A capsule is made of a cylinder with a hemisphere at one end of the cylinder.
The cylinder has a height, h cmh\text{ cm} and radius, r cmr\text{ cm}.
The hemisphere also has radius, r cmr\text{ cm}.
(Volume of sphere = 43πr3\frac{4}{3}\pi r^3, Surface Area of sphere = 4πr24\pi r^2,
Volume of cylinder = πr2h\pi r^2 h, Curved surface area of cylinder = 2πrh2\pi r h)
Given that the volume of the capsule is 100π cm3100\pi\text{ cm}^3.

  1. (a)

    Show that h=100r2−23rh = \frac{100}{r^2} - \frac{2}{3}r.

  2. (b)

    Show that the total surface area of the capsule is A=5π3r2+200πrA = \frac{5\pi}{3}r^2 + \frac{200\pi}{r}.

  3. (c)

    Find the value of rr for the stationary value of AA.
    Explain if the value of rr gives the maximum or minimum value of AA.

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Worked solution

8(a)

1. Formulate the expression for the total volume of the capsule

Volume of capsule = Volume of cylinder + Volume of hemisphere
V=πr2h+12(43πr3)V = \pi r^2 h + \frac{1}{2} \left( \frac{4}{3}\pi r^3 \right)
V=πr2h+23πr3V = \pi r^2 h + \frac{2}{3}\pi r^3

2. Equate the volume to the given value and make $h$ the subject

Given V=100πV = 100\pi:
πr2h+23πr3=100π\pi r^2 h + \frac{2}{3}\pi r^3 = 100\pi
Divide both sides by π\pi:
r2h+23r3=100r^2 h + \frac{2}{3}r^3 = 100
r2h=100−23r3r^2 h = 100 - \frac{2}{3}r^3
h=100r2−23rh = \frac{100}{r^2} - \frac{2}{3}r (Shown)

Answer

h=100r2−23rh = \frac{100}{r^2} - \frac{2}{3}r (Shown)

8(b)

1. Formulate the expression for the total surface area of the capsule

The total surface area AA consists of the curved surface area of the hemisphere, the curved surface area of the cylinder, and the circular base of the cylinder.
A=2πr2+2πrh+πr2A = 2\pi r^2 + 2\pi rh + \pi r^2
A=3πr2+2πrhA = 3\pi r^2 + 2\pi rh

2. Substitute the expression for $h$ from part (a) into the area equation

Substitute h=100r2−23rh = \frac{100}{r^2} - \frac{2}{3}r:
A=3πr2+2πr(100r2−23r)A = 3\pi r^2 + 2\pi r\left(\frac{100}{r^2} - \frac{2}{3}r\right)

3. Expand and simplify to show the required result

A=3πr2+200πr−4π3r2A = 3\pi r^2 + \frac{200\pi}{r} - \frac{4\pi}{3}r^2
A=(3−43)πr2+200πrA = \left(3 - \frac{4}{3}\right)\pi r^2 + \frac{200\pi}{r}
A=5π3r2+200πrA = \frac{5\pi}{3}r^2 + \frac{200\pi}{r} (Shown)

Answer

A=5π3r2+200πrA = \frac{5\pi}{3}r^2 + \frac{200\pi}{r} (Shown)

8(c)

1. Differentiate $A$ with respect to $r$

A=5π3r2+200πr−1A = \frac{5\pi}{3}r^2 + 200\pi r^{-1}
dAdr=10π3r−200πr−2\frac{\mathrm{d}A}{\mathrm{d}r} = \frac{10\pi}{3}r - 200\pi r^{-2}

2. Set the derivative to zero to find the stationary value of $r$

For stationary value, dAdr=0\frac{\mathrm{d}A}{\mathrm{d}r} = 0
10π3r−200πr2=0\frac{10\pi}{3}r - \frac{200\pi}{r^2} = 0
10π3r=200πr2\frac{10\pi}{3}r = \frac{200\pi}{r^2}

3. Solve for $r$

r3=200π×310πr^3 = \frac{200\pi \times 3}{10\pi}
r3=60r^3 = 60
r=603≈3.9148≈3.91r = \sqrt[3]{60} \approx 3.9148 \approx 3.91 (to 3 s.f.)

4. Find the second derivative to determine the nature of the stationary point

d2Adr2=10π3−(−2)(200π)r−3\frac{\mathrm{d}^2A}{\mathrm{d}r^2} = \frac{10\pi}{3} - (-2)(200\pi)r^{-3}
d2Adr2=10π3+400πr3\frac{\mathrm{d}^2A}{\mathrm{d}r^2} = \frac{10\pi}{3} + \frac{400\pi}{r^3}

5. Evaluate the second derivative at the stationary point to conclude

When r=603r = \sqrt[3]{60}, r>0r > 0, so 400πr3>0\frac{400\pi}{r^3} > 0.
Thus, d2Adr2>0\frac{\mathrm{d}^2A}{\mathrm{d}r^2} > 0.
Since the second derivative is positive, the value of rr gives a minimum value of AA.

Answer

r=3.91r = 3.91 (to 3 s.f.), Minimum value

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