Compute the volume of a solid of revolution generated by rotating a region around the y‑axis using the shell method.Enter a function f(x) ≥ 0, interval [a, b] (a ≥ 0 for classic shell radius), and instantly obtain volume via adaptive numeric integration. Visualize the curve, a representative cylindrical shell, and the solid’s cross‑section.
When a plane region bounded by y = f(x) (with f(x) ≥ 0), the x‑axis, and vertical lines x = a and x = b is revolved about the y‑axis, the resulting solid’s volume can be computed by summing infinitesimally thin cylindrical shells. Each shell has radius x, height f(x), and thickness dx. Its lateral surface area is 2π·radius·height, leading to the elemental volume dV = 2π x f(x) dx. Integrating from a to b gives the exact volume:
This method is particularly powerful when the region is defined as a function of x and rotation occurs around a vertical axis. Unlike the disk/washer method (which integrates along the axis of rotation), shells often simplify integrals, especially when the functions are easier to express in terms of x.
Tested against exact analytic integrals:
Our adaptive Simpson routine recursively bisects intervals until estimated local error falls below 1e-7 × length scaling. The final error estimate is displayed alongside the volume, providing transparency. All calculations are performed in double-precision floating point (IEEE 754).
1. Setup: Given f(x), a, b (a ≥ 0). Ensure f(x) ≥ 0 on the interval.
2. Shell element: At a generic x, cut a vertical slice. When rotated about y‑axis, it sweeps a cylindrical shell of radius x, height f(x), thickness dx. Unwrapping gives a rectangular slab: width = 2πx (circumference), height = f(x), thickness = dx ⇒ volume element = (2πx)·f(x)·dx.
3. Integration: Sum all shells from x = a to x = b → V = 2π ∫ab x·f(x) dx.
4. Numerical Integration: Because symbolic antiderivatives may be unavailable for arbitrary user functions, we implement an adaptive Simpson quadrature that recursively refines subintervals until estimated error falls below 1e-7. The algorithm evaluates the integrand g(x) = 2π·x·f(x). The final volume is reported with an error estimate.
5. Verification: For polynomial inputs, the relative error often vanishes below machine precision; examples are cross-checked with exact analytic integration.
| Method | Orientation | Integration variable | When preferred |
|---|---|---|---|
| Shell Method | Vertical rotation axis (y‑axis) | x (perpendicular to axis) | Function given as y = f(x); region bounded by y-axis or vertical lines |
| Disk / Washer | Horizontal rotation axis (x‑axis) | x (parallel to axis) | Function given as y = f(x) and rotation around x‑axis |
Our calculator focuses on the shell method around the y-axis. However, if you need rotation about the x‑axis, you can apply the disk method via our upcoming toolset or transform the function accordingly.
A chemical engineer needs to design a vertical cylindrical tank with a curved bottom given by y = √(x) from x=0 to x=4 (units: meters). Rotating this curve around the y‑axis yields the internal volume. Using the shell method: V = 2π ∫04 x·√x dx = 2π ∫04 x3/2 dx = 2π·(2/5)x5/2 |04 = 2π·(2/5)·32 = (128π/5) ≈ 80.425 m³. This tool reproduces the analytic result within 1e-6. The visualization helps communicate the shell concept to stakeholders.