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Chapter 9 · Differential Equations

Miscellaneous · Q2: Verify four solutions, from xy=aex+be−x+x2xy = ae^x + be^{-x} + x^2 to x2=2y2log⁡yx^2 = 2y^2\log y

Miscellaneous ExerciseVerifying a solution · Section 9.3
The question

2. For each of the exercises given below, verify that the given function (implicit or explicit) is a solution of the corresponding differential equation.

(i) xy=a ex+b e−x+x2xy = a\,e^x + b\,e^{-x} + x^2 : xd2ydx2+2dydx−xy+x2−2=0x\dfrac{d^2y}{dx^2} + 2\dfrac{dy}{dx} - xy + x^2 - 2 = 0

(ii) y=ex(acos⁡x+bsin⁡x)y = e^x(a\cos x + b\sin x) : d2ydx2−2dydx+2y=0\dfrac{d^2y}{dx^2} - 2\dfrac{dy}{dx} + 2y = 0

(iii) y=xsin⁡3xy = x\sin 3x : d2ydx2+9y−6cos⁡3x=0\dfrac{d^2y}{dx^2} + 9y - 6\cos 3x = 0

(iv) x2=2y2log⁡yx^2 = 2y^2\log y : (x2+y2)dydx−xy=0(x^2 + y^2)\dfrac{dy}{dx} - xy = 0

Exam answer

(i) Given

xy=aex+be−x+x2…(1)xy = ae^x + be^{-x} + x^2\quad\ldots(1)

Differentiating (1) with respect to xx⁠,

xdydx+y=aex−be−x+2xx\frac{dy}{dx} + y = ae^x - be^{-x} + 2x

Differentiating again with respect to xx⁠,

xd2ydx2+dydx+dydx=aex+be−x+2=xy−x2+2[by (1)]\begin{aligned} &x\frac{d^2y}{dx^2} + \frac{dy}{dx} + \frac{dy}{dx} \\ &= ae^x + be^{-x} + 2 \\ &= xy - x^2 + 2\quad[\text{by } (1)] \end{aligned} ∴ xd2ydx2+2dydx−xy+x2−2=0\therefore\ x\frac{d^2y}{dx^2} + 2\frac{dy}{dx} - xy + x^2 - 2 = 0

Hence the given function is a solution.

(ii) Given

y=ex(acos⁡x+bsin⁡x)…(2)y = e^x(a\cos x + b\sin x)\quad\ldots(2)

Differentiating with respect to xx (product rule),

dydx=ex(acos⁡x+bsin⁡x)+ex(−asin⁡x+bcos⁡x)=y+ex(bcos⁡x−asin⁡x)…(3)\begin{aligned} \frac{dy}{dx} &= e^x(a\cos x + b\sin x) \\ &\quad + e^x(-a\sin x + b\cos x) \\ &= y + e^x(b\cos x - a\sin x) \\ &\quad\ldots(3) \end{aligned}

Differentiating (3) with respect to xx⁠,

d2ydx2=dydx+ex(bcos⁡x−asin⁡x)+ex(−bsin⁡x−acos⁡x)=dydx+(dydx−y)−y=2dydx−2y\begin{aligned} \frac{d^2y}{dx^2} &= \frac{dy}{dx} + e^x(b\cos x - a\sin x) \\ &\quad + e^x(-b\sin x - a\cos x) \\ &= \frac{dy}{dx} + \left(\frac{dy}{dx} - y\right) - y \\ &= 2\frac{dy}{dx} - 2y \end{aligned}

using (3) for the second term and (2) for the third.

∴ d2ydx2−2dydx+2y=0\therefore\ \frac{d^2y}{dx^2} - 2\frac{dy}{dx} + 2y = 0

Hence the given function is a solution.

(iii) Given y=xsin⁡3xy = x\sin 3x⁠. Differentiating with respect to xx⁠,

dydx=sin⁡3x+3xcos⁡3xd2ydx2=3cos⁡3x+3cos⁡3x−9xsin⁡3x=6cos⁡3x−9xsin⁡3x\begin{aligned} \frac{dy}{dx} &= \sin 3x + 3x\cos 3x \\ \frac{d^2y}{dx^2} &= 3\cos 3x + 3\cos 3x \\ &\quad - 9x\sin 3x \\ &= 6\cos 3x - 9x\sin 3x \end{aligned}

Substituting in the L.H.S. of the given equation,

L.H.S.=6cos⁡3x−9xsin⁡3x+9xsin⁡3x−6cos⁡3x=0=R.H.S.\begin{aligned} \text{L.H.S.} &= 6\cos 3x - 9x\sin 3x \\ &\quad + 9x\sin 3x - 6\cos 3x \\ &= 0 = \text{R.H.S.} \end{aligned}

Hence the given function is a solution.

(iv) Given x2=2y2log⁡yx^2 = 2y^2\log y⁠, with y>0y > 0⁠. Since x2≥0x^2 \ge 0⁠, log⁡y≥0\log y \ge 0⁠, so 1+2log⁡y>01 + 2\log y > 0⁠.

Differentiating with respect to xx⁠,

2x=2(2ylog⁡y+y2⋅1y)dydx2x=2y(1+2log⁡y)dydxdydx=xy(1+2log⁡y)\begin{aligned} 2x &= 2\left(2y\log y + y^2\cdot\frac{1}{y}\right)\frac{dy}{dx} \\ 2x &= 2y(1 + 2\log y)\frac{dy}{dx} \\ \frac{dy}{dx} &= \frac{x}{y(1 + 2\log y)} \end{aligned}

Also x2+y2=2y2log⁡y+y2x^2 + y^2 = 2y^2\log y + y^2 =y2(1+2log⁡y)= y^2(1 + 2\log y)⁠. So

L.H.S.=y2(1+2log⁡y)⋅xy(1+2log⁡y)−xy=xy−xy=0=R.H.S.\begin{aligned} \text{L.H.S.} &= y^2(1 + 2\log y) \\ &\quad\cdot\frac{x}{y(1 + 2\log y)} - xy \\ &= xy - xy = 0 = \text{R.H.S.} \end{aligned}

∴\therefore In each case, the given function is a solution of the corresponding differential equation.

Want the reason behind every step, the basics and the checks?

The one idea this problem is built on

To verify a solution, differentiate the given function as often as the equation needs, put the derivatives into the equation, and show that the two sides agree for every xx (and every value of the constants). When the function is given implicitly, as in (i) and (iv), differentiate the relation as it stands, treating yy as a function of xx⁠, and use the relation itself again to remove what does not belong (the constants a,ba, b in (i), log⁡y\log y in (iv)).

Given, to find, and the plan
Given
Four functions with four differential equations: (i) xy=aex+be−x+x2xy = ae^x + be^{-x} + x^2⁠, defined for x≠0x \ne 0⁠; (ii) y=ex(acos⁡x+bsin⁡x)y = e^x(a\cos x + b\sin x) and (iii) y=xsin⁡3xy = x\sin 3x⁠, defined for every real xx⁠; (iv) x2=2y2log⁡yx^2 = 2y^2\log y⁠, which needs y>0y > 0⁠. The letters aa⁠, bb are arbitrary constants.
To show
That each function satisfies its equation.
Plan
For each part: (1) differentiate once; (2) differentiate again if the equation is of second order; (3) substitute and simplify to L.H.S. = R.H.S., using the given relation where it removes aa⁠, bb or log⁡y\log y⁠.

Basics you need

1What a solution is

A function is a solution when substituting it and its derivatives into the equation makes L.H.S. = R.H.S. (Section 9.3). Lesson: general and particular solutions

2Product rule and implicit differentiation

(uv)′=u′v+uv′(uv)' = u'v + uv'⁠. In a relation such as xy=…xy = \ldots⁠, differentiate each side with respect to xx⁠, writing ddx(xy)=xdydx+y\frac{d}{dx}(xy) = x\frac{dy}{dx} + y and ddx(y2)=2ydydx\frac{d}{dx}(y^2) = 2y\frac{dy}{dx} (Chapter 5). Basics: y′ and y″

3Derivatives of exe^x⁠, e−xe^{-x}⁠, sine, cosine and log

(ex)′=ex(e^x)' = e^x⁠, (e−x)′=−e−x(e^{-x})' = -e^{-x}⁠, (sin⁡3x)′=3cos⁡3x(\sin 3x)' = 3\cos 3x⁠, (cos⁡3x)′=−3sin⁡3x(\cos 3x)' = -3\sin 3x⁠, (log⁡y)′=1y y′(\log y)' = \frac{1}{y}\,y' (Chapter 5). Basics: e^{kt} and its rate

4Arbitrary constants and the order

A second order equation has two arbitrary constants in its general solution; the functions in (i) and (ii) carry exactly two, aa and bb (chapter Summary). Basics: order n gives n constants

Part (i): xy=aex+be−x+x2xy = ae^x + be^{-x} + x^2

  1. Differentiate the relation once

    Differentiate both sides of xy=aex+be−x+x2…(1)xy = ae^x + be^{-x} + x^2\quad\ldots(1) with respect to xx⁠. On the left, the product rule gives xdydx+yx\frac{dy}{dx} + y⁠:

    xdydx+y=aex−be−x+2x.…(2)x\frac{dy}{dx} + y = ae^x - be^{-x} + 2x.\quad\ldots(2)
    The function is given implicitly (yy times xx⁠), so we differentiate the relation as it stands rather than first dividing by xx⁠. Both ways work for x≠0x \ne 0⁠; this one is shorter.
    Product rule; (e−x)′=−e−x(e^{-x})' = -e^{-x} (Chapter 5). Basics: y′ and y″
  2. Differentiate again

    Differentiate (2): xdydxx\frac{dy}{dx} gives dydx+xd2ydx2\frac{dy}{dx} + x\frac{d^2y}{dx^2} by the product rule, and yy gives dydx\frac{dy}{dx}⁠:

    xd2ydx2+2dydx=aex+be−x+2.x\frac{d^2y}{dx^2} + 2\frac{dy}{dx} = ae^x + be^{-x} + 2.
    The equation to be verified is of second order, so we need d2ydx2\frac{d^2y}{dx^2}⁠. Notice that the sign of be−xbe^{-x} has turned back to ++⁠: differentiating e−xe^{-x} twice gives e−xe^{-x}⁠.
    Second order derivative (Chapter 5, Section 5.7). Basics: y′ and y″
  3. Remove aa and bb with (1), and conclude

    From (1), aex+be−x=xy−x2ae^x + be^{-x} = xy - x^2⁠. So

    xd2ydx2+2dydx=xy−x2+2,xd2ydx2+2dydx−xy+x2−2=0.\begin{aligned} &x\frac{d^2y}{dx^2} + 2\frac{dy}{dx} = xy - x^2 + 2, \\ &x\frac{d^2y}{dx^2} + 2\frac{dy}{dx} - xy \\ &\quad + x^2 - 2 = 0. \end{aligned}

    This is the given equation, for every x≠0x \ne 0 and all a,ba, b⁠. So the function is a solution.

    The constants aa and bb appear in the same combination aex+be−xae^x + be^{-x} as in (1), so (1) replaces them by xy−x2xy - x^2 at one stroke. What is left contains only xx⁠, yy and the derivatives, which is what a differential equation may contain.
    Section 9.3: substitute and compare the two sides. Lesson: is it a solution?

Part (ii): y=ex(acos⁡x+bsin⁡x)y = e^x(a\cos x + b\sin x)

  1. First derivative, written through yy

    By the product rule,

    dydx=ex(acos⁡x+bsin⁡x)+ex(−asin⁡x+bcos⁡x)=y+ex(bcos⁡x−asin⁡x).\begin{aligned} \frac{dy}{dx} &= e^x(a\cos x + b\sin x) \\ &\quad + e^x(-a\sin x + b\cos x) \\ &= y + e^x(b\cos x - a\sin x). \end{aligned}

    Call this (3).

    The first product, exe^x times the bracket, is yy itself, because (ex)′=ex(e^x)' = e^x⁠. Keeping it as yy makes the next step shorter.
    Product rule; (cos⁡x)′=−sin⁡x(\cos x)' = -\sin x⁠, (sin⁡x)′=cos⁡x(\sin x)' = \cos x⁠. Basics: e^{kt} and its rate
  2. Second derivative

    Differentiate (3). The derivative of yy is dydx\frac{dy}{dx}⁠; the product ex(bcos⁡x−asin⁡x)e^x(b\cos x - a\sin x) gives two terms:

    d2ydx2=dydx+ex(bcos⁡x−asin⁡x)+ex(−bsin⁡x−acos⁡x).\begin{aligned} \frac{d^2y}{dx^2} &= \frac{dy}{dx} + e^x(b\cos x - a\sin x) \\ &\quad + e^x(-b\sin x - a\cos x). \end{aligned}

    By (3), ex(bcos⁡x−asin⁡x)=dydx−ye^x(b\cos x - a\sin x) = \frac{dy}{dx} - y⁠. And the last term is −ex(acos⁡x+bsin⁡x)-e^x(a\cos x + b\sin x)⁠, which is −y-y⁠. So

    d2ydx2=dydx+(dydx−y)−y=2dydx−2y.\begin{aligned} \frac{d^2y}{dx^2} &= \frac{dy}{dx} + \left(\frac{dy}{dx} - y\right) - y \\ &= 2\frac{dy}{dx} - 2y. \end{aligned}
    Every piece is now written through yy and dydx\frac{dy}{dx}⁠, so aa and bb have disappeared.
    Differentiate (3) term by term (Chapter 5). Basics: y′ and y″
  3. Substitute and conclude

    d2ydx2−2dydx+2y=(2dydx−2y)−2dydx+2y=0.\begin{aligned} &\frac{d^2y}{dx^2} - 2\frac{dy}{dx} + 2y \\ &= \left(2\frac{dy}{dx} - 2y\right) - 2\frac{dy}{dx} + 2y = 0. \end{aligned}

    So L.H.S. = 0 = R.H.S. for every real xx and all a,ba, b⁠: the function is a solution, with two arbitrary constants for a second order equation.

    This is a special case of Example 19, where eax(c1cos⁡bx+c2sin⁡bx)e^{ax}(c_1\cos bx + c_2\sin bx) solves y′′−2ay′+(a2+b2)y=0y'' - 2ay' + (a^2 + b^2)y = 0⁠. Taking the exponent and the frequency there both equal to 1 gives our function and our equation y′′−2y′+2y=0y'' - 2y' + 2y = 0⁠.
    Section 9.3: L.H.S. = R.H.S. Lesson: Examples 19 to 22

Part (iii): y=xsin⁡3xy = x\sin 3x

  1. First derivative

    dydx=sin⁡3x+x⋅3cos⁡3x=sin⁡3x+3xcos⁡3x.\begin{aligned} \frac{dy}{dx} &= \sin 3x + x\cdot 3\cos 3x \\ &= \sin 3x + 3x\cos 3x. \end{aligned}
    yy is a product of xx and sin⁡3x\sin 3x⁠; the chain rule gives (sin⁡3x)′=3cos⁡3x(\sin 3x)' = 3\cos 3x⁠.
    Product rule and chain rule (Chapter 5). Basics: y′ and y″
  2. Second derivative

    d2ydx2=3cos⁡3x+(3cos⁡3x−9xsin⁡3x)=6cos⁡3x−9xsin⁡3x.\begin{aligned} \frac{d^2y}{dx^2} &= 3\cos 3x + \left(3\cos 3x - 9x\sin 3x\right) \\ &= 6\cos 3x - 9x\sin 3x. \end{aligned}
    The first term, sin⁡3x\sin 3x⁠, gives 3cos⁡3x3\cos 3x⁠. The second, 3xcos⁡3x3x\cos 3x⁠, is again a product: 3cos⁡3x+3x(−3sin⁡3x)3\cos 3x + 3x(-3\sin 3x)⁠.
    (cos⁡3x)′=−3sin⁡3x(\cos 3x)' = -3\sin 3x (Chapter 5). Basics: y′ and y″
  3. Substitute and conclude

    d2ydx2+9y−6cos⁡3x=6cos⁡3x−9xsin⁡3x+9xsin⁡3x−6cos⁡3x=0.\begin{aligned} &\frac{d^2y}{dx^2} + 9y - 6\cos 3x \\ &= 6\cos 3x - 9x\sin 3x \\ &\quad + 9x\sin 3x - 6\cos 3x \\ &= 0. \end{aligned}

    So L.H.S. = 0 = R.H.S. for every real xx⁠: the function is a solution. It has no arbitrary constant, so it is a particular solution of this second order equation.

    The 9xsin⁡3x9x\sin 3x terms cancel, and so do the 6cos⁡3x6\cos 3x terms. The first derivative was only a stage on the way: dydx\frac{dy}{dx} does not appear in the equation.
    Section 9.3: a solution with no arbitrary constant is a particular solution. Basics: order n gives n constants

Part (iv): x2=2y2log⁡yx^2 = 2y^2\log y

  1. Where the relation lives

    log⁡y\log y needs y>0y > 0⁠. The left side x2x^2 is never negative, so 2y2log⁡y≥02y^2\log y \ge 0⁠, that is log⁡y≥0\log y \ge 0⁠, that is y≥1y \ge 1⁠. Hence

    1+2log⁡y≥1>0.1 + 2\log y \ge 1 > 0.
    We will divide by 1+2log⁡y1 + 2\log y in the next step, so we first make sure it is never 0. On this curve it cannot be: 1+2log⁡y=01 + 2\log y = 0 would need y=e−1/2<1y = e^{-1/2} < 1⁠.
    log⁡y\log y is defined for y>0y > 0 and is ≥0\ge 0 exactly when y≥1y \ge 1 (Chapter 5, Section 5.4). Basics: e^{kt} and log
  2. Differentiate implicitly and find dydx\frac{dy}{dx}

    Differentiate both sides with respect to xx⁠, using the product rule on y2⋅log⁡yy^2\cdot\log y⁠:

    2x=2(2ylog⁡y+y2⋅1y)dydx=2y(1+2log⁡y)dydx,dydx=xy(1+2log⁡y).\begin{aligned} 2x &= 2\left(2y\log y + y^2\cdot\frac{1}{y}\right)\frac{dy}{dx} \\ &= 2y(1 + 2\log y)\frac{dy}{dx}, \\ \frac{dy}{dx} &= \frac{x}{y(1 + 2\log y)}. \end{aligned}
    Each factor that contains yy carries a dydx\frac{dy}{dx} by the chain rule. The divisor y(1+2log⁡y)y(1 + 2\log y) is positive by Part (iv), Step 1, so the division is allowed.
    Implicit differentiation; (log⁡y)′=1ydydx(\log y)' = \frac{1}{y}\frac{dy}{dx} (Chapter 5). Basics: y′ and y″
  3. Use the relation to rewrite x2+y2x^2 + y^2⁠, substitute and conclude

    By the given relation, x2+y2=2y2log⁡y+y2=y2(1+2log⁡y)x^2 + y^2 = 2y^2\log y + y^2 = y^2(1 + 2\log y)⁠. So

    (x2+y2)dydx−xy=y2(1+2log⁡y)⋅xy(1+2log⁡y)−xy=xy−xy=0.\begin{aligned} &(x^2 + y^2)\frac{dy}{dx} - xy \\ &= y^2(1 + 2\log y)\cdot\frac{x}{y(1 + 2\log y)} - xy \\ &= xy - xy = 0. \end{aligned}

    So L.H.S. = 0 = R.H.S. at every point of the curve: the relation is a solution of the equation.

    The factor 1+2log⁡y1 + 2\log y appears in both places and cancels, and y2y=y\frac{y^2}{y} = y⁠. The relation was used twice: once to differentiate, once to replace x2x^2⁠.
    Section 9.3: an implicit relation is a solution when it makes L.H.S. = R.H.S. Lesson: Miscellaneous exercise player
Result

(i) xd2ydx2+2dydx−xy+x2−2=0x\frac{d^2y}{dx^2} + 2\frac{dy}{dx} - xy + x^2 - 2 = 0 holds (for x≠0x \ne 0 and all a,ba, b⁠). (ii) d2ydx2=2dydx−2y\frac{d^2y}{dx^2} = 2\frac{dy}{dx} - 2y⁠, so the equation holds for all a,ba, b⁠. (iii) L.H.S. =0= 0⁠. (iv) (x2+y2)dydx=xy(x^2 + y^2)\frac{dy}{dx} = xy on the curve, where y≥1y \ge 1⁠. In each case the given function is a solution of its equation.

(Textbook answer: the answer key prints nothing for this question; each part is a verification.)

Check it with numbers

(i) Take a=1a = 1⁠, b=2b = 2⁠, x=1x = 1⁠, so y=e+2e−1+1y = e + 2e^{-1} + 1⁠. Then xd2ydx2≈6.3970762x\frac{d^2y}{dx^2} \approx 6.3970762⁠, 2dydx≈−0.94303552\frac{dy}{dx} \approx -0.9430355 and xy≈4.4540407xy \approx 4.4540407⁠, and

6.3970762−0.9430355−4.4540407+1−2=0.0000000.\begin{aligned} &6.3970762 - 0.9430355 \\ &\quad - 4.4540407 + 1 - 2 \\ &= 0.0000000. \end{aligned}

(ii) Take a=b=1a = b = 1 and x=0.5x = 0.5⁠: d2ydx2≈1.312900\frac{d^2y}{dx^2} \approx 1.312900⁠, 2dydx≈5.7875562\frac{dy}{dx} \approx 5.787556⁠, 2y≈4.4746562y \approx 4.474656⁠, and

1.312900−5.787556+4.474656=0.000000.\begin{aligned} &1.312900 - 5.787556 \\ &\quad + 4.474656 = 0.000000. \end{aligned}

(iii) At x=1x = 1⁠: d2ydx2≈−7.210035\frac{d^2y}{dx^2} \approx -7.210035⁠, 9y≈1.2700809y \approx 1.270080⁠, 6cos⁡3≈−5.9399556\cos 3 \approx -5.939955⁠, and

−7.210035+1.270080+5.939955=0.000000.\begin{aligned} &-7.210035 + 1.270080 \\ &\quad + 5.939955 = 0.000000. \end{aligned}

(iv) Take y=ey = e⁠. Then x2=2e2x^2 = 2e^2⁠, so x=2 e≈3.844231x = \sqrt2\,e \approx 3.844231⁠, and Part (iv), Step 2 gives dydx=2 e3e=23≈0.471405\frac{dy}{dx} = \frac{\sqrt2\,e}{3e} = \frac{\sqrt2}{3} \approx 0.471405⁠. Now x2+y2=3e2≈22.167168x^2 + y^2 = 3e^2 \approx 22.167168⁠, so (x2+y2)dydx=2 e2≈10.449703(x^2 + y^2)\frac{dy}{dx} = \sqrt2\,e^2 \approx 10.449703⁠, and xy=2 e2≈10.449703xy = \sqrt2\,e^2 \approx 10.449703 as well.

Common mistakes
  1. In (i), forgetting the yy when differentiating xyxy⁠: the product rule gives xdydx+yx\frac{dy}{dx} + y⁠, and the second derivative then has 2dydx2\frac{dy}{dx}⁠, not one.
  2. Leaving aa and bb in the answer. In (i) and (ii) they must be removed with the given function; a verification that still contains them is unfinished.
  3. Sign slips with e−xe^{-x} and cos⁡\cos⁠. (e−x)′=−e−x(e^{-x})' = -e^{-x} and (cos⁡3x)′=−3sin⁡3x(\cos 3x)' = -3\sin 3x⁠.
  4. In (iv), dividing by 1+2log⁡y1 + 2\log y without a word. It is safe only because y≥1y \ge 1 on the curve.
What to take away
  1. Verify a solution: differentiate, substitute, simplify to L.H.S. = R.H.S.
  2. For an implicit function, differentiate the relation as it stands, then use the relation again to remove constants or awkward terms.
  3. Before dividing, check that the divisor cannot be 0 on the curve.

Every fact used, and where it comes from

FactUsed inSource
A solution makes L.H.S. = R.H.S. when substitutedAll parts, last stepSection 9.3 (Lesson)
Product rule, chain rule, implicit differentiation, second order derivativeAll partsChapter 5, Sections 5.3, 5.3.1, 5.3.2 and 5.7 (Basics)
(ex)′=ex(e^x)' = e^x⁠, (log⁡y)′=1y(\log y)' = \frac{1}{y}Parts (i), (ii), (iv)Chapter 5, Section 5.4 (Basics)
(sin⁡x)′=cos⁡x(\sin x)' = \cos x⁠, (cos⁡x)′=−sin⁡x(\cos x)' = -\sin xParts (ii), (iii)Chapter 5 (Basics)
y=eax(c1cos⁡bx+c2sin⁡bx)y = e^{ax}(c_1\cos bx + c_2\sin bx) solves y′′−2ay′+(a2+b2)y=0y'' - 2ay' + (a^2 + b^2)y = 0Part (ii), Step 3Example 19 (Lesson)
General solution: as many arbitrary constants as the order; particular: noneParts (ii), (iii)Chapter Summary; Section 9.3 (Basics)
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