Cylindrical Shell Method: Formula & Examples

#Calculus
TL;DR
The cylindrical shell method finds the volume of a solid of revolution by adding up thin nested tubes instead of flat slices. For a region revolved about the $y$-axis, the volume is $V = \int_a^b 2\pi,(\text{radius})(\text{height}),dx = \int_a^b 2\pi x,f(x),dx$. Its advantage over the disk and washer methods is that you integrate along the axis perpendicular to the axis of revolution, so you rarely have to solve the curve for its inverse.
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Bhanzu TeamLast updated on September 27, 202614 min read

What Is The Cylindrical Shell Method?

The cylindrical shell method is a technique for finding the volume of a solid of revolution by slicing the region into thin strips parallel to the axis of revolution, so each strip sweeps out a hollow cylinder, or shell, when the region turns. You add up the volumes of all the shells with a definite integral. It is one of the standard tools for volume of solids of revolution, alongside the disk and washer methods.

For a region under $y = f(x)$ from $x = a$ to $x = b$ revolved about the $y$-axis, the formula is:

$$V = \int_a^b 2\pi x,f(x),dx$$

Read the three pieces directly off the picture. The factor $2\pi x$ is the circumference of a shell whose radius is $x$; the value $f(x)$ is the height of that shell; and $dx$ is its thickness. A single shell holds a volume of about $2\pi x,f(x),dx$, and the integral sums them from the inner radius $a$ to the outer radius $b$.

In general, for any straight axis of revolution, the shell method reads:

$$V = \int 2\pi,(\text{radius})(\text{height}),(\text{thickness})$$

The whole method is choosing the radius and height correctly for the axis you are turning about, then integrating. Everything below is that one idea applied to the $y$-axis, the $x$-axis, and an offset line.

How Do You Derive The Cylindrical Shell Formula?

The formula comes from one geometric move: unroll a thin shell into a flat sheet. This pairs the algebra with a picture at every step.

Take a shell of inner radius $x$, thickness $dx$, and height $f(x)$. Its volume is the difference of two cylinders, the outer one of radius $x + dx$ and the inner one of radius $x$:

$$dV = \pi (x + dx)^2 f(x) - \pi x^2 f(x) = \pi f(x)\left(2x,dx + (dx)^2\right)$$

The term $(dx)^2$ is vanishingly small next to $2x,dx$, so it drops out in the limit, leaving:

$$dV = 2\pi x,f(x),dx$$

The same result falls out of the unrolling picture with no algebra. Slit the thin tube down its side and flatten it: you get a rectangular sheet whose length is the circumference $2\pi x$, whose height is $f(x)$, and whose depth is the thickness $dx$. Its volume is length times height times depth, which is exactly $2\pi x,f(x),dx$. Summing every sheet from $x = a$ to $x = b$ gives the integral.

When Should You Use Shells Instead Of Disks Or Washers?

The disk method and the washer method slice the region perpendicular to the axis of revolution, so each slice is a flat coin or ring. The shell method slices parallel to the axis, so each slice is a tube. That single difference decides which method is easier.

  • Match the slice to the variable you can integrate. Disks and washers integrate along the axis parallel to the axis of revolution; shells integrate along the axis perpendicular to it. If the region is described as $y = f(x)$ and you are revolving about the $y$-axis, shells let you keep everything in $x$ and integrate $dx$.

  • Shells avoid solving for the inverse. To use washers about the $y$-axis you must rewrite $y = f(x)$ as $x = f^{-1}(y)$. For a curve like $y = 2x - x^2$ that inverse has two branches and forces you to split the integral. Shells never ask for the inverse, so one integral does the job.

  • Shells often replace two integrals with one. When a region's boundary switches from one curve to another partway up, the washer method may need several integrals stacked in $y$. Shells in $x$ frequently cover the whole region in a single sweep.

A quick rule of thumb: if solving the boundary for the other variable is ugly, or if the region touches the axis in an awkward way, reach for shells. If the region is a clean stack of disks perpendicular to the axis, disks or washers are simpler. For the shared foundations behind all three, see applications of integration and area between two curves.

How Do You Use The Cylindrical Shell Method? Worked Examples

Each example is fully stepped, and the volume is checked against the disk or washer method (or by Pappus's theorem) wherever a second route exists. Every integral here is a definite integral, so there is no constant of integration.

Example 1: Revolve about the $y$-axis (basic shells).

Find the volume when the region under $y = x^2$ from $x = 0$ to $x = 2$ is revolved about the $y$-axis.

The radius of a shell at position $x$ is $x$, and its height is $f(x) = x^2$:

$$V = \int_0^2 2\pi x,(x^2),dx = 2\pi \int_0^2 x^3,dx = 2\pi\left[\frac{x^4}{4}\right]_0^2 = 2\pi\left(\frac{16}{4}\right) = 8\pi$$

Check with washers in $y$: for a height $y$ between $0$ and $4$, the slice runs from $x = \sqrt{y}$ to $x = 2$, so $V = \pi\int_0^4\left(2^2 - (\sqrt{y})^2\right)dy = \pi\int_0^4 (4 - y),dy = \pi[4y - \tfrac{y^2}{2}]_0^4 = \pi(16 - 8) = 8\pi$. The two agree.

Final answer: $V = 8\pi$ cubic units.

Example 2: Revolve about the $y$-axis where the inverse is messy.

Find the volume when the region bounded by $y = 2x - x^2$ and $y = 0$ is revolved about the $y$-axis.

The curve meets the $x$-axis where $2x - x^2 = x(2 - x) = 0$, so $x$ runs from $0$ to $2$. The radius is $x$ and the height is $2x - x^2$:

$$V = \int_0^2 2\pi x,(2x - x^2),dx = 2\pi \int_0^2 \left(2x^2 - x^3\right)dx = 2\pi\left[\frac{2x^3}{3} - \frac{x^4}{4}\right]_0^2$$

$$V = 2\pi\left(\frac{16}{3} - 4\right) = 2\pi\left(\frac{16 - 12}{3}\right) = 2\pi\cdot\frac{4}{3} = \frac{8\pi}{3}$$

This is where shells earn their keep: inverting $y = 2x - x^2$ gives $x = 1 \pm \sqrt{1 - y}$, a two-branch inverse that would force the washer method into a split integral. Shells stay in $x$ and finish in one line.

Final answer: $V = \dfrac{8\pi}{3}$ cubic units.

Example 3: Revolve about the $x$-axis (shells in $y$).

Find the volume when the region bounded by $y = \sqrt{x}$, $y = 0$, and $x = 4$ is revolved about the $x$-axis.

Revolving about the $x$-axis while using shells means the shells are horizontal, so integrate in $y$. A shell at height $y$ has radius $y$. Its height runs in the $x$-direction from the curve $x = y^2$ across to $x = 4$, so the shell height is $4 - y^2$, with $y$ from $0$ to $2$:

$$V = \int_0^2 2\pi y,(4 - y^2),dy = 2\pi \int_0^2 \left(4y - y^3\right)dy = 2\pi\left[2y^2 - \frac{y^4}{4}\right]_0^2 = 2\pi(8 - 4) = 8\pi$$

Check with disks in $x$: $V = \pi\int_0^4 (\sqrt{x})^2,dx = \pi\int_0^4 x,dx = \pi[\tfrac{x^2}{2}]_0^4 = 8\pi$. The two agree.

Final answer: $V = 8\pi$ cubic units.

Example 4: Revolve about an offset vertical line.

Find the volume when the region bounded by $y = x - x^2$ and $y = 0$ is revolved about the line $x = 2$.

The curve meets $y = 0$ at $x = 0$ and $x = 1$, so $x$ runs from $0$ to $1$. The axis is now $x = 2$, so the radius is no longer $x$ but the distance from the strip to that line: $\text{radius} = 2 - x$. The height stays $x - x^2$:

$$V = \int_0^1 2\pi,(2 - x)(x - x^2),dx = 2\pi \int_0^1 \left(2x - 3x^2 + x^3\right)dx$$

$$V = 2\pi\left[x^2 - x^3 + \frac{x^4}{4}\right]_0^1 = 2\pi\left(1 - 1 + \frac{1}{4}\right) = \frac{\pi}{2}$$

Check with Pappus's centroid theorem: the region has area $\int_0^1 (x - x^2),dx = \tfrac{1}{6}$ and centroid $\bar{x} = \tfrac{1}{2}$, so the centroid travels a distance $2\pi(2 - \tfrac{1}{2}) = 3\pi$. Then $V = 3\pi \cdot \tfrac{1}{6} = \tfrac{\pi}{2}$. The two agree.

Final answer: $V = \dfrac{\pi}{2}$ cubic units.

What Are The Shell Formulas For The Different Axes?

The method never changes; only the radius and the height do. This table collects the three cases you will meet.

Table: Cylindrical shell formulas by axis of revolution.

Axis of revolution

Slice / variable

Radius

Height

Volume

The $y$-axis

vertical strip, integrate $dx$

$x$

$f(x)$

$\displaystyle\int_a^b 2\pi x,f(x),dx$

The $x$-axis

horizontal strip, integrate $dy$

$y$

$g(y)$

$\displaystyle\int_c^d 2\pi y,g(y),dy$

Vertical line $x = L$ (region left of it)

vertical strip, integrate $dx$

$L - x$

$f(x)$

$\displaystyle\int_a^b 2\pi (L - x),f(x),dx$

Vertical line $x = L$ (region right of it)

vertical strip, integrate $dx$

$x - L$

$f(x)$

$\displaystyle\int_a^b 2\pi (x - L),f(x),dx$

For a region trapped between two curves, the height is the top curve minus the bottom curve, exactly as in area between two curves. The radius is always the distance from the strip to the axis, so keep it positive by subtracting in the order that the picture demands.

Why Does The Cylindrical Shell Method Work?

The method works because a solid of revolution can be built two equally valid ways, and shells pick the one that matches the region's natural description.

  • A solid is the sum of its shells. Just as a tree trunk is a set of growth rings, a solid of revolution is a nest of thin tubes. Add the volume of every tube and you have the whole solid, which is what the integral does.

  • Circumference carries the $2\pi$. Each shell, unrolled, is a rectangle whose width is the circle it came from. That circle has circumference $2\pi r$, which is why every shell integral carries a factor of $2\pi$ times the radius. The height and thickness are just the other two sides of the flattened sheet.

  • Perpendicular slicing is the whole point. Shells cut parallel to the axis, so the variable of integration runs perpendicular to it. That is the geometric reason shells succeed where disks stall: the region gets measured in the variable it was written in, with no inverse to solve.

Seen this way, shells and disks are not rivals but two readings of one solid. Disks sum flat cross-sections; shells sum nested tubes. Both land on the same volume, and the fundamental theorem of calculus is what turns either sum into an exact number.

Who Invented The Cylindrical Shell Method?

Volumes of revolution were computed long before integral notation existed, by slicing solids into pieces small enough to add.

Two other figures shaped the volumes-of-revolution story:

  • Pappus of Alexandria (c. 290 – c. 350 CE, Roman Egypt) stated the centroid theorem that still cross-checks shell answers: a region's volume of revolution equals its area times the distance its centroid travels. It is the shortcut used to verify Example 4 above.

  • Johannes Kepler (1571–1630, Germany) computed the volumes of wine barrels by imagining them as stacks of thin slices in his 1615 Nova Stereometria, an early, practical use of the same slicing instinct the shell method formalises.

Where Is The Cylindrical Shell Method Used In The Real World?

Any object made by spinning a profile around an axis, or any quantity that accumulates in rings, is shell-method territory.

  • Manufacturing and machining: pipes, bottles, wheels, and lathe-turned parts are solids of revolution, and their material volume and weight are computed by integrating shells across the radius.

  • Engineering and pressure vessels: the force of water or gas on the curved wall of a tank, and the volume it holds at each radius, are found by summing thin cylindrical layers.

  • Physics and rotation: the moment of inertia of a spinning disk or flywheel is an integral of $r^2$ over nested rings, the same shell decomposition weighted by radius.

  • 3D printing and modelling: software that spins a 2D outline into a 3D object estimates its volume, and the filament it needs, by adding concentric shells.

  • Environmental science: the volume of water in a circular reservoir at a given depth profile is a stack of rings, integrated the same way.

One idea, adding up nested tubes, spans a lathe shop, a water tank, and a spinning flywheel, which is why the shell method outlives the exam it is first taught for.

What Are The Most Common Mistakes With The Cylindrical Shell Method?

These four errors account for most lost marks with shells, and each matches a question real students ask on r/calculus, r/learnmath, and course common-error handouts.

Swapping the radius and the height.

Where it slips in:

A student revolving $y = f(x)$ about the $y$-axis writes the shell height as $x$ and the radius as $f(x)$, reversing the two.

Don't do this:

Do not guess which factor is which. The radius is the distance from the strip to the axis; the height is how tall the strip is.

The correct way:

For a vertical strip revolved about the $y$-axis, radius $= x$ and height $= f(x)$, giving $2\pi x,f(x),dx$. Sketch one strip and label the distance to the axis before writing anything.

Integrating in the wrong variable.

Where it slips in:

A student revolves about the $x$-axis but keeps integrating $dx$, mixing the shell method up with disks.

Don't do this:

Do not integrate parallel to the axis of revolution when you chose shells. Shells cut parallel to the axis, so the variable of integration is perpendicular to it.

The correct way:

About the $x$-axis, shells are horizontal, so integrate $dy$ with radius $y$. About the $y$-axis, integrate $dx$ with radius $x$.

Using $x$ as the radius when the axis is offset.

Where it slips in:

A student revolving about the line $x = 2$ writes the radius as $x$, as if the axis were still the $y$-axis.

Don't do this:

Do not use the bare coordinate as the radius unless the axis is the coordinate axis itself.

The correct way:

The radius is the distance from the strip to the actual axis. About $x = 2$ with the region to its left, radius $= 2 - x$, giving $2\pi(2 - x),f(x),dx$. Choose the subtraction order that keeps the radius positive.

Dropping the factor of $2\pi$ or leaving a stray $+C$.

Where it slips in:

A student integrates $x,f(x)$ but forgets the $2\pi$ from the circumference, or attaches a constant of integration to a definite integral.

Don't do this:

Do not omit the circumference factor, and do not write $+C$ on a definite integral.

The correct way:

Carry the full $2\pi,(\text{radius})(\text{height})$ into the integral, then evaluate between the two limits. A definite integral returns a number, so no $+C$ appears.

Practice Problems On The Cylindrical Shell Method

Work each one, then check against the verified answer.

  1. Revolve the region under $y = x^3$ from $x = 0$ to $x = 1$ about the $y$-axis.
    (Answer: $V = \int_0^1 2\pi x,x^3,dx = 2\pi[\tfrac{x^5}{5}]_0^1 = \tfrac{2\pi}{5}$.)

  2. Revolve the region bounded by $y = x$, $y = 0$, $x = 1$ about the $y$-axis.
    (Answer: $V = \int_0^1 2\pi x,(x),dx = 2\pi[\tfrac{x^3}{3}]_0^1 = \tfrac{2\pi}{3}$. Washer check: $\pi\int_0^1(1 - y^2),dy = \tfrac{2\pi}{3}$.)

  3. Revolve the region under $y = x^2$ from $x = 1$ to $x = 3$ about the $y$-axis.
    (Answer: $V = \int_1^3 2\pi x,x^2,dx = 2\pi[\tfrac{x^4}{4}]_1^3 = 2\pi\cdot 20 = 40\pi$.)

  4. Revolve the region bounded by $y = \sqrt{x}$, $y = 0$, $x = 1$ about the $x$-axis (use shells in $y$).
    (Answer: $V = \int_0^1 2\pi y,(1 - y^2),dy = 2\pi[\tfrac{y^2}{2} - \tfrac{y^4}{4}]_0^1 = \tfrac{\pi}{2}$. Disk check: $\pi\int_0^1 x,dx = \tfrac{\pi}{2}$.)

  5. Revolve the region bounded by $y = x$, $y = 0$, $x = 2$ about the line $x = 3$.
    (Answer: radius $= 3 - x$, so $V = \int_0^2 2\pi(3 - x)x,dx = 2\pi[\tfrac{3x^2}{2} - \tfrac{x^3}{3}]_0^2 = \tfrac{20\pi}{3}$. Pappus check confirms $\tfrac{20\pi}{3}$.)

  6. Revolve the region under $y = x^2$ from $x = 0$ to $x = 1$ about the $y$-axis.
    (Answer: $V = \int_0^1 2\pi x,x^2,dx = 2\pi[\tfrac{x^4}{4}]_0^1 = \tfrac{\pi}{2}$.)

Where Should You Go Next After The Cylindrical Shell Method?

Shells are one of three routes to a volume of revolution, and the natural next doors compare and extend them.

  1. The disk method. The perpendicular-slice counterpart for solids with no hole, and the fastest check on a shell answer.

  2. The washer method. Handles solids with a gap between the region and the axis, the case shells and disks each cover differently.

  3. Volume of solids of revolution. The overview that ties disks, washers, and shells into one decision framework.

If your child is meeting volumes of revolution for the first time, a live Bhanzu trainer teaches the shell method from the nested-tube picture up in the Bhanzu math program.

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Frequently Asked Questions

What is the cylindrical shell method formula?
For a region under $y = f(x)$ from $x = a$ to $x = b$ revolved about the $y$-axis, the volume is $V = \int_a^b 2\pi x,f(x),dx$. The factor $2\pi x$ is the shell's circumference, $f(x)$ is its height, and $dx$ is its thickness.
When should you use the cylindrical shell method instead of disks?
Use shells when solving the boundary curve for the other variable is hard, or when the washer method would need several integrals. Shells integrate perpendicular to the axis of revolution, so you keep the curve in its original variable and avoid finding an inverse.
Do you integrate with respect to $x$ or $y$ in the shell method?
Integrate in the variable that runs perpendicular to the axis of revolution. About the $y$-axis, integrate $dx$ with radius $x$; about the $x$-axis, integrate $dy$ with radius $y$.
How do you find the radius for an offset axis?
The radius is the distance from the strip to the axis, not the bare coordinate. About the vertical line $x = L$ with the region to its left, the radius is $L - x$; to its right, it is $x - L$. Choose the order that keeps the radius positive.
What is the difference between the shell method and the disk method?
The disk and washer methods slice perpendicular to the axis of revolution, making flat coins or rings. The shell method slices parallel to the axis, making nested tubes. Both give the same volume; they differ in which variable you integrate.
Does the shell method give the same answer as the washer method?
Yes. For any solid of revolution both methods return the identical volume, as the worked examples confirm by cross-checking each answer. You pick whichever makes the integral simpler for the region you have.
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