[The volume of a right circular cone of radius rr and height hh is 13πr2h\frac{1}{3}\pi r^2 h.] A student makes a printer nozzle for his self-built 3D printer. The printer nozzle consists of a hollow inverted right circular cone of negligible thickness with radius rr mm where 0<r<20 < r < 2, height hh mm and slanted edge 2 mm joined to a hollow cylinder of negligible thickness with radius rr mm and height rr mm. A height of 14h\frac{1}{4}h mm is cut off from the vertex of the cone for the nozzle opening (see diagram). The volume of the printer nozzle is V mm3V\text{ mm}^3.

  1. (a)

    Show that V=πr3+2164πr24−r2V = \pi r^3 + \frac{21}{64}\pi r^2 \sqrt{4-r^2}.

  2. (b)

    The student wants VV to be a maximum.

    It is given that r=r1r = r_1 gives the maximum value of VV. Show that r1r_1 satisfies the equation 4537r4−18736r2+3136=04537r^4 - 18736r^2 + 3136 = 0.

  3. (c)

    Show that one of the positive roots of the equation in part (b) does not give a stationary value of VV. Suggest a reason why this value is a solution to the equation in part (b) even though it does not give a stationary value of VV.

  4. (d)

    Given that r1r_1 is the largest positive root of the equation in part (b), state the value of r1r_1 and find the corresponding value of hh. (You need not show that your answer gives a maximum.)

  5. (e)

    With reference to the value of r1r_1 found in part (d), comment on the practicality of having a maximum volume for the printer nozzle.

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Worked solution

11(a)

1. Express the volume of the cylindrical part.

The volume of the cylinder is given by:
Vcyl=πr2(r)=πr3V_{\text{cyl}} = \pi r^2(r) = \pi r^3

2. Express the height of the cone, $h$, in terms of $r$.

Using Pythagoras' theorem on the original right circular cone:
r2+h2=22r^2 + h^2 = 2^2
h2=4−r2h^2 = 4 - r^2
h=4−r2(since h>0)h = \sqrt{4 - r^2} \quad (\text{since } h > 0)

3. Find the volume of the truncated cone.

The cut-off cone and the original cone are similar. The ratio of their heights is 14hh=14\frac{\frac{1}{4}h}{h} = \frac{1}{4}.
The ratio of their volumes is (14)3=164\left(\frac{1}{4}\right)^3 = \frac{1}{64}.
The volume of the truncated cone (frustum) is therefore (1−164)=6364\left(1 - \frac{1}{64}\right) = \frac{63}{64} of the original cone's volume.
Vfrustum=6364(13πr2h)V_{\text{frustum}} = \frac{63}{64} \left( \frac{1}{3}\pi r^2 h \right)
Vfrustum=2164πr2hV_{\text{frustum}} = \frac{21}{64}\pi r^2 h

4. Combine the volumes to obtain the final expression.

Substitute h=4−r2h = \sqrt{4-r^2} into VfrustumV_{\text{frustum}} and add to the cylinder's volume:
V=Vcyl+VfrustumV = V_{\text{cyl}} + V_{\text{frustum}}
V=πr3+2164πr24−r2V = \pi r^3 + \frac{21}{64}\pi r^2 \sqrt{4-r^2}

Answer

Shown\text{Shown}

11(b)

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

Given V=πr3+2164πr24−r2V = \pi r^3 + \frac{21}{64}\pi r^2 \sqrt{4-r^2},
dVdr=3πr2+2164π[2r4−r2+r2(124−r2)(−2r)]\frac{\mathrm{d}V}{\mathrm{d}r} = 3\pi r^2 + \frac{21}{64}\pi \left[ 2r\sqrt{4-r^2} + r^2\left(\frac{1}{2\sqrt{4-r^2}}\right)(-2r) \right]
dVdr=3πr2+2164π[2r4−r2−r34−r2]\frac{\mathrm{d}V}{\mathrm{d}r} = 3\pi r^2 + \frac{21}{64}\pi \left[ 2r\sqrt{4-r^2} - \frac{r^3}{\sqrt{4-r^2}} \right]
Make the terms in the bracket a single fraction:
dVdr=3πr2+2164π[2r(4−r2)−r34−r2]\frac{\mathrm{d}V}{\mathrm{d}r} = 3\pi r^2 + \frac{21}{64}\pi \left[ \frac{2r(4-r^2) - r^3}{\sqrt{4-r^2}} \right]
dVdr=3πr2+2164π[8r−3r34−r2]\frac{\mathrm{d}V}{\mathrm{d}r} = 3\pi r^2 + \frac{21}{64}\pi \left[ \frac{8r - 3r^3}{\sqrt{4-r^2}} \right]

2. Set the derivative to zero and simplify by factoring out $r_1$.

For a stationary point, dVdr=0\frac{\mathrm{d}V}{\mathrm{d}r} = 0. Since the maximum occurs at r=r1r = r_1:
3πr12+2164π[8r1−3r134−r12]=03\pi r_1^2 + \frac{21}{64}\pi \left[ \frac{8r_1 - 3r_1^3}{\sqrt{4-r_1^2}} \right] = 0
Since r1>0r_1 > 0, we can divide the entire equation by 3πr13\pi r_1:
r1+764[8−3r124−r12]=0r_1 + \frac{7}{64} \left[ \frac{8 - 3r_1^2}{\sqrt{4-r_1^2}} \right] = 0
Multiply through by 644−r1264\sqrt{4-r_1^2}:
64r14−r12+7(8−3r12)=064r_1\sqrt{4-r_1^2} + 7(8 - 3r_1^2) = 0

3. Rearrange and square both sides to eliminate the square root and obtain the required polynomial equation.

64r14−r12=7(3r12−8)64r_1\sqrt{4-r_1^2} = 7(3r_1^2 - 8)
Square both sides:
4096r12(4−r12)=49(3r12−8)24096r_1^2(4 - r_1^2) = 49(3r_1^2 - 8)^2
16384r12−4096r14=49(9r14−48r12+64)16384r_1^2 - 4096r_1^4 = 49(9r_1^4 - 48r_1^2 + 64)
16384r12−4096r14=441r14−2352r12+313616384r_1^2 - 4096r_1^4 = 441r_1^4 - 2352r_1^2 + 3136
Rearranging all terms to one side yields:
0=4537r14−18736r12+3136 (shown)0 = 4537r_1^4 - 18736r_1^2 + 3136 \text{ (shown)}

Answer

4537r4−18736r2+3136=04537r^4 - 18736r^2 + 3136 = 0

11(c)

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

Let x=r2x = r^2. The equation is 4537x2−18736x+3136=04537x^2 - 18736x + 3136 = 0.
Using the quadratic formula:
x=18736±(−18736)2−4(4537)(3136)2(4537)x = \frac{18736 \pm \sqrt{(-18736)^2 - 4(4537)(3136)}}{2(4537)}
x=18736±2941337609074x = \frac{18736 \pm \sqrt{294133760}}{9074}
x≈18736±17150.339074x \approx \frac{18736 \pm 17150.33}{9074}
r2≈3.9548orr2≈0.17475r^2 \approx 3.9548 \quad \text{or} \quad r^2 \approx 0.17475
Since r>0r > 0, the positive roots are:
r≈1.989orr≈0.418r \approx 1.989 \quad \text{or} \quad r \approx 0.418

2. Determine the condition for a stationary point and show that the smaller positive root fails this condition.

To find stationary points, we set dVdr=0\frac{dV}{dr} = 0:
V=πr3+2164πr24−r2V = \pi r^3 + \frac{21}{64}\pi r^2 \sqrt{4-r^2}
dVdr=3πr2+2164π(2r(4−r2)−r34−r2)=0\frac{dV}{dr} = 3\pi r^2 + \frac{21}{64}\pi \left( \frac{2r(4-r^2) - r^3}{\sqrt{4-r^2}} \right) = 0
Dividing by 3πr3\pi r (since r>0r > 0) and rearranging gives the condition before squaring:
r4−r2=764(3r2−8)r\sqrt{4-r^2} = \frac{7}{64}(3r^2 - 8)
Test the smaller positive root r≈0.418r \approx 0.418 (where r2≈0.17475r^2 \approx 0.17475):

  • Left-Hand Side (LHS): Since 0<r<20 < r < 2, r4−r2>0r\sqrt{4-r^2} > 0.
  • Right-Hand Side (RHS): 764(3(0.17475)−8)≈−0.817<0\frac{7}{64}(3(0.17475) - 8) \approx -0.817 < 0.

Since a positive LHS cannot equal a negative RHS, dVdr≠0\frac{dV}{dr} \neq 0 for r≈0.418r \approx 0.418. Therefore, this root does not give a stationary value of VV.

3. Suggest the mathematical reason for the existence of this solution.

During the derivation of the polynomial equation in part (b), the algebraic step of squaring both sides of the equation (to eliminate the square root) was required. Squaring both sides of an equation introduces extraneous roots.

Answer

The root r≈0.418r \approx 0.418 does not satisfy the original condition dVdr=0\frac{dV}{dr} = 0, thus it does not give a stationary value.

Reason: Squaring both sides of the equation during the derivation in part (b) introduced an extraneous root.

11(d)

1. Solve the given equation for the roots of $r^2$.

Let x=r2x = r^2. The given equation is 4537x2−18736x+3136=04537x^2 - 18736x + 3136 = 0.
Using the quadratic formula (or a calculator's polynomial solver):
x=18736±(−18736)2−4(4537)(3136)2(4537)x = \frac{18736 \pm \sqrt{(-18736)^2 - 4(4537)(3136)}}{2(4537)}
x=18736±2941258249074x = \frac{18736 \pm \sqrt{294125824}}{9074}
x≈3.9548orx≈0.17477x \approx 3.9548 \quad \text{or} \quad x \approx 0.17477

2. Find the largest positive root $r_1$.

Since r1r_1 is the largest positive root, we take the larger value of r2r^2:
r1=3.95482...≈1.9887r_1 = \sqrt{3.95482...} \approx 1.9887
r1=1.99 (to 3 s.f.)r_1 = 1.99 \text{ (to 3 s.f.)}

3. Calculate the corresponding value of $h$ using the geometry of the cone.

From the right circular cone's dimensions (radius rr, height hh, and slanted edge 22), we use Pythagoras' theorem:
r2+h2=22r^2 + h^2 = 2^2
h2=4−r2h^2 = 4 - r^2
Substituting the exact value of r12r_1^2:
h2=4−3.95482...=0.04517...h^2 = 4 - 3.95482... = 0.04517...
h=0.04517...≈0.21254h = \sqrt{0.04517...} \approx 0.21254
h=0.213 (to 3 s.f.)h = 0.213 \text{ (to 3 s.f.)}

Answer

r1=1.99r_1 = 1.99, h=0.213h = 0.213

11(e)

1. Comment on the shape of the nozzle using the dimensions from part (d).

From part (d), r1≈1.99 mmr_1 \approx 1.99\text{ mm} and h≈0.213 mmh \approx 0.213\text{ mm}. Since the height hh is significantly smaller than the radius r1r_1, the conical part of the nozzle is extremely shallow (almost a flat disc). This geometric shape is impractical for effectively directing and extruding material in a 3D printer, meaning the mathematical maximum volume does not yield a practical design.

Answer

From part (d), r1≈1.99r_1 \approx 1.99 and h≈0.213h \approx 0.213. Since the height hh is much smaller than the radius r1r_1, the conical part of the nozzle is almost flat (or too shallow), making it impractical for use as a 3D printer nozzle.

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