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Original question & working

The product substitution absorbs a linear term · source reference

[2012/RVHS/Prelim/II/1 (modified)] · Question pp. 1 · Working pp. 2

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Printed question

Use the substitution u=xyu=xy, where uu is a function of xx, to reduce the differential equation xdydx+(1−x3)y−x2=0x\frac{dy}{dx}+(1-x^3)y-x^2=0 to dudx=(u+1)x2\frac{du}{dx}=(u+1)x^2.

Hence show that the general solution to the differential equation is of the form y=Aef(x)−1xy=\frac{Ae^{f(x)}-1}{x}, where ff is a function in xx. [5]

Sketch, on separate diagrams, the particular solution curve for (i) A=2A=2 and (ii) A=−3A=-3. [2]

[2012/RVHS/Prelim/II/1 (modified)]

Printed working

Given xy′+(1−x3)y−x2=0xy'+(1-x^3)y-x^2=0 (1). Let u=xy⇒u′=xy′+yu=xy\Rightarrow u'=xy'+y.

Substitute into (1): u′−y+y−x3y−x2=0⇒u′−x2(xy)−x2=0⇒u′=ux2+x2=(u+1)x2u'-y+y-x^3y-x^2=0\Rightarrow u'-x^2(xy)-x^2=0\Rightarrow u'=ux^2+x^2=(u+1)x^2 (shown).

u′/(u+1)=x2u'/(u+1)=x^2; ∫du/(u+1)=∫x2dx\int du/(u+1)=\int x^2dx; ln⁡∣u+1∣=x3/3+C\ln|u+1|=x^3/3+C.

∣u+1∣=ex3/3+C|u+1|=e^{x^3/3+C}; u+1=Aex3/3u+1=Ae^{x^3/3}, where A=±eCA=\pm e^C; u=Aex3/3−1u=Ae^{x^3/3}-1; y=(Aex3/3−1)/xy=(Ae^{x^3/3}-1)/x, f(x)=x3/3f(x)=x^3/3.

The source sketches A=2A=2 and A=−3A=-3 on separate axes; both have vertical asymptote x=0x=0.

Printed answer key

f(x)=x3/3f(x)=x^3/3; (i) and (ii) native sketches below.

Teacher note 1

Note that u,x,yu,x,y are variables, so need to use product rule in differentiation of u=xyu=xy with respect to xx.

Teacher note 2

Given DE of form du/dx=f(x)g(u)du/dx=f(x)g(u). Rearrange by bringing all “uu” terms to the left where du/dxdu/dx is and leave “xx” terms on the right before integrating with respect to xx (“separate” the variables):

1g(u)dudx=f(x),∫1g(u)dudxdx=∫f(x)dx,∫1g(u)du=∫f(x)dx.\frac1{g(u)}\frac{du}{dx}=f(x),\qquad\int\frac1{g(u)}\frac{du}{dx}dx=\int f(x)dx,\qquad\int\frac1{g(u)}du=\int f(x)dx.

The intermediate integral can be skipped once familiar with the process.

Diagram 10-03-A2

Particular solution A = 2

Two disconnected branches, x=0 excluded.

Diagram 10-03-Aminus3

Particular solution A = -3

Two disconnected branches, x=0 excluded.

Mathematical review

u′=xy′+y=x3y+x2=(u+1)x2u'=xy'+y=x^3y+x^2=(u+1)x^2. Thus ln⁡∣u+1∣=x3/3+C\ln|u+1|=x^3/3+C and u+1=Aex3/3u+1=Ae^{x^3/3}. The family, including A=0A=0, is y=(Aex3/3−1)/xy=(Ae^{x^3/3}-1)/x for x≠0x\ne0, with f(x)=x3/3f(x)=x^3/3.

For A=2A=2, the zero is x=−3ln⁡23x=-\sqrt[3]{3\ln2}; near zero y∼1/xy\sim1/x, and as x→−∞x\to-\infty, y∼−1/x→0+y\sim-1/x\to0^+. The positive branch tends to +∞+\infty at both ends and has a minimum; the negative branch has a maximum before crossing zero and tending to −∞-\infty at 0−0^-. For A=−3A=-3, the numerator is always negative: the negative-x branch is positive and rises from 0+0^+ to +∞+\infty; the positive branch is negative and tends to −∞-\infty at both ends, with a maximum.

These turning behaviors follow y′=[Aex3/3(x3−1)+1]/x2y'=[Ae^{x^3/3}(x^3-1)+1]/x^2. The zero of the bracket on each appropriate side gives the corresponding turning point.

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): 2. Original records remain private for QA; this native article has no PDF or raster worksheet dependency.