[A sphere of radius rr has surface area 4πr24\pi r^2 and volume 43πr3\dfrac{4}{3}\pi r^3.] A water fountain is to be constructed in the middle of Bishan East Park. It consists of a hemisphere with radius rr joined to an open cylinder with radius rr and height hh (see diagram). The thickness of the fountain is negligible. It is given that the fountain, when filled to the brim, can hold a fixed volume kk m^3 of water.

  1. (a)

    The interior of the fountain is to be painted with a layer of special reflecting paint. The cost of painting is $3\char36{}3 per m2^2 for the hemispherical surface and $2.50\char36{}2.50 per m2^2 for the cylindrical wall. Show that the total cost of painting, CC, is given by ${83πr2+5kr}\char36{}\left\{\dfrac{8}{3}\pi r^2 + \dfrac{5k}{r}\right\}.

  2. (b)

    Using differentiation, find the value of rr, in terms of kk, such that CC is a minimum.

  3. (c)

    Keeping CC at a minimum, it is now given that k=50k = 50.

    Find the numerical values of rr and hh.

  4. (d)

    When the fountain is filled to the brim, a leak develops at the joint between the cylinder and the hemisphere. Water leaks at a constant rate of 0.0020.002 m3^3 per minute. Assuming that water is neither lost nor added to the fountain in any other way, find the rate at which the level of water is decreasing.

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Worked solution

11(a)

1. Express the total volume $k$ in terms of $r$ and $h$, and make $h$ the subject.

The total volume kk is the sum of the volume of the hemisphere and the volume of the cylinder:
k=23πr3+πr2hk = \frac{2}{3}\pi r^3 + \pi r^2 h
πr2h=k−23πr3\pi r^2 h = k - \frac{2}{3}\pi r^3
h=kπr2−2r3h = \frac{k}{\pi r^2} - \frac{2r}{3}

2. Formulate the total cost $C$ in terms of $r$ and $h$.

Area of the inner hemispherical surface =2πr2= 2\pi r^2
Area of the inner cylindrical wall =2πrh= 2\pi rh

Cost of painting hemispherical surface =3×2πr2=6πr2= 3 \times 2\pi r^2 = 6\pi r^2
Cost of painting cylindrical wall =2.50×2πrh=5πrh= 2.50 \times 2\pi rh = 5\pi rh

C=6πr2+5πrhC = 6\pi r^2 + 5\pi rh

3. Substitute $h$ into the cost equation and simplify to obtain the final expression.

C=6πr2+5πr(kπr2−2r3)C = 6\pi r^2 + 5\pi r \left( \frac{k}{\pi r^2} - \frac{2r}{3} \right)
C=6πr2+5kr−103πr2C = 6\pi r^2 + \frac{5k}{r} - \frac{10}{3}\pi r^2
C=(6−103)πr2+5krC = \left(6 - \frac{10}{3}\right)\pi r^2 + \frac{5k}{r}
C=83πr2+5kr (Shown)C = \frac{8}{3}\pi r^2 + \frac{5k}{r} \text{ (Shown)}

Answer

C=83πr2+5kr (Shown)C = \frac{8}{3}\pi r^2 + \frac{5k}{r} \text{ (Shown)}

11(b)

1. Find the first derivative of $C$ with respect to $r$.

dCdr=163πr−5kr2\frac{\mathrm{d}C}{\mathrm{d}r} = \frac{16}{3}\pi r - \frac{5k}{r^2}

2. Set the first derivative to zero to find the stationary point.

163πr−5kr2=0\frac{16}{3}\pi r - \frac{5k}{r^2} = 0

3. Solve for $r$ in terms of $k$.

163πr=5kr2\frac{16}{3}\pi r = \frac{5k}{r^2}\n16πr3=15k16\pi r^3 = 15k\nr3=15k16πr^3 = \frac{15k}{16\pi}\nr=15k16π3r = \sqrt[3]{\frac{15k}{16\pi}}

4. Verify that this value of $r$ yields a minimum cost using the second derivative test.

d2Cdr2=163π+10kr3\frac{\mathrm{d}^2C}{\mathrm{d}r^2} = \frac{16}{3}\pi + \frac{10k}{r^3}\nSince k>0k > 0 and r>0r > 0 for physical dimensions, d2Cdr2>0\frac{\mathrm{d}^2C}{\mathrm{d}r^2} > 0.\nThus, the cost CC is a minimum at r=15k16π3r = \sqrt[3]{\frac{15k}{16\pi}}.

Answer

r=15k16π3r = \sqrt[3]{\frac{15k}{16\pi}}

11(c)

1. Substitute $k = 50$ into the expression for $r$ obtained in part (b) to find its numerical value.

From part (b), we established that for a minimum cost CC, dCdr=163πr−5kr2=0\frac{\mathrm{d}C}{\mathrm{d}r} = \frac{16}{3}\pi r - \frac{5k}{r^2} = 0, which gives r=15k16π3r = \sqrt[3]{\frac{15k}{16\pi}}.
Substituting k=50k = 50:
r=15(50)16π3=3758π3r = \sqrt[3]{\frac{15(50)}{16\pi}} = \sqrt[3]{\frac{375}{8\pi}}
r≈2.4618 mr \approx 2.4618 \text{ m}

2. Use the volume formula to find the corresponding value of $h$.

The total volume kk is the sum of the volumes of the cylinder and the hemisphere:
k=πr2h+23πr3k = \pi r^2 h + \frac{2}{3}\pi r^3
Substituting k=50k = 50 and the exact value of r3=3758πr^3 = \frac{375}{8\pi}:
50=πr2h+23π(3758π)50 = \pi r^2 h + \frac{2}{3}\pi \left(\frac{375}{8\pi}\right)
50=πr2h+31.2550 = \pi r^2 h + 31.25
πr2h=18.75\pi r^2 h = 18.75
h=18.75π(2.4618)2h = \frac{18.75}{\pi (2.4618)^2}
h≈0.98476 mh \approx 0.98476 \text{ m}
Rounding to 3 significant figures, we get:
r=2.46r = 2.46, h=0.985h = 0.985

Answer

r=2.46r = 2.46, h=0.985h = 0.985

11(d)

1. Determine the cross-sectional area of the free surface using the value of $r$ from part (c).

From part (c), the radius is r=15(50)16π3≈2.4618 mr = \sqrt[3]{\frac{15(50)}{16\pi}} \approx 2.4618 \text{ m}.
Since the fountain is filled to the brim, the water level is initially within the cylindrical section.
The volume of water VV when the water level is at height yy above the joint in the cylinder is given by V=23πr3+πr2yV = \frac{2}{3}\pi r^3 + \pi r^2 y.
Differentiating with respect to yy, the cross-sectional area is:
dVdy=πr2=π(2.4618)2≈19.040 m2\frac{\mathrm{d}V}{\mathrm{d}y} = \pi r^2 = \pi (2.4618)^2 \approx 19.040 \text{ m}^2

2. Apply the chain rule to find the rate of decrease of the water level.

We are given the rate of water leaking, which represents the rate of change of volume with respect to time:
dVdt=−0.002 m3/min\frac{\mathrm{d}V}{\mathrm{d}t} = -0.002 \text{ m}^3/\text{min}
Using the chain rule, dVdt=dVdy×dydt\frac{\mathrm{d}V}{\mathrm{d}t} = \frac{\mathrm{d}V}{\mathrm{d}y} \times \frac{\mathrm{d}y}{\mathrm{d}t}:
−0.002=19.040×dydt-0.002 = 19.040 \times \frac{\mathrm{d}y}{\mathrm{d}t}
dydt=−0.00219.040≈−0.00010504 m/min\frac{\mathrm{d}y}{\mathrm{d}t} = \frac{-0.002}{19.040} \approx -0.00010504 \text{ m/min}
Thus, the rate at which the level of water is decreasing is 0.000105 m/min0.000105 \text{ m/min} (or 1.05×10−4 m/min1.05 \times 10^{-4} \text{ m/min}).

Answer

1.05×10−4 m/min1.05 \times 10^{-4} \text{ m/min}

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