[The volume of a cone of base radius rr and height hh is given by V=13πr2hV = \frac{1}{3}\pi r^2 h.] A manufacturer makes a funnel-shaped ornament from the same material which consists of two parts as shown in Figure 1.
  • a right cone of radius rr cm, height hh cm and a slant height of 4 cm,
  • a cylinder with radius arar cm and height rr cm, where 0<a<10 < a < 1.
From the original cone, a similar cone with radius arar cm is removed from the vertex as shown in Figure 2. The remaining part of the cone is joined to the cylinder to form the funnel as shown in Figure 3. It may be assumed that the thickness of the funnel is negligible. Given that the volume of the ornament is V cm3V\text{ cm}^3, find VV in terms of aa and rr.

  1. (a)

    For the remainder of this question, assume that a=0.25a = 0.25.

    The manufacturer wants VV to be a maximum. If r=r1r = r_1 gives the maximum value of VV, show that r1r_1 satisfies the equation 457r4−9664r2+50176=0457r^4 - 9664r^2 + 50176 = 0.

  2. (b)

    Show that one of the positive roots to the equation in part (a) does not give a stationary value of VV. Hence find the value of hh for which VV is stationary.

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Worked solution

5(a)

1. Express the total volume $V$ in terms of $r$ by evaluating the volumes of the frustum and cylinder.

From the given information, the slant height of the original cone is 44. Let its vertical height be hh. By Pythagoras' Theorem:
r2+h2=42  ⟹  h=16−r2r^2 + h^2 = 4^2 \implies h = \sqrt{16 - r^2}

The similar cone removed from the vertex has radius arar and, by similarity, height ahah.
Volume of the frustum = 13πr2h−13π(ar)2(ah)=13πr2h(1−a3)\frac{1}{3}\pi r^2 h - \frac{1}{3}\pi (ar)^2 (ah) = \frac{1}{3}\pi r^2 h (1 - a^3)
Volume of the cylinder = π(ar)2(r)=πa2r3\pi (ar)^2(r) = \pi a^2 r^3

Total volume VV:
V=13πr216−r2(1−a3)+πa2r3V = \frac{1}{3}\pi r^2 \sqrt{16 - r^2} (1 - a^3) + \pi a^2 r^3

2. Substitute $a = 0.25$ to express $V$ solely in terms of $r$.

Given a=0.25=14a = 0.25 = \frac{1}{4}:
a2=116a^2 = \frac{1}{16}
a3=164  ⟹  1−a3=6364a^3 = \frac{1}{64} \implies 1 - a^3 = \frac{63}{64}

Substitute into VV:
V=13πr216−r2(6364)+π(116)r3V = \frac{1}{3}\pi r^2 \sqrt{16 - r^2} \left(\frac{63}{64}\right) + \pi \left(\frac{1}{16}\right) r^3
V=21π64r216−r2+π16r3V = \frac{21\pi}{64} r^2 \sqrt{16 - r^2} + \frac{\pi}{16} r^3
V=π64[21r216−r2+4r3]V = \frac{\pi}{64} \left[ 21r^2 \sqrt{16 - r^2} + 4r^3 \right]

3. Differentiate $V$ with respect to $r$ using the product and chain rules.

dVdr=π64[ddr(21r2(16−r2)1/2)+ddr(4r3)]\frac{dV}{dr} = \frac{\pi}{64} \left[ \frac{d}{dr}\left(21r^2 (16 - r^2)^{1/2}\right) + \frac{d}{dr}\left(4r^3\right) \right]

Applying the product rule on the first term:
dVdr=π64[42r(16−r2)1/2+21r2(12)(16−r2)−1/2(−2r)+12r2]\frac{dV}{dr} = \frac{\pi}{64} \left[ 42r (16 - r^2)^{1/2} + 21r^2 \left(\frac{1}{2}\right)(16 - r^2)^{-1/2}(-2r) + 12r^2 \right]
dVdr=π64[42r16−r2−21r316−r2+12r2]\frac{dV}{dr} = \frac{\pi}{64} \left[ 42r \sqrt{16 - r^2} - \frac{21r^3}{\sqrt{16 - r^2}} + 12r^2 \right]

4. Equate $\frac{dV}{dr}$ to 0 for a maximum value and substitute $r = r_1$.

For VV to be a maximum, dVdr=0\frac{dV}{dr} = 0. Let r=r1r = r_1.
π64[42r116−r12−21r1316−r12+12r12]=0\frac{\pi}{64} \left[ 42r_1 \sqrt{16 - r_1^2} - \frac{21r_1^3}{\sqrt{16 - r_1^2}} + 12r_1^2 \right] = 0

Since r1>0r_1 > 0, divide the entire equation by 3r13r_1:
1416−r12−7r1216−r12+4r1=014 \sqrt{16 - r_1^2} - \frac{7r_1^2}{\sqrt{16 - r_1^2}} + 4r_1 = 0

Multiply through by 16−r12\sqrt{16 - r_1^2} to clear the denominator:
14(16−r12)−7r12+4r116−r12=014(16 - r_1^2) - 7r_1^2 + 4r_1\sqrt{16 - r_1^2} = 0
224−14r12−7r12+4r116−r12=0224 - 14r_1^2 - 7r_1^2 + 4r_1\sqrt{16 - r_1^2} = 0
224−21r12=−4r116−r12224 - 21r_1^2 = -4r_1\sqrt{16 - r_1^2}

5. Square both sides to eliminate the square root and form the required equation.

Square both sides:
(224−21r12)2=(−4r116−r12)2(224 - 21r_1^2)^2 = (-4r_1\sqrt{16 - r_1^2})^2
50176−2(224)(21)r12+441r14=16r12(16−r12)50176 - 2(224)(21)r_1^2 + 441r_1^4 = 16r_1^2(16 - r_1^2)
50176−9408r12+441r14=256r12−16r1450176 - 9408r_1^2 + 441r_1^4 = 256r_1^2 - 16r_1^4

Rearranging the terms to one side:
(441+16)r14−(9408+256)r12+50176=0(441 + 16)r_1^4 - (9408 + 256)r_1^2 + 50176 = 0
457r14−9664r12+50176=0457r_1^4 - 9664r_1^2 + 50176 = 0 (shown)

Answer

457r14−9664r12+50176=0457r_1^4 - 9664r_1^2 + 50176 = 0 (shown)

5(b)

1. Solve the equation from part (a) to find the possible positive roots for $r$.

457r4−9664r2+50176=0457r^4 - 9664r^2 + 50176 = 0
Let y=r2y = r^2. Using the quadratic formula:
r2=9664±(−9664)2−4(457)(50176)2(457)r^2 = \frac{9664 \pm \sqrt{(-9664)^2 - 4(457)(50176)}}{2(457)}
r2=9664±1671168914r^2 = \frac{9664 \pm \sqrt{1671168}}{914}
r2=4832±64102457r^2 = \frac{4832 \pm 64\sqrt{102}}{457}
Evaluating these gives:
r2≈9.1589orr2≈11.9877r^2 \approx 9.1589 \quad \text{or} \quad r^2 \approx 11.9877
Taking the positive square roots (since radius r>0r > 0):
r≈3.026orr≈3.462r \approx 3.026 \quad \text{or} \quad r \approx 3.462

2. Test the first positive root in the original, un-squared condition for a stationary point to show it is extraneous.

From part (a), equating dVdr\frac{dV}{dr} to zero leads to the condition before squaring:
21r2−224=4r16−r221r^2 - 224 = 4r\sqrt{16 - r^2}
Substitute r≈3.026r \approx 3.026 (r2≈9.1589r^2 \approx 9.1589) into both sides:
LHS=21(9.1589)−224≈−31.66\text{LHS} = 21(9.1589) - 224 \approx -31.66
RHS=4(3.026)16−9.1589=12.104(2.6155)≈31.66\text{RHS} = 4(3.026)\sqrt{16 - 9.1589} = 12.104(2.6155) \approx 31.66
Since LHS ≠\neq RHS (they have opposite signs), r≈3.026r \approx 3.026 is an extraneous root introduced by squaring and does not give a stationary value of VV.

3. Find the value of $h$ corresponding to the valid root.

The valid root for the stationary point must be the other one, r2≈11.9877r^2 \approx 11.9877.
Using the relationship between slant height, radius, and height from the original cone (r2+h2=42=16r^2 + h^2 = 4^2 = 16):
h=16−r2h = \sqrt{16 - r^2}
h=16−11.9877h = \sqrt{16 - 11.9877}
h=4.0123h = \sqrt{4.0123}
h≈2.003h \approx 2.003
Thus, h=2.00h = 2.00 cm (to 3 s.f.).

Answer

h=2.00h = 2.00 (to 3 s.f.)

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