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Draining a sphere: height is not volume · source reference

[2019/NYJC/Prelim/I/7] · Question pp. 1 · Working pp. 4

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A spherical tank with negligible thickness and internal radius aa cm contains water. At time tt s, the water surface is at a height xx cm above the lowest point of the tank and the volume of water in the tank, VV cm³, is given by V=13πx2(3a−x)V=\frac13\pi x^2(3a-x). Water flows from the tank, through an outlet at its lowest point, at a rate πkx\pi k\sqrt x cm³ s⁻¹, where kk is a positive constant.

(i) Show that (2ax−x2)dxdt=−kx(2ax-x^2)\frac{dx}{dt}=-k\sqrt x. [2]

(ii) Find the general solution for tt in terms of x,a,kx,a,k. [3]

(iii) Find the ratio T1:T2T_1:T_2, where T1T_1 is the time taken to empty the tank when initially it is completely full, and T2T_2 is the time taken to empty the tank when initially it is half full. [4]

[2019/NYJC/Prelim/I/7]

Printed working

V=πx2(3a−x)/3V=\pi x^2(3a-x)/3; dV/dt=(2πax−πx2)dx/dtdV/dt=(2\pi ax-\pi x^2)dx/dt.

Since dV/dt=−πkxdV/dt=-\pi k\sqrt x, (2πax−πx2)dx/dt=−πkx⇒(2ax−x2)dx/dt=−kx(2\pi ax-\pi x^2)dx/dt=-\pi k\sqrt x\Rightarrow(2ax-x^2)dx/dt=-k\sqrt x.

∫(2ax−x2)/x dx=∫−kdt\int(2ax-x^2)/\sqrt x\,dx=\int-kdt; ∫(2ax−x3/2)dx=−kt+c\int(2a\sqrt x-x^{3/2})dx=-kt+c; 4ax3/2/3−2x5/2/5=−kt+c4ax^{3/2}/3-2x^{5/2}/5=-kt+c.

t=[c−4ax3/2/3+2x5/2/5]/kt=[c-4ax^{3/2}/3+2x^{5/2}/5]/k.

Initially full: x=2ax=2a when t=0t=0, so c=(4/3)a(2a)3/2−(2/5)(2a)5/2=(16/15)a22ac=(4/3)a(2a)^{3/2}-(2/5)(2a)^{5/2}=(16/15)a^2\sqrt{2a}. Thus T1=c/k=(16/(15k))a22aT_1=c/k=(16/(15k))a^2\sqrt{2a}.

Initially half full: x=ax=a when t=0t=0, so c=(4/3)a(a)3/2−(2/5)a5/2=(14/15)a2ac=(4/3)a(a)^{3/2}-(2/5)a^{5/2}=(14/15)a^2\sqrt a. Thus T2=(14/(15k))a2aT_2=(14/(15k))a^2\sqrt a.

T1/T2=16a22a/(14a2a)=82/7T_1/T_2=16a^2\sqrt{2a}/(14a^2\sqrt a)=8\sqrt2/7; required ratio 82:78\sqrt2:7.

Printed answer key

(ii) t=[c−4ax3/2/3+2x5/2/5]/kt=[c-4ax^{3/2}/3+2x^{5/2}/5]/k. (iii) 82:78\sqrt2:7.

Teacher note 1

Since water flows from the tank, volume decreases as time increases, so dV/dt<0dV/dt<0. Need to put in the negative sign for the rate.

Teacher note 2

Given a DE of form dx/dt=f(x)dx/dt=f(x), rearrange before integrating with respect to tt: 1f(x)dxdt=1\frac1{f(x)}\frac{dx}{dt}=1, hence ∫1f(x)dx=∫1dt\int\frac1{f(x)}dx=\int1dt.

Teacher note 3

“Initially” means when t=0t=0.

Mathematical review

(i) dV/dx=π(2ax−x2)dV/dx=\pi(2ax-x^2) and dV/dt=−πkxdV/dt=-\pi k\sqrt x. The chain rule gives the equation for 0<x<2a0<x<2a.

(ii) dt/dx=−(2ax−x3/2)/kdt/dx=-(2a\sqrt x-x^{3/2})/k. Thus t=[C−(4a/3)x3/2+(2/5)x5/2]/kt=[C-(4a/3)x^{3/2}+(2/5)x^{5/2}]/k.

(iii) Taking the initial time as zero and final height zero, T1=[(4a/3)(2a)3/2−(2/5)(2a)5/2]/k=162a5/2/(15k)T_1=[(4a/3)(2a)^{3/2}-(2/5)(2a)^{5/2}]/k=16\sqrt2a^{5/2}/(15k). Half volume occurs at x=a, so T2=14a5/2/(15k)T_2=14a^{5/2}/(15k). Therefore T1:T2=82:7T_1:T_2=8\sqrt2:7. The initial full-height derivative is singular, but the integrated emptying time is finite.

The continuation row on solution page 4 is numbered “6 (iii)” in print; its tank-emptying calculation belongs to Q5(iii).

Provenance

TJC JC2 2025 H2 Maths (9758) MSM. Native transcription checked against original visible question, working and sidebars. Question page(s): 1. Working page(s): 4. Original records remain private for QA; this native article has no PDF or raster worksheet dependency.