A closed container is made up of a cylinder of base radius rr cm and height hh cm, and a hemispherical top with the same radius rr. It is inscribed within a fixed right circular cone of base radius 5 cm and height 12 cm, as shown in the diagram below.

  1. (i)

    By using similar triangles, show that h=12−135rh = 12 - \frac{13}{5}r.

    Determine the exact range of possible values of length rr.

  2. (ii)

    Find the total volume VV of the closed container in terms of rr.
    By differentiation, find the exact value of rr that produces the maximum container volume VV, as rr varies.

    [Volume of a sphere with radius RR is 43πR3\frac{4}{3}\pi R^3.]

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Worked solution

4(i)

1. Determine the slant height of the cone from its cross-section.

Let VV be the vertex of the cone, OO be the centre of its base, and BB be a point on the perimeter of the base.
Consider the vertical cross-section △VOB\triangle VOB, which is right-angled at OO.
The vertical height VO=12VO = 12 and base radius OB=5OB = 5.
By Pythagoras' theorem, the slant edge is:
VB=122+52=144+25=169=13 cmVB = \sqrt{12^2 + 5^2} = \sqrt{144 + 25} = \sqrt{169} = 13 \text{ cm}

2. Set up a similarity relationship between the cone and the inscribed container.

Let CC be the centre of the hemispherical top. It lies on VOVO such that OC=hOC = h, giving VC=12−hVC = 12 - h.
The hemisphere is tangent to the slant edge VBVB at a point TT. Thus, the radius to the point of tangency is perpendicular to the slant edge (CT⊥VBCT \perp VB) and CT=rCT = r.
In △VTC\triangle VTC and △VOB\triangle VOB:

  • ∠TVC=∠OVB\angle TVC = \angle OVB (common angle)
  • ∠VTC=∠VOB=90∘\angle VTC = \angle VOB = 90^\circ
    Therefore, △VTC\triangle VTC is similar to △VOB\triangle VOB.
    Using the ratio of corresponding sides:
    CTOB=VCVB\frac{CT}{OB} = \frac{VC}{VB}
    r5=12−h13\frac{r}{5} = \frac{12 - h}{13}

3. Rearrange to show the required expression for $h$ and determine the exact range of $r$.

13r=5(12−h)13r = 5(12 - h)
13r=60−5h13r = 60 - 5h
5h=60−13r5h = 60 - 13r
h=12−135r(shown)h = 12 - \frac{13}{5}r \quad \text{(shown)}
For the container to be physically composed of a cylinder and a hemisphere, its dimensions must be strictly positive.
Since h>0h > 0:
12−135r>012 - \frac{13}{5}r > 0
135r<12  ⟹  r<6013\frac{13}{5}r < 12 \implies r < \frac{60}{13}
Since rr is a length, r>0r > 0. Therefore, the exact range of possible values for rr is:
0<r<60130 < r < \frac{60}{13}

Answer

h=12−135rh = 12 - \frac{13}{5}r

0<r<60130 < r < \frac{60}{13}

4(ii)

1. Express the total volume $V$ of the closed container in terms of $r$.

The container consists of a cylinder and a hemisphere.
V=Vcylinder+VhemisphereV = V_{\text{cylinder}} + V_{\text{hemisphere}}
V=πr2h+23πr3V = \pi r^2 h + \frac{2}{3}\pi r^3
Substitute h=12−135rh = 12 - \frac{13}{5}r from part (i):
V=πr2(12−135r)+23πr3V = \pi r^2 \left(12 - \frac{13}{5}r\right) + \frac{2}{3}\pi r^3
V=12πr2−135πr3+23πr3V = 12\pi r^2 - \frac{13}{5}\pi r^3 + \frac{2}{3}\pi r^3
V=12πr2+(−3915+1015)πr3V = 12\pi r^2 + \left(-\frac{39}{15} + \frac{10}{15}\right)\pi r^3
V=12πr2−2915πr3V = 12\pi r^2 - \frac{29}{15}\pi r^3

2. Differentiate $V$ with respect to $r$.

dVdr=24πr−3(2915π)r2\frac{dV}{dr} = 24\pi r - 3\left(\frac{29}{15}\pi\right)r^2
dVdr=24πr−295πr2\frac{dV}{dr} = 24\pi r - \frac{29}{5}\pi r^2

3. Set the derivative to zero and solve for the optimal value of $r$.

To find the stationary point, set dVdr=0\frac{dV}{dr} = 0:
24πr−295πr2=024\pi r - \frac{29}{5}\pi r^2 = 0
πr(24−295r)=0\pi r \left( 24 - \frac{29}{5}r \right) = 0
Since r>0r > 0 for a valid physical container, we reject r=0r = 0:
24−295r=024 - \frac{29}{5}r = 0
295r=24  ⟹  r=12029\frac{29}{5}r = 24 \implies r = \frac{120}{29}

4. Verify that this value of $r$ produces a maximum volume using the second derivative test.

d2Vdr2=24π−2(295π)r\frac{d^2V}{dr^2} = 24\pi - 2\left(\frac{29}{5}\pi\right)r
d2Vdr2=24π−585πr\frac{d^2V}{dr^2} = 24\pi - \frac{58}{5}\pi r
Substitute r=12029r = \frac{120}{29}:
d2Vdr2=24π−585π(12029)\frac{d^2V}{dr^2} = 24\pi - \frac{58}{5}\pi \left(\frac{120}{29}\right)
d2Vdr2=24π−2(24)π=−24π\frac{d^2V}{dr^2} = 24\pi - 2(24)\pi = -24\pi
Since d2Vdr2<0\frac{d^2V}{dr^2} < 0, the volume is indeed maximized at r=12029r = \frac{120}{29}.

Answer

V=12πr2−2915πr3V = 12\pi r^2 - \frac{29}{15}\pi r^3

r=12029r = \frac{120}{29}

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