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Chapter 6 · Application of Derivatives

Exercise 6.3 · Q21: Closed can of 100 cm³ with least surface: h=2rh = 2r

Exercise 6.3Optimisation · Section 6.4
The question

21. Of all the closed cylindrical cans (right circular), of a given volume of 100 cubic centimetres, find the dimensions of the can which has the minimum surface area?

Exam answer

Let the radius be rr cm and the height hh cm, r>0r > 0⁠. Then

πr2h=100⇒h=100πr2\pi r^2 h = 100 \Rightarrow h = \frac{100}{\pi r^2}

The total surface area is

S=2πr2+2πrh=2πr2+200r\begin{aligned} S &= 2\pi r^2 + 2\pi rh \\ &= 2\pi r^2 + \frac{200}{r} \end{aligned} S′(r)=4πr−200r2S′′(r)=4π+400r3\begin{aligned} S'(r) &= 4\pi r - \frac{200}{r^2} \\ S''(r) &= 4\pi + \frac{400}{r^3} \end{aligned}

S′(r)=0⇒r3=50πS'(r) = 0 \Rightarrow r^3 = \frac{50}{\pi}⁠, so r=(50π)1/3r = \left(\frac{50}{\pi}\right)^{1/3}⁠.

As S′′(r)>0S''(r) > 0⁠, SS is minimum there. S′S' is negative before this point and positive after it, so this is the least surface area.

Since πr3=50\pi r^3 = 50⁠,

h=100πr2=2πr3πr2=2rh = \frac{100}{\pi r^2} = \frac{2\pi r^3}{\pi r^2} = 2r

∴\therefore Radius =(50π)1/3= \left(\dfrac{50}{\pi}\right)^{1/3} cm and height =2(50π)1/3= 2\left(\dfrac{50}{\pi}\right)^{1/3} cm.

Want the reason behind every step, the basics and the checks?

The one idea this problem is built on

A can has two dimensions, radius rr and height hh⁠, but the fixed volume ties them together: once rr is chosen, hh is forced. So the surface area is really a function of one variable, rr⁠. A very thin can wastes metal on its tall side; a very flat can wastes metal on its two big lids. Calculus finds the balance point in between, and it turns out to be the can whose height equals its diameter.

Given, to find, and the plan
Given
A closed right circular cylinder (both ends covered) with volume πr2h=100\pi r^2 h = 100 cm³.
To find
The radius rr and height hh that make the total surface area as small as possible.
Plan
Use the volume to write hh in terms of rr⁠; write the surface area SS as a function of rr alone on r>0r > 0⁠; find the critical point; use the second derivative test; then prove from the sign of S′S' that this point gives the least value among all cans, not just nearby ones.

Basics you need

1Volume and surface area of a cylinder

Radius rr⁠, height hh⁠: volume πr2h\pi r^2 h⁠; curved surface 2πrh2\pi r h (the side unrolls into a rectangle 2πr2\pi r wide and hh tall); each circular end has area πr2\pi r^2⁠. A closed can has both ends, so its total surface area is 2πr2+2πrh2\pi r^2 + 2\pi r h⁠. Basics: area and volume formulas

2Building the function to optimise

Name the quantity to minimise, use the given condition (the "constraint") to remove all but one variable, and state the range of that variable. Basics: building the function to optimise

3Second derivative test (Theorem 4, Section 6.4)

If S′(c)=0S'(c) = 0 and S′′(c)>0S''(c) > 0⁠, then cc is a point of local minima. Lesson: first and second derivative tests

4From local to least

A local minimum only beats nearby values. To show it is the least value on the whole range, look at the sign of S′S' on each side of cc all the way to the ends of the range (the Mean Value Theorem, as in the proof of Theorem 1, Section 6.3). Lesson: optimisation problems

Solution

  1. Name the variables and use the volume

    Let the can have radius rr cm and height hh cm. The volume is fixed:

    πr2h=100,soh=100πr2.\pi r^2 h = 100, \qquad\text{so}\qquad h = \frac{100}{\pi r^2}.

    Every positive rr gives a positive hh and hence a genuine can, so the allowed range is r>0r > 0⁠, that is r∈(0,∞)r \in (0, \infty)⁠.

    r h V = 100 cm³ Least surface: r ≈ 2.52 cm h ≈ 5.03 cm h = 2r drawn to scale, 1 cm = 40 px
    The can with radius rr and height hh⁠, drawn to scale at the answer found below: r≈2.52r \approx 2.52 cm, h≈5.03h \approx 5.03 cm, so the height equals the diameter.
    The surface area depends on both rr and hh⁠, but we cannot vary them independently: making the can wider forces it to be shorter to keep 100 cm³. Solving the volume equation for hh expresses that link, and leaves a single variable to work with.
    r=0r = 0 is excluded (no can at all), and there is no upper limit on rr⁠: a very wide can is simply very flat. Basics: interval notation
  2. The surface area as a function of rr

    Two ends plus the curved side:

    S=2πr2+2πrh=2πr2+2πr⋅100πr2=2πr2+200r,r>0.\begin{aligned} S &= 2\pi r^2 + 2\pi r h \\ &= 2\pi r^2 + 2\pi r \cdot \frac{100}{\pi r^2} \\ &= 2\pi r^2 + \frac{200}{r}, \qquad r > 0. \end{aligned}
    This is the quantity to make as small as possible. The two terms pull in opposite directions: 2πr22\pi r^2 (the lids) grows as rr grows, while 200r\frac{200}{r} (the side) shrinks. The best can is where neither wins outright.
    Closed can: both circular ends count, so 2πr22\pi r^2⁠, not πr2\pi r^2 (Basic 1). Basics: building the function to optimise
  3. Differentiate and find the critical point

    S′(r)=4πr−200r2=4πr3−200r2=4πr2(r3−50π).\begin{aligned} S'(r) &= 4\pi r - \frac{200}{r^2} \\ &= \frac{4\pi r^3 - 200}{r^2} \\ &= \frac{4\pi}{r^2}\left(r^3 - \frac{50}{\pi}\right). \end{aligned}

    Since 4πr2>0\frac{4\pi}{r^2} > 0⁠, S′(r)=0S'(r) = 0 exactly when

    r3=50π,r=(50π)1/3.r^3 = \frac{50}{\pi}, \qquad r = \left(\frac{50}{\pi}\right)^{1/3}.

    Call this value cc⁠. A real number has exactly one real cube root, so cc is the only critical point in (0,∞)(0, \infty)⁠; SS is differentiable at every r>0r > 0⁠, so there are no others.

    Points of local maxima or minima inside an open interval can only be where the derivative is zero or does not exist (Theorem 2, Section 6.4). Writing S′S' as a positive factor times (r3−50π)\left(r^3 - \frac{50}{\pi}\right) makes both the zero and, in Step 5, the sign easy to read.
    Power rule: ddr(2πr2)=4πr\frac{d}{dr}(2\pi r^2) = 4\pi r and ddr(200r−1)=−200r−2\frac{d}{dr}(200 r^{-1}) = -200 r^{-2}⁠.
  4. Second derivative test

    S′′(r)=4π+400r3.S''(r) = 4\pi + \frac{400}{r^3}.

    For every r>0r > 0 both terms are positive, so in particular S′′(c)>0S''(c) > 0⁠. By the second derivative test, r=cr = c is a point of local minima of SS⁠.

    S′′>0S'' > 0 means the slope S′S' is increasing: the graph of SS bends upwards like a valley, so the flat point is the bottom of a valley.
    Theorem 4 (ii), Section 6.4. ddr(−200r−2)=400r−3\frac{d}{dr}(-200 r^{-2}) = 400 r^{-3}⁠. Lesson: first and second derivative tests
  5. It is the least value among all cans

    From Step 3, S′(r)S'(r) has the sign of r3−50πr^3 - \frac{50}{\pi}⁠, and r3r^3 increases with rr⁠:

    • for 0<r<c0 < r < c⁠: r3<c3=50πr^3 < c^3 = \frac{50}{\pi}⁠, so S′(r)<0S'(r) < 0⁠;
    • for r>cr > c⁠: r3>50πr^3 > \frac{50}{\pi}⁠, so S′(r)>0S'(r) > 0⁠.

    Take any allowed r≠cr \ne c⁠. By the Mean Value Theorem on the interval between rr and cc⁠, S(r)−S(c)=S′(ξ)(r−c)S(r) - S(c) = S'(\xi)(r - c) for some ξ\xi strictly between them. If r<cr < c⁠, then S′(ξ)<0S'(\xi) < 0 and r−c<0r - c < 0⁠; if r>cr > c⁠, then S′(ξ)>0S'(\xi) > 0 and r−c>0r - c > 0⁠. Either way the product is positive, so

    S(r)>S(c)for every r>0, r≠c.S(r) > S(c) \quad\text{for every } r > 0,\ r \ne c.

    The ends of the range agree: as r→0+r \to 0^+⁠, 200r→∞\frac{200}{r} \to \infty⁠; as r→∞r \to \infty⁠, 2πr2→∞2\pi r^2 \to \infty⁠. So SS falls all the way down to r=cr = c and rises all the way after it.

    The second derivative test only says cc beats its neighbours. The question asks for the minimum among all cans, so we need the sign of S′S' on the whole range (0,∞)(0, \infty)⁠. One critical point, with SS decreasing before it and increasing after it, means it is the lowest point of the entire graph.
    This is the argument in the proof of Theorem 1, Section 6.3 (a negative derivative means decreasing, a positive one increasing), which rests on the Mean Value Theorem. (The book's proof calls it "Theorem 8 in Chapter 5"; that theorem is not printed in this reprint's Chapter 5, but the statement used is exactly the one above.) Lesson: increasing and decreasing functions
  6. The height of the best can

    From c3=50πc^3 = \frac{50}{\pi} we get πc3=50\pi c^3 = 50⁠, so 100=2πc3100 = 2\pi c^3⁠. Then

    h=100πc2=2πc3πc2=2c=2(50π)1/3.h = \frac{100}{\pi c^2} = \frac{2\pi c^3}{\pi c^2} = 2c = 2\left(\frac{50}{\pi}\right)^{1/3}.

    So the height is twice the radius: the height equals the diameter of the base.

    Using πc3=50\pi c^3 = 50 avoids messy fractional powers and shows the shape of the answer at once. This matches Q20 just before, where the same h=2rh = 2r appears for a fixed surface and maximum volume: the two problems are two views of the same best shape.
    Substitute only after differentiating: the formula h=100πr2h = \frac{100}{\pi r^2} from Step 1 now gives the height for the chosen r=cr = c⁠.
  7. The numbers, and the least surface area

    50π≈15.9155\frac{50}{\pi} \approx 15.9155⁠, so c≈2.5154c \approx 2.5154 cm and h=2c≈5.0308h = 2c \approx 5.0308 cm. Since 200=4πc3200 = 4\pi c^3⁠, the side term is 200c=4πc2\frac{200}{c} = 4\pi c^2⁠, and

    S(c)=2πc2+4πc2=6πc2≈119.27 cm2.S(c) = 2\pi c^2 + 4\pi c^2 = 6\pi c^2 \approx 119.27 \text{ cm}^2.
    The question asks only for the dimensions; the area is a useful extra and is what the numerical check below compares against.
Result

The can of least surface area has radius (50π)1/3\left(\frac{50}{\pi}\right)^{1/3} cm (about 2.52 cm) and height 2(50π)1/32\left(\frac{50}{\pi}\right)^{1/3} cm (about 5.03 cm): its height equals its diameter. Its surface area is 6π(50π)2/3≈119.276\pi\left(\frac{50}{\pi}\right)^{2/3} \approx 119.27 cm².

(Textbook answer: radius =(50π)1/3= \left(\frac{50}{\pi}\right)^{1/3} cm and height =2(50π)1/3= 2\left(\frac{50}{\pi}\right)^{1/3} cm. Agrees.)

Check it with numbers

S(r)=2πr2+200rS(r) = 2\pi r^2 + \frac{200}{r} at a few radii (in cm²):

rr (cm)22.52.51543
S(r)S(r)125.1327119.2699119.2654123.2153

The smallest value is at r≈2.5154r \approx 2.5154⁠, and it beats r=2.5r = 2.5 only in the fourth significant figure: near the minimum the graph is very flat, which is why a can a little off the ideal shape costs almost no extra metal.

Common mistakes
  1. Leaving out a lid. A closed can has two ends: S=2πr2+2πrhS = 2\pi r^2 + 2\pi r h⁠. With only one end (an open can) the answer changes to h=rh = r⁠.
  2. Differentiating with two variables. S=2πr2+2πrhS = 2\pi r^2 + 2\pi r h cannot be differentiated with respect to rr while hh is treated as a constant: hh changes with rr⁠. Substitute h=100πr2h = \frac{100}{\pi r^2} first.
  3. Stopping at the second derivative test. It proves a local minimum only. The sign of S′S' over the whole range (Step 5) is what proves it is the least surface area of all.
  4. Wrong power of the cube root. r3=50πr^3 = \frac{50}{\pi} gives r=(50π)1/3r = \left(\frac{50}{\pi}\right)^{1/3}⁠, not (50π)1/2\left(\frac{50}{\pi}\right)^{1/2}⁠.
What to take away
  1. Use the fixed quantity (here the volume) to reduce the problem to one variable, and state that variable's range.
  2. Factor the derivative as (positive factor) × (simple expression): the zero and the sign on each side can then be read off directly.
  3. The closed can of least surface for a given volume has height equal to its diameter, whatever the volume (100 cm³ only fixes the size).

Every fact used, and where it comes from

FactUsed inSource
Volume πr2h\pi r^2 h⁠; surface 2πr2+2πrh2\pi r^2 + 2\pi r hSteps 1, 2Mensuration (Basics: formulas)
Extrema in an open interval only at critical pointsStep 3Theorem 2 and the Note after it, Section 6.4
Second Derivative TestStep 4Theorem 4, Section 6.4 (Lesson: tests)
Sign of the derivative and increasing/decreasingStep 5Theorem 1, Section 6.3, and the Mean Value Theorem used in its proof
Height equals diameter (Q20)Step 6Exercise 6.3, Q20
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