radius 1.5 cm. The distance the tip travels is not the straight-line distance between two positions — it is the length of the curved path, which is an arc of the circle.
The key idea: the distance travelled by the tip in a given time is proportional to the angle through which the hand turns. In 60 minutes, the minute hand completes one full revolution — that is, it sweeps an angle of 2π radians. So in 40 minutes, it sweeps 6040=32 of a full revolution.
The arc length s for a circle of radius r and central angle θ (in radians) is given by:
s=rθ
This formula is the definition of radian measure: the angle in radians is the ratio of arc length to radius. So if you know the angle, the arc length follows directly.
Now let’s work through the calculation.
Find the angle swept in 40 minutes.
Full circle = 60 minutes = 2π radians.
Angle for 40 minutes: