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Shells and Integral Applications · Tutorial 706 of 999

Shell Volumes for Symmetric Regions

Use symmetry carefully: identify which slices share a radius, compare their extents, and integrate each distinct shell only once.

Advanced 11 min read

What You'll Learn

  • Identify when a mirrored interval gives the same shell radii and heights.
  • Use the shell-height union when slices from opposite sides generate the same radius.
  • Recognize when overlapping extents must not be added as separate heights.
  • Preserve distinct radii when the axis of rotation is not the region’s symmetry axis.
  • Set up and evaluate shell integrals using symmetry without double-counting.

Why Symmetry Needs Care in Shell Integrals

Symmetry can make a shell-volume integral shorter, but it does not automatically mean that one side contributes twice the other. A shell is determined by its radius and by the full vertical extent of the region at that radius. Two slices that rotate to the same radius may trace out the same shell, and their vertical extents may overlap.

The safe approach is to ask two questions before using symmetry: Do the slices have the same distance from the axis of rotation? If they do, what vertical heights do they cover together? The answers determine whether the shell is counted once, whether heights can be added, or whether the slices belong to different radii.

Key principle: Count each distinct shell radius once. At that radius, use the union of the vertical extents contributed by all slices that rotate there. Add heights only when those extents are disjoint.

Shell Height When Slices Share a Radius

Consider rotation about the vertical line \(x=c\). A vertical slice at \(x\) has radius \(r=|x-c|\). For a given positive radius \(r\), the possible source slices are at \(x=c-r\) and \(x=c+r\), provided those slices lie in the region.

Each source slice contributes a set of vertical \(y\)-values. If the region is between two curves on that slice, this set is often one interval. If a slice has several separate pieces, keep track of each piece. The shell at radius \(r\) reaches exactly the heights covered by at least one source slice. Its height is the total length of that union; if the union has gaps, do not count the gaps as height.

Definition: For rotation about \(x=c\), the shell height \(H(r)\) is the total length of the union of the vertical \(y\)-sets in the region at \(x=c-r\) and \(x=c+r\), omitting slices that are outside the region. The shell-volume formula is $$ V=2\pi\int rH(r)\,dr, $$ over the distinct radii occupied by the rotated region.

This is the usual cylindrical-shell formula, with the height defined carefully when multiple slices produce the same radius. If the two vertical extents overlap, their union can be shorter than the sum of their individual lengths. If they are disjoint, their lengths do add.

When Reflection Really Reduces the Integral

Suppose the region is symmetric about \(x=c\), and it is rotated about that same line. Reflection sends each slice at \(x=c-r\) to the slice at \(x=c+r\). Symmetry means those slices have the same vertical extent. They also have the same radius \(r\). They therefore generate the same shell, not two different shells to be added together.

Theorem: If a region is symmetric about the vertical axis of rotation \(x=c\), then, for each \(r>0\), the slices at \(c-r\) and \(c+r\) have identical vertical extents whenever both are in the region. The shell height at radius \(r\) is that common extent, counted once. Thus a shell integral over just one side of the symmetry axis accounts for the entire solid, as long as that side covers all occupied radii.

Why this works: Rotating a point \((c-r,y)\) about \(x=c\) traces a circle of radius \(r\) at height \(y\). The reflected point \((c+r,y)\) traces the very same circle. For each height present on one slice, symmetry places that height on the other slice too. The two slices therefore add no new heights at radius \(r\). The shell height is the common vertical extent, and each distinct radius is integrated once.

By contrast, if the axis of rotation is not the symmetry axis, reflection may change the distance to the axis. The paired slices can then produce different radii, so their contributions must be assigned to those radii separately. Symmetry may still simplify the calculation, but not by automatically doubling one side.

Worked Example: A Symmetric Semicircle About Its Symmetry Axis

Worked Example: A Symmetric Semicircle About Its Symmetry Axis

Rotate the upper half-disk \(x^2+y^2\le 4,\ y\ge 0\) about the \(y\)-axis. Use symmetry to find the volume.

At a fixed \(x\), the upper boundary is \(y=\sqrt{4-x^2}\), and the lower boundary is \(y=0\). For \(0\le x\le2\), the shell radius is \(x\), and its height is

$$ h(x)=\sqrt{4-x^2}-0=\sqrt{4-x^2}. $$

The region is symmetric about the \(y\)-axis, which is also the axis of rotation. The slices at \(x\) and \(-x\) have the same height and generate the same radius \(x\). Therefore, integrate over the right half only:

$$ V=2\pi\int_0^2 x\sqrt{4-x^2}\,dx. $$

Set \(u=4-x^2\), so \(du=-2x\,dx\), or \(x\,dx=-\frac12du\). When \(x=0\), \(u=4\); when \(x=2\), \(u=0\). Thus

$$ \begin{aligned} V &=2\pi\left(-\frac12\int_4^0\sqrt{u}\,du\right)\\ &=\pi\int_0^4 u^{1/2}\,du\\ &=\pi\left[\frac23u^{3/2}\right]_0^4\\ &=\pi\left(\frac23\cdot 8-0\right)\\ &=\frac{16\pi}{3}. \end{aligned} $$

Check: differentiating \(\frac23u^{3/2}\) gives \(u^{1/2}\), so the antiderivative is correct; the bounds give \(u=4\) and \(u=0\). The result is the volume of a hemisphere of radius \(2\), consistent with the solid formed by rotating the upper half-disk.

Overlapping Extents Must Be Combined

If mirrored slices have the same radius but different vertical extents, the shell height is not automatically either one height or the sum. It is the length of their union. In particular, overlap contributes only once. The following example makes this distinction explicit.

Worked Example: Different Extents at the Same Radius

Let the region be the union of the rectangles \([-1,0]\times[0,1]\) and \([0,1]\times[0,2]\). Rotate it about the \(y\)-axis.

For any radius \(r\) with \(0<r\le1\), the two source slices are \(x=-r\) and \(x=r\). Their vertical extents are

$$ S(-r)=[0,1], \qquad S(r)=[0,2]. $$

These slices have the same radius \(r\). Their union is \([0,2]\), which has length \(2\). Therefore the shell height is \(H(r)=2\), not \(1+2\). The volume is

$$ \begin{aligned} V &=2\pi\int_0^1 r(2)\,dr\\ &=4\pi\left[\frac{r^2}{2}\right]_0^1\\ &=4\pi\left(\frac12-0\right)\\ &=2\pi. \end{aligned} $$

Check: at every radius from \(0\) to \(1\), the solid reaches heights \(0\le y\le2\), so it is a cylinder of radius \(1\) and height \(2\). Its volume is \(\pi(1)^2(2)=2\pi\), matching the shell integral.

A tempting but incorrect calculation adds the two slice heights at every radius: \(2\pi\int_0^1 r(1+2)\,dr=3\pi\). That counts the shared height interval \([0,1]\) twice. The correction is to take the union of the extents first, then integrate the resulting shell height.

When a Symmetry Axis and Rotation Axis Differ

A region may be symmetric while the axis of rotation is elsewhere. Reflection still matches the shapes and heights of paired slices, but it need not match their radii. In that situation, do not replace one slice’s contribution by twice the other’s. Keep the actual radius for each slice, or pair the terms while preserving both radii.

Worked Example: A Symmetric Disk Rotated About an Offset Axis

Rotate the disk \(x^2+y^2\le1\) about the vertical line \(x=1\). The disk is symmetric about the \(y\)-axis, but the axis of rotation is \(x=1\), not \(x=0\).

At coordinate \(x\), the vertical extent is from \(-\sqrt{1-x^2}\) to \(\sqrt{1-x^2}\), so its height is \(2\sqrt{1-x^2}\). Since every point of the disk has \(x\le1\), the radius is \(1-x\). The shell integral over the full interval is

$$ V=2\pi\int_{-1}^1(1-x)\,2\sqrt{1-x^2}\,dx. $$

To use the disk’s symmetry, pair the terms at \(x\) and \(-x\) for \(0\le x\le1\). Their heights agree, but their radii are \(1-x\) and \(1+x\), respectively. Their combined radius factor is

$$ (1-x)+(1+x)=2. $$

Consequently,

$$ \begin{aligned} V &=2\pi\int_0^1\bigl((1-x)+(1+x)\bigr)\,2\sqrt{1-x^2}\,dx\\ &=8\pi\int_0^1\sqrt{1-x^2}\,dx\\ &=8\pi\left(\frac{\pi}{4}\right)\\ &=2\pi^2. \end{aligned} $$

For the integral, \(\int_0^1\sqrt{1-x^2}\,dx=\pi/4\), the area of a quarter-unit disk. Check by expanding the original integrand: the term \(2x\sqrt{1-x^2}\) is odd and integrates to zero over \([-1,1]\), while \(\int_{-1}^1 2\sqrt{1-x^2}\,dx=\pi\). Hence the original expression is \(2\pi(\pi)=2\pi^2\), confirming the paired calculation.

The symmetry simplified the heights and allowed the interval to be paired, but it did not make the two radii equal. Treating the reflected slices as identical shells would lose the difference between radii \(1-x\) and \(1+x\).

A Reliable Process for Symmetric Shell Problems

Before shortening a shell integral, identify its radius and height from the geometry. Then decide which mirrored slices truly correspond to the same shell.

1
Locate the axis and choose slices.
For rotation about a vertical line, use vertical slices; for rotation about a horizontal line, use horizontal slices.
2
Compute the radius.
Use the distance from each slice to the axis. Reflected slices need not have equal distances if the axis is not the symmetry axis.
3
Find the extent at each radius.
For slices that share a radius, take the union of the heights they cover. Add lengths only when those height intervals do not overlap.
4
Integrate distinct shells once.
Apply \(2\pi\int rH(r)\,dr\) over the occupied radii. Use symmetry only after the radii and shell heights are established.

The same reasoning applies to horizontal shells about a horizontal axis: use horizontal slices, compare their distances to the axis, and combine the corresponding horizontal extents at each shared radius. Symmetry is a tool for organizing the geometry, not a substitute for determining what the rotated solid actually contains.

Common Mistakes to Avoid

  • Doubling a half-integral without checking the axis. This is justified only when the paired slices contribute the same shells in the way the setup requires. A symmetry axis different from the rotation axis usually changes the paired radii.
  • Adding heights that overlap. If two source slices produce the same radius, their combined shell height is the union of their vertical extents. Overlapping portions count once.
  • Using the outermost boundary as the height across a gap. If the shell’s vertical set has separate pieces, its total height is the sum of the lengths of those pieces, not the length of an interval that includes empty space.
  • Integrating over both sides when they describe the same shells. For a region symmetric about its rotation axis, mirrored slices at the same radius duplicate the same shell. Count that radius once.

Why the Distinction Matters

A symmetry argument can make a correct integral shorter, but a careless one can change the solid being measured. Matching boundaries alone is not enough: the radius determines which cylindrical shell is involved, and the union of the slice extents determines its height. Checking both prevents duplicate shells and duplicate heights.

Before using a symmetry shortcut, describe one typical shell in words: its radius, the source slices that generate it, and the heights it reaches. If a mirrored slice produces the same radius, combine the extents. If it produces a different radius, keep its distinct radius in the integral. This geometric check is often quicker than repairing a double-counted integral later.

Check Your Understanding

For each problem, identify the radii and shell heights before deciding whether symmetry reduces the integral.

  1. A region is symmetric about the \(y\)-axis and is rotated about the \(y\)-axis. Why do slices at \(x=r\) and \(x=-r\) not represent two separate shells?
  2. At radius \(r\), two slices have extents \([0,2]\) and \([1,3]\). What is the union of their extents, and what is its length?
  3. A region is symmetric about \(x=0\) and rotated about \(x=2\). What are the radii of the slices at \(x\) and \(-x\), for \(0\le x\le1\)?
  4. When can the lengths of two vertical extents at the same shell radius be added?
  5. If a shell’s vertical extent consists of two disjoint intervals, should its height include the gap between them? Explain.

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