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Chapter 6 · Application of Derivatives

Exercise 6.3 · Q25: Given slant height, greatest volume: angle tan⁡−12\tan^{-1}\sqrt{2}

Exercise 6.3Optimisation · Section 6.4
The question

25. Show that the semi-vertical angle of the cone of the maximum volume and of given slant height is tan⁡−12\tan^{-1}\sqrt{2}⁠.

Exam answer

Let θ\theta be the semi-vertical angle and ll the given slant height, 0<θ<π20 < \theta < \frac{\pi}{2}⁠. Then r=lsin⁡θr = l\sin\theta and h=lcos⁡θh = l\cos\theta⁠.

V(θ)=13πr2h=πl33sin⁡2θcos⁡θ\begin{aligned} V(\theta) &= \frac13\pi r^2 h \\ &= \frac{\pi l^3}{3}\sin^2\theta\cos\theta \end{aligned} V′(θ)=πl33(2sin⁡θcos⁡2θ−sin⁡3θ)=πl33sin⁡θcos⁡2θ×(2−tan⁡2θ)\begin{aligned} V'(\theta) &= \frac{\pi l^3}{3}\big(2\sin\theta\cos^2\theta \\ &\qquad - \sin^3\theta\big) \\ &= \frac{\pi l^3}{3}\sin\theta\cos^2\theta \\ &\qquad\times(2 - \tan^2\theta) \end{aligned}

V′(θ)=0⇒tan⁡2θ=2V'(\theta) = 0 \Rightarrow \tan^2\theta = 2⁠, so tan⁡θ=2\tan\theta = \sqrt2 (as θ\theta is acute).

V′′(θ)=πl33cos⁡θ (2cos⁡2θ−7sin⁡2θ)\begin{aligned} V''(\theta) &= \frac{\pi l^3}{3}\cos\theta\,\big(2\cos^2\theta \\ &\qquad - 7\sin^2\theta\big) \end{aligned}

When tan⁡θ=2\tan\theta = \sqrt2⁠, cos⁡2θ=13\cos^2\theta = \frac13 and sin⁡2θ=23\sin^2\theta = \frac23⁠, so

V′′(θ)=πl33⋅13⋅(−4)<0V''(\theta) = \frac{\pi l^3}{3}\cdot\frac{1}{\sqrt3}\cdot(-4) < 0

So VV is maximum at θ=tan⁡−12\theta = \tan^{-1}\sqrt2⁠. V′V' is positive before this point and negative after it, so this is the greatest volume.

∴\therefore The semi-vertical angle of the cone of maximum volume is tan⁡−12\tan^{-1}\sqrt2⁠. Hence proved.

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

The one idea this problem is built on

Picture a cone made of fixed-length sticks (the slant height ll⁠) hinged at the apex. Close the sticks up and the cone is tall but thin; open them out and it is wide but flat. Both extremes hold almost nothing. The semi-vertical angle θ\theta describes every cone in between, and since the radius is lsin⁡θl\sin\theta and the height lcos⁡θl\cos\theta⁠, the volume is a trigonometric function of θ\theta alone. Its maximum is where tan⁡θ=2\tan\theta = \sqrt{2}⁠.

Given, to show, and the plan
Given
Right circular cones all with the same slant height ll (a fixed positive number).
To show
The cone of greatest volume has semi-vertical angle θ=tan⁡−12\theta = \tan^{-1}\sqrt{2}⁠.
Plan
Take θ\theta as the variable, 0<θ<π20 < \theta < \frac{\pi}{2}⁠; write rr⁠, hh and then VV in terms of θ\theta⁠; find where V′(θ)=0V'(\theta) = 0⁠; apply the second derivative test; prove from the sign of V′V' that this is the greatest volume of all such cones.

Basics you need

1The cone's right triangle

The axis (height hh⁠), a base radius rr and the slant side ll form a right triangle with the right angle at the centre of the base. The semi-vertical angle θ\theta is the angle at the apex between the axis and the slant side. So r=lsin⁡θr = l\sin\theta and h=lcos⁡θh = l\cos\theta⁠. Basics: area and volume formulas

2Sine, cosine and tangent in the first quadrant

For 0<θ<π20 < \theta < \frac{\pi}{2}⁠: sin⁡θ>0\sin\theta > 0⁠, cos⁡θ>0\cos\theta > 0⁠, and tan⁡θ\tan\theta increases from 0 towards ∞\infty⁠. Also cos⁡2θ=11+tan⁡2θ\cos^2\theta = \frac{1}{1 + \tan^2\theta}⁠. Basics: signs of sin and cos

3Derivatives of sin⁡\sin and cos⁡\cos⁠, and the chain rule

ddθsin⁡θ=cos⁡θ\frac{d}{d\theta}\sin\theta = \cos\theta⁠, ddθcos⁡θ=−sin⁡θ\frac{d}{d\theta}\cos\theta = -\sin\theta⁠; for example ddθsin⁡2θ=2sin⁡θcos⁡θ\frac{d}{d\theta}\sin^2\theta = 2\sin\theta\cos\theta⁠. Basics: the chain rule

4Second derivative test, and from local to greatest

V′(c)=0V'(c) = 0⁠, V′′(c)<0V''(c) < 0 gives a local maximum (Theorem 4, Section 6.4); the sign of V′V' over the whole range proves it is the greatest. Lesson: first and second derivative tests

Solution

  1. The variable and its range

    Let θ\theta be the semi-vertical angle of a cone with slant height ll⁠. In the right triangle formed by the axis, a base radius and the slant side (Basic 1),

    r=lsin⁡θ,h=lcos⁡θ.r = l\sin\theta, \qquad h = l\cos\theta.

    A genuine cone needs r>0r > 0 and h>0h > 0⁠, which happens exactly for 0<θ<π20 < \theta < \frac{\pi}{2}⁠; every such θ\theta gives a cone of slant height ll⁠.

    θ r = l sin θ h = l cos θ l (fixed) drawn for tan θ = √2, θ ≈ 54.7°
    A cone of fixed slant height ll and semi-vertical angle θ\theta⁠: radius lsin⁡θl\sin\theta⁠, height lcos⁡θl\cos\theta⁠. Drawn for the answer, tan⁡θ=2\tan\theta = \sqrt{2}⁠, θ≈54.7∘\theta \approx 54.7^\circ⁠.
    The question asks about the angle, so the angle is the natural variable. With ll fixed, θ\theta alone decides the cone. At θ=0\theta = 0 the cone collapses to a line, at θ=π2\theta = \frac{\pi}{2} to a flat disc, so both ends are excluded.
    In a right triangle, the side opposite an angle is hypotenuse × sine and the adjacent side is hypotenuse × cosine; here the hypotenuse is ll⁠, the opposite side rr and the adjacent side hh⁠. Basics: interval notation
  2. The volume as a function of θ\theta

    V(θ)=13πr2h=13π (lsin⁡θ)2 (lcos⁡θ)=πl33 sin⁡2θ cos⁡θ,0<θ<π2.\begin{aligned} V(\theta) &= \frac{1}{3}\pi r^2 h = \frac{1}{3}\pi\,(l\sin\theta)^2\,(l\cos\theta) \\ &= \frac{\pi l^3}{3}\,\sin^2\theta\,\cos\theta, \quad 0 < \theta < \frac{\pi}{2}. \end{aligned}
    This is the quantity to maximise. The factor πl33\frac{\pi l^3}{3} is a positive constant, so all the variation is in sin⁡2θcos⁡θ\sin^2\theta\cos\theta⁠.
    Volume of a cone 13πr2h\frac{1}{3}\pi r^2 h⁠. Basics: building the function to optimise
  3. Differentiate

    Product rule, with ddθsin⁡2θ=2sin⁡θcos⁡θ\frac{d}{d\theta}\sin^2\theta = 2\sin\theta\cos\theta (chain rule) and ddθcos⁡θ=−sin⁡θ\frac{d}{d\theta}\cos\theta = -\sin\theta⁠:

    V′(θ)=πl33(2sin⁡θcos⁡2θ−sin⁡3θ)=πl33 sin⁡θ(2cos⁡2θ−sin⁡2θ)=πl33 sin⁡θcos⁡2θ(2−tan⁡2θ).\begin{aligned} V'(\theta) &= \frac{\pi l^3}{3}\left(2\sin\theta\cos^2\theta - \sin^3\theta\right) \\ &= \frac{\pi l^3}{3}\,\sin\theta\left(2\cos^2\theta - \sin^2\theta\right) \\ &= \frac{\pi l^3}{3}\,\sin\theta\cos^2\theta\left(2 - \tan^2\theta\right). \end{aligned}
    The last line divides the bracket by cos⁡2θ\cos^2\theta and multiplies it back outside, which is allowed because cos⁡θ≠0\cos\theta \ne 0 on (0,π2)\left(0, \frac{\pi}{2}\right)⁠. It leaves one factor whose sign can change, 2−tan⁡2θ2 - \tan^2\theta⁠, and that is the form we want for both the zero and the sign.
    Product rule: (uv)′=u′v+uv′(uv)' = u'v + uv' with u=sin⁡2θu = \sin^2\theta⁠, v=cos⁡θv = \cos\theta⁠. Chain rule: inner sin⁡θ\sin\theta⁠, outer u2u^2⁠. Basics: the chain rule
  4. The critical point

    On (0,π2)\left(0, \frac{\pi}{2}\right)⁠, sin⁡θ>0\sin\theta > 0 and cos⁡2θ>0\cos^2\theta > 0⁠. So V′(θ)=0V'(\theta) = 0 exactly when tan⁡2θ=2\tan^2\theta = 2⁠, and since tan⁡θ>0\tan\theta > 0 there,

    tan⁡θ=2,θ=tan⁡−12.\tan\theta = \sqrt{2}, \qquad \theta = \tan^{-1}\sqrt{2}.

    The principal value tan⁡−12\tan^{-1}\sqrt{2} lies in (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) and is positive because 2>0\sqrt{2} > 0⁠, so it is in our range (0,π2)\left(0, \frac{\pi}{2}\right)⁠. Because tan⁡\tan is strictly increasing on this interval, it takes the value 2\sqrt{2} only once: this is the only critical point. Call it θ0\theta_0 (about 54.7356∘54.7356^\circ⁠).

    We reject tan⁡θ=−2\tan\theta = -\sqrt{2} because the tangent of an angle between 0 and π2\frac{\pi}{2} is positive. Writing the answer as tan⁡−12\tan^{-1}\sqrt{2} is valid precisely because θ0\theta_0 lies inside the principal range of tan⁡−1\tan^{-1}⁠.
    Range of the principal value branch of tan⁡−1\tan^{-1} is (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) (Chapter 2). Basics: signs of sin and cos
  5. Second derivative test

    Differentiate 2sin⁡θcos⁡2θ−sin⁡3θ2\sin\theta\cos^2\theta - \sin^3\theta term by term:

    V′′(θ)=πl33(2cos⁡3θ−7sin⁡2θcos⁡θ)=πl33cos⁡θ(2cos⁡2θ−7sin⁡2θ).\begin{aligned} V''(\theta) &= \frac{\pi l^3}{3}\left(2\cos^3\theta - 7\sin^2\theta\cos\theta\right) \\ &= \frac{\pi l^3}{3}\cos\theta\left(2\cos^2\theta - 7\sin^2\theta\right). \end{aligned}

    At θ0\theta_0⁠, tan⁡2θ0=2\tan^2\theta_0 = 2 gives cos⁡2θ0=13\cos^2\theta_0 = \frac{1}{3} and sin⁡2θ0=23\sin^2\theta_0 = \frac{2}{3}⁠, so the bracket is 23−143=−4\frac{2}{3} - \frac{14}{3} = -4 and

    V′′(θ0)=πl33⋅13⋅(−4)<0.V''(\theta_0) = \frac{\pi l^3}{3}\cdot\frac{1}{\sqrt{3}}\cdot(-4) < 0.

    By the second derivative test, θ0\theta_0 is a point of local maxima of VV⁠.

    For the first term, by the product rule, ddθ(2sin⁡θcos⁡2θ)\frac{d}{d\theta}(2\sin\theta\cos^2\theta) equals 2cos⁡3θ−4sin⁡2θcos⁡θ2\cos^3\theta - 4\sin^2\theta\cos\theta⁠; for the second, ddθsin⁡3θ=3sin⁡2θcos⁡θ\frac{d}{d\theta}\sin^3\theta = 3\sin^2\theta\cos\theta⁠. Together: 2cos⁡3θ−7sin⁡2θcos⁡θ2\cos^3\theta - 7\sin^2\theta\cos\theta⁠.
    Theorem 4 (i), Section 6.4. cos⁡2θ=11+tan⁡2θ=13\cos^2\theta = \frac{1}{1 + \tan^2\theta} = \frac{1}{3} and sin⁡2θ=1−cos⁡2θ\sin^2\theta = 1 - \cos^2\theta⁠. Lesson: first and second derivative tests
  6. It is the greatest volume of all

    From Step 3, V′(θ)V'(\theta) has the sign of 2−tan⁡2θ2 - \tan^2\theta on (0,π2)\left(0, \frac{\pi}{2}\right)⁠. As tan⁡θ\tan\theta increases through 2\sqrt{2}⁠:

    • for 0<θ<θ00 < \theta < \theta_0⁠: 0<tan⁡θ<20 < \tan\theta < \sqrt{2}⁠, so V′(θ)>0V'(\theta) > 0⁠;
    • for θ0<θ<π2\theta_0 < \theta < \frac{\pi}{2}⁠: tan⁡θ>2\tan\theta > \sqrt{2}⁠, so V′(θ)<0V'(\theta) < 0⁠.

    So VV increases on (0,θ0](0, \theta_0] and decreases on [θ0,π2)\left[\theta_0, \frac{\pi}{2}\right)⁠: V(θ)<V(θ0)V(\theta) < V(\theta_0) for every other allowed θ\theta⁠. At both ends V→0V \to 0 (sin⁡θ→0\sin\theta \to 0 at one end, cos⁡θ→0\cos\theta \to 0 at the other).

    "Cone of the maximum volume" means greatest among all cones with this slant height. One critical point, with VV rising before it and falling after it, is the top of the whole graph.
  7. Conclusion, and a cross-check with the height

    The volume is greatest when the semi-vertical angle is θ=tan⁡−12\theta = \tan^{-1}\sqrt{2}. Its value is V(θ0)=πl33⋅23⋅13V(\theta_0) = \frac{\pi l^3}{3}\cdot\frac{2}{3}\cdot\frac{1}{\sqrt{3}} =23 πl327= \frac{2\sqrt{3}\,\pi l^3}{27}⁠.

    Cross-check using the height as the variable: r2=l2−h2r^2 = l^2 - h^2⁠, so V=π3(l2h−h3)V = \frac{\pi}{3}(l^2 h - h^3) on 0<h<l0 < h < l⁠, and V′=π3(l2−3h2)=0V' = \frac{\pi}{3}(l^2 - 3h^2) = 0 gives h=l3h = \frac{l}{\sqrt{3}}⁠. Then r=l2−l23=23 lr = \sqrt{l^2 - \frac{l^2}{3}} = \sqrt{\frac{2}{3}}\,l⁠, and tan⁡θ=rh=2\tan\theta = \frac{r}{h} = \sqrt{2}⁠, the same angle.

    Two different choices of variable lead to the same cone, which is strong evidence that no slip was made. The second route avoids trigonometry until the very end.
    tan⁡θ=oppositeadjacent=rh\tan\theta = \frac{\text{opposite}}{\text{adjacent}} = \frac{r}{h} in the cone's right triangle.
Result

For cones of given slant height ll⁠, the volume πl33sin⁡2θcos⁡θ\frac{\pi l^3}{3}\sin^2\theta\cos\theta is greatest exactly when tan⁡θ=2\tan\theta = \sqrt{2}⁠. So the semi-vertical angle of the cone of maximum volume is tan⁡−12\tan^{-1}\sqrt{2} (about 54.7∘54.7^\circ⁠), as was to be shown. The maximum volume is 23 πl327\frac{2\sqrt{3}\,\pi l^3}{27}⁠.

Check it with numbers

Take l=1l = 1⁠, so V(θ)=π3sin⁡2θcos⁡θV(\theta) = \frac{\pi}{3}\sin^2\theta\cos\theta⁠:

θ\theta45°50°54.7356°60°65°
VV0.37020.39500.40310.39270.3635

The largest value is at θ≈54.7356∘\theta \approx 54.7356^\circ⁠, where tan⁡θ≈1.4142=2\tan\theta \approx 1.4142 = \sqrt{2}⁠, and 23π27≈0.4031\frac{2\sqrt{3}\pi}{27} \approx 0.4031⁠.

Common mistakes
  1. Swapping sine and cosine. θ\theta is measured from the axis, so the radius (opposite θ\theta⁠) is lsin⁡θl\sin\theta and the height (adjacent) is lcos⁡θl\cos\theta⁠. Swapping them gives cot⁡θ=2\cot\theta = \sqrt{2}⁠, the wrong angle.
  2. Dividing by sin⁡θ\sin\theta or cos⁡θ\cos\theta without comment. It is allowed only because both are non-zero on (0,π2)\left(0, \frac{\pi}{2}\right)⁠; say so.
  3. Keeping tan⁡θ=−2\tan\theta = -\sqrt{2}⁠. A semi-vertical angle is acute, so its tangent is positive.
  4. Stopping at V′′(θ0)<0V''(\theta_0) < 0⁠. That proves a local maximum only; the sign of V′V' over the whole range (Step 6) proves it is the greatest.
What to take away
  1. When the answer is an angle, use the angle as the variable and express lengths with sin⁡\sin and cos⁡\cos⁠.
  2. Factor the derivative so that one simple factor carries the sign, here 2−tan⁡2θ2 - \tan^2\theta⁠.
  3. Compare Q24 (given volume, least curved surface: tan⁡θ=12\tan\theta = \frac{1}{\sqrt{2}}⁠) and Q26 (given surface area, greatest volume: sin⁡θ=13\sin\theta = \frac{1}{3}⁠): what is held fixed changes the best shape.

Every fact used, and where it comes from

FactUsed inSource
r=lsin⁡θr = l\sin\theta⁠, h=lcos⁡θh = l\cos\theta⁠, volume 13πr2h\frac{1}{3}\pi r^2 hSteps 1, 2Right-triangle trigonometry; mensuration (Basics: formulas)
Product and chain rules; derivatives of sin⁡\sin⁠, cos⁡\cosSteps 3, 5Chapter 5 (Basics: chain rule)
Principal range of tan⁡−1\tan^{-1} is (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right)Step 4Chapter 2, Inverse Trigonometric Functions
Extrema in an open interval only at critical pointsStep 4Theorem 2, Section 6.4
Second Derivative TestStep 5Theorem 4, Section 6.4 (Lesson: tests)
Sign of the derivative and increasing/decreasingStep 6Theorem 1, Section 6.3
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