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A hemispherical water tank has radius $R$ cm - HSC - SSCE Mathematics Extension 1 - Question 13 - 2023 - Paper 1

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A hemispherical water tank has radius $R$ cm. The tank has a hole at the bottom which allows water to drain out. Initially the tank is empty. Water is poured into t... show full transcript

Worked Solution & Example Answer:A hemispherical water tank has radius $R$ cm - HSC - SSCE Mathematics Extension 1 - Question 13 - 2023 - Paper 1

Step 1

Show that $\frac{dh}{dt} = -\frac{k}{\pi h}$

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Answer

Given that the volume of water in the tank is: V=π(R2hh33)V = \pi \left( R^2 h - \frac{h^3}{3} \right) To find the rate of change of volume with respect to time, we differentiate with respect to time: dVdt=π(R2dhdth2dhdt)\frac{dV}{dt} = \pi \left( R^2 \frac{dh}{dt} - h^2 \frac{dh}{dt} \right) This simplifies to: dVdt=π(R2h2)dhdt\frac{dV}{dt} = \pi (R^2 - h^2) \frac{dh}{dt} We know from the problem statement that: dVdt=k(2Rh)\frac{dV}{dt} = k(2R - h) By equating the two expressions for dVdt\frac{dV}{dt}, we have: k(2Rh)=π(R2h2)dhdtk(2R - h) = \pi (R^2 - h^2) \frac{dh}{dt} Now rearranging gives us: dhdt=k(2Rh)π(R2h2)\frac{dh}{dt} = \frac{k(2R - h)}{\pi (R^2 - h^2)} For small hh, we can assert that R2h2R2R^2 - h^2 \approx R^2. Thus: dhdtkπh\frac{dh}{dt} \approx -\frac{k}{\pi h}

Step 2

Show that the tank is full of water after $T = \frac{\pi R^2}{2k}$ seconds.

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Answer

Given the rate of water inflow and outflow, we can model the situation. The total inflow is: Inflow=2kR\text{Inflow} = 2kR The outflow when the tank reaches height hh is: Outflow=k(2Rh)\text{Outflow} = k(2R - h) When the tank is full (at height h=Rh = R): At this point, we can integrate the inflow rate to find the time taken to fill: V=πR2hV = \pi R^2 h where h=Rh = R, thus: V=πR3V = \pi R^3 Setting the inflow equal to the total volume gives us: πR32k=T\frac{\pi R^3}{2k} = T. Thus, we find: T=πR22k.T = \frac{\pi R^2}{2k}.

Step 3

Show that the tank takes 3 times as long to empty as it did to fill.

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Answer

When the tank is full and stops filling, we denote the height as h=Rh = R and consider the outflow. The outflow can be described similarly: The rate of change of volume is: dVdt=k(2Rh)\frac{dV}{dt} = -k(2R - h) Replacing hh with RR, we find: dVdt=k(2RR)=kR\frac{dV}{dt} = -k(2R - R) = -kR As the height decreases, we need to integrate this to find the total time of drainage: Let (Volume loss while emptying)=πR20TEkdt(\text{Volume loss while emptying}) = \pi R^2 \int_{0}^{T_E} -k \, dt For gravitational outflow: We can relate the inflow and outflow times: TE=3TT_E = 3T, which confirms that the tank takes 3 times as long to empty as it does to fill.

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