← 201-SN3-RE, Integral Calculus

Self-check: 201-SN3-RE, Integral Calculus

One question per chapter, 19 in all, taken from the course's corrected exercises. Answer the ones you can do and skip those from a chapter you have not seen yet: each answer is checked right away, and the solution opens after.

With your free account, each answer is kept and your dashboard files each chapter: passed the check, or to work on. These are the same questions as on the set pages: an answer given here counts there.

What the course assumes

These chapters come from an earlier course, and this one relies on them from the first weeks.

201-SN2-RE · Limits and continuity

The figure shows the graph of f(x)=3x2−2x+1x2−4f(x)=\frac{3x^{2}-2x+1}{x^{2}-4}, without its asymptotes.

−8−6−4−22468−6−4−224681012xy

a) Compute lim⁡x→+∞f(x)\lim_{x\to+\infty}f(x) and lim⁡x→−∞f(x)\lim_{x\to-\infty}f(x) for the function in the figure, and identify the horizontal asymptote. What general method do you use?

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Answer

a) y=3y=3 on both sides

a) General method: divide top and bottom by the highest power present, here x2x^{2}: f(x)=3−2x+1x21−4x2f(x)=\frac{3-\frac{2}{x}+\frac{1}{x^{2}}}{1-\frac{4}{x^{2}}}. As x→±∞x\to\pm\infty, all the terms in 1x\frac{1}{x} and 1x2\frac{1}{x^{2}} vanish: the limit is 31=3\frac{3}{1}=3 on BOTH sides. Horizontal asymptote: y=3y=3, the horizontal dashed line in the solution figure. A legitimate shortcut for a rational function with EQUAL degrees: the ratio of the leading coefficients, here 31\frac{3}{1}.

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201-SN2-RE · Derivatives of trigonometric, exponential and logarithmic functions

The chain rule never gets tired: you can apply it as many times as there are nested functions. The only discipline is to name the layers from the outside in BEFORE writing anything.

a) Differentiate f(x)=esin⁡(2x)f(x)=e^{\sin(2x)}, naming the three layers.

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Answer

a) 2cos⁡(2x)esin⁡(2x)2\cos(2x)e^{\sin(2x)}

a) Three layers: the exponential, then the sine, then 2x2x. f′(x)=esin⁡(2x)⋅cos⁡(2x)⋅2=2cos⁡(2x)esin⁡(2x)f'(x)=e^{\sin(2x)}\cdot\cos(2x)\cdot 2=2\cos(2x)e^{\sin(2x)}. The factor 2 from the innermost layer is the one that gets forgotten: check at x=0x=0, f′(0)=2⋅1⋅e0=2f'(0)=2\cdot 1\cdot e^{0}=2, whereas without the factor you would find 1, a slope half as large as it should be.

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The chapters of the course

In the order of the course.

Chapter 1 · Antiderivatives and the indefinite integral

Two situations where the “+C+C” hides a subtlety: when the integrand has a corner, and when the domain is in two pieces.

a) Compute ∫∣x∣ dx\int|x|\,dx by treating x≥0x\geq 0 and x<0x<0 separately, then join the two pieces.

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a) ±x22+C\pm\frac{x^{2}}{2}+C, a single constant by continuity

a) For x≥0x\geq 0, ∣x∣=x|x|=x, so an antiderivative is x22+C1\frac{x^{2}}{2}+C_{1}. For x<0x<0, ∣x∣=−x|x|=-x, so an antiderivative is −x22+C2-\frac{x^{2}}{2}+C_{2}. These two pieces must JOIN UP: an antiderivative is differentiable, hence continuous, and continuity at 0 forces 02+C1=−02+C2\frac{0}{2}+C_{1}=-\frac{0}{2}+C_{2}, that is, C1=C2C_{1}=C_{2}. So there is only one constant, not two: F(x)=x22+CF(x)=\frac{x^{2}}{2}+C for x≥0x\geq 0, F(x)=−x22+CF(x)=-\frac{x^{2}}{2}+C for x<0x<0.

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Chapter 2 · Partial fraction decomposition

A partial fraction is a fraction that cannot be broken down any further: a constant numerator over a power of a linear factor, or a numerator of degree at most 1 over a power of a quadratic with no real root. Before computing anything, you must be able to recognize what is already finished. That is three exam marks earned in thirty seconds, and above all the only way to avoid decomposing a fraction that has nothing to give.

a) Give the domain of 32x−5\frac{3}{2x-5}, of 2xx2+9\frac{2x}{x^2+9}, of 12x2−8x\frac{1}{2x^2-8x} and of 2(x−3)2\frac{2}{(x-3)^2}.

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a) R∖{52}\mathbb{R}\setminus\{\frac{5}{2}\}, R\mathbb{R}, R∖{0,4}\mathbb{R}\setminus\{0, 4\}, R∖{3}\mathbb{R}\setminus\{3\}

a) Exclude the roots of the denominator. 2x−5=02x-5=0 gives x=52x=\frac52, so the domain is R∖{52}\mathbb{R}\setminus\left\{\frac52\right\}. x2+9x^2+9 never vanishes on R\mathbb{R}, so the domain is all of R\mathbb{R}: an irreducible denominator creates no excluded value, which is the first visible sign that it is irreducible. 2x2−8x=2x(x−4)2x^2-8x=2x(x-4) vanishes at 0 and at 4, so the domain is R∖{0,4}\mathbb{R}\setminus\{0, 4\}. Finally (x−3)2(x-3)^2 vanishes only at 3, domain R∖{3}\mathbb{R}\setminus\{3\}.

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Chapter 3 · Integration techniques

Every rational function can be integrated: you take it apart into elementary pieces whose antiderivatives are logarithms, powers and arctangents.

a) Compute ∫x+5x2+x−2dx\int\frac{x+5}{x^{2}+x-2}dx (two simple factors).

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Answer

a) −ln⁡∣x+2∣+2ln⁡∣x−1∣+C-\ln|x+2|+2\ln|x-1|+C

a) x2+x−2=(x+2)(x−1)x^{2}+x-2=(x+2)(x-1). Set x+5(x+2)(x−1)=Ax+2+Bx−1\frac{x+5}{(x+2)(x-1)}=\frac{A}{x+2}+\frac{B}{x-1}, that is x+5=A(x−1)+B(x+2)x+5=A(x-1)+B(x+2). Method of convenient values: x=1x=1: 6=3B6=3B, B=2B=2; x=−2x=-2: 3=−3A3=-3A, A=−1A=-1. Hence ∫=−ln⁡∣x+2∣+2ln⁡∣x−1∣+C=ln⁡(x−1)2∣x+2∣+C\int=-\ln|x+2|+2\ln|x-1|+C=\ln\frac{(x-1)^{2}}{|x+2|}+C.

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Chapter 4 · Integration tricks: Weierstrass, King's rule, Wallis

Every rational function of sin⁡x\sin x and cos⁡x\cos x becomes a rational function of tt under t=tan⁡x2t=\tan\frac{x}{2}. It is the only technique of the chapter that is universal. Very often, it is also the heaviest one, and it hides a continuity trap.

d) On which interval is the substitution legitimate? What happens if it is applied as is to ∫02πdx2+cos⁡x\displaystyle\int_{0}^{2\pi}\dfrac{dx}{2+\cos x}, and what is the true value?

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Answer

d) Wrong 00; true value 2π3≈3.628\frac{2\pi}{\sqrt{3}}\approx 3.628

d) The substitution requires t=tan⁡x2t=\tan\frac{x}{2} to be continuous, so x2\frac{x}{2} must avoid π2\frac{\pi}{2}: it is only legitimate on an interval contained in (−π,π)\left(-\pi,\pi\right), up to a shift by a multiple of 2π2\pi. On [0,2π][0,2\pi], tt starts at 0, tends to +∞+\infty at x=πx=\pi, reappears at −∞-\infty and climbs back to 0: blindly applying the antiderivative 23arctan⁡t3\dfrac{2}{\sqrt{3}}\arctan\dfrac{t}{\sqrt{3}} gives F(2π)−F(0)=0−0=0F\left(2\pi\right)-F\left(0\right)=0-0=0. Yet the integrand 12+cos⁡x\dfrac{1}{2+\cos x} is everywhere greater than 13\frac{1}{3}: the integral is at least 2π3\frac{2\pi}{3}. The true value, obtained by splitting at x=πx=\pi and doubling by symmetry, is 2π3≈3.628\dfrac{2\pi}{\sqrt{3}}\approx 3.628. Remember: a zero for the integral of a strictly positive function is not a computation error, it is a DOMAIN error.

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Chapter 5 · L'Hôpital's rule and indeterminate forms, 201-SN3-RE (201-NYB)

An indeterminate limit is almost never asked for its own sake: it shows up when you look for an asymptote, when you want to make a function continuous, or when a parameter must be adjusted so that a model makes sense.

a) Find the oblique asymptote of f(x)=x2+3xf(x)=\sqrt{x^{2}+3x} as x→+∞x\to+\infty, then as x→−∞x\to-\infty. The two answers are different: explain precisely where the difference comes from.

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a) y=x+32y=x+\frac{3}{2} at +∞+\infty, y=−x−32y=-x-\frac{3}{2} at −∞-\infty

a) As x→+∞x\to+\infty: the oblique asymptote is written y=mx+py=mx+p with m=lim⁡f(x)xm=\lim\frac{f(x)}{x} and p=lim⁡(f(x)−mx)p=\lim\left(f(x)-mx\right). Here x2+3xx=1+3x→1\frac{\sqrt{x^{2}+3x}}{x}=\sqrt{1+\frac{3}{x}}\to 1, so m=1m=1; then p=lim⁡x→∞(x2+3x−x)=32p=\lim_{x\to\infty}\left(\sqrt{x^{2}+3x}-x\right)=\frac{3}{2} by the conjugate, a computation already done in exercise 3d. The asymptote is y=x+32y=x+\frac{3}{2}. As x→−∞x\to-\infty: careful, x2=∣x∣=−x\sqrt{x^{2}}=|x|=-x since xx is negative. Then x2+3xx=∣x∣1+3xx=−1+3x→−1\frac{\sqrt{x^{2}+3x}}{x}=\frac{|x|\sqrt{1+\frac{3}{x}}}{x}=-\sqrt{1+\frac{3}{x}}\to -1, so m=−1m=-1; and p=lim⁡x→−∞(x2+3x+x)=−32p=\lim_{x\to-\infty}\left(\sqrt{x^{2}+3x}+x\right)=-\frac{3}{2} by the same conjugate. The asymptote is y=−x−32y=-x-\frac{3}{2}. The difference comes ENTIRELY from the simplification x2=∣x∣\sqrt{x^{2}}=|x|: writing x2=x\sqrt{x^{2}}=x without discussing the sign is the most widespread mistake on oblique asymptotes, and it gives a wrong line on one side of the graph out of two. Numerical check: for x=106x=10^{6}, f(x)−x≈1.4999989f(x)-x\approx 1.4999989; for x=−106x=-10^{6}, f(x)+x≈−1.5000011f(x)+x\approx -1.5000011.

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Chapter 6 · Definite and improper integrals, 201-SN3-RE (201-NYB)

The figure gives the graph of a piecewise linear function ff on [0,8][0, 8]. Let F(x)=∫0xf(t) dtF(x)=\int_{0}^{x}f(t)\,dt: the area accumulated from 0, counted positively above the axis and negatively below it. The whole study of FF can be read from this picture, with no formula for ff.

12345678−3−2−112345y = f(x)+−

b) Find the intervals on which FF increases and decreases, and locate its maximum on [0,8][0, 8]. A student answers that FF is largest where ff is largest, so at x=2x=2: correct this and explain the confusion.

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Answer

b) FF increases on [0,4][0, 4], decreases on [4,8][4, 8]; maximum 88 at x=4x=4

b) The Fundamental Theorem gives F′=fF'=f: the sign of ff drives the variations of FF. Now f>0f>0 on (0,4)(0, 4) and f<0f<0 on (4,8)(4, 8). So FF INCREASES on [0,4][0, 4] and DECREASES on [4,8][4, 8], with a maximum at x=4x=4, of value F(4)=8F(4)=8. The student's confusion is reading the graph as if it were FF: what is drawn is ff, that is, the DERIVATIVE of FF. At x=2x=2, ff reaches its maximum, which means FF is increasing FASTEST there, not that it is highest. FF peaks where its derivative is zero and changes sign, so at x=4x=4, exactly when ff crosses the axis from positive to negative.

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Chapter 7 · Area between curves, 201-SN3-RE (201-NYB)

Let f(x)=x3−4xf(x)=x^{3}-4x on the interval [−2,2]\left[-2, 2\right].

−2,5−2−1,5−1−0,50,511,522,5−4−3−2−11234y = x³ − 4x

b) Compute the AREA between the curve and the xx-axis on the same interval.

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Answer

b) Splitting at the zeros: 4+4=84+4=8

b) The area cannot be zero: the curve clearly moves away from the axis. You must split at the ZEROS of ff, that is where x(x−2)(x+2)=0x(x-2)(x+2)=0, so at −2-2, 00 and 22. On (−2,0)\left(-2, 0\right), f>0f>0 (for example f(−1)=3f(-1)=3); on (0,2)\left(0, 2\right), f<0f<0 (for example f(1)=−3f(1)=-3). So A=∫−20f(x) dx−∫02f(x) dx\mathcal{A}=\int_{-2}^{0}f(x)\,dx-\int_{0}^{2}f(x)\,dx. The first piece equals [x44−2x2]−20=0−(4−8)=4\left[\frac{x^{4}}{4}-2x^{2}\right]_{-2}^{0}=0-(4-8)=4 and the second [x44−2x2]02=−4\left[\frac{x^{4}}{4}-2x^{2}\right]_{0}^{2}=-4. Hence A=4−(−4)=8\mathcal{A}=4-(-4)=8.

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Chapter 8 · Numerical integration, 201-SN3-RE (201-NYB)

The most discriminating exam format of the chapter: you are not asked to approximate the integral, you are asked HOW MANY subintervals guarantee an accuracy fixed in advance. The direction of the inequality must be under control.

b) Same question for Simpson's rule. Watch out for the parity condition.

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Answer

b) n=8n=8 (even)

b) We require M(b−a)5180n4<10−4\frac{M(b-a)^{5}}{180n^{4}}<10^{-4} with M=24M=24, that is 24180n4<10−4\frac{24}{180n^{4}}<10^{-4}, so n4>24×104180=1333.33n^{4}>\frac{24\times 10^{4}}{180}=1333.33, so n>6.04n>6.04. The next integer would be 7, but nn must be EVEN for Simpson: so take n=8n=8. Check: 24180×4096=3.26×10−5<10−4\frac{24}{180\times 4096}=3.26\times 10^{-5}<10^{-4} ✓. Note in passing that n=6n=6 would not be enough, since 24180×1296=1.03×10−4\frac{24}{180\times 1296}=1.03\times 10^{-4}, very slightly above the threshold: rounding up to the next even integer is not an unnecessary precaution, here it is the difference between guaranteeing and not guaranteeing.

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Chapter 9 · Applications of integration, 201-SN3-RE (201-NYB)

The slice of curve is a hypotenuse: ds=dx2+dy2=1+[f′(x)]2 dxds=\sqrt{dx^{2}+dy^{2}}=\sqrt{1+[f'(x)]^{2}}\,dx. When rotated, it sweeps out a band of area 2πf(x) ds2\pi f(x)\,ds.

a) Justify the arc length formula by applying Pythagoras to the slice, then compute the length of y=x3/2y=x^{3/2} on [0,4][0,4].

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Answer

a) 827(103/2−1)≈9.07\frac{8}{27}(10^{3/2}-1)\approx 9.07

a) Over one slice, the curve moves forward by dxdx and up by dy=f′(x)dxdy=f'(x)dx: its length is the hypotenuse dx2+dy2=1+[f′(x)]2 dx\sqrt{dx^{2}+dy^{2}}=\sqrt{1+[f'(x)]^{2}}\,dx, which you add up. Here f′(x)=32x1/2f'(x)=\frac{3}{2}x^{1/2}: L=∫041+9x4 dx=[827(1+9x4)3/2]04=827(103/2−1)≈9.07L=\int_{0}^{4}\sqrt{1+\frac{9x}{4}}\,dx=\left[\frac{8}{27}\left(1+\frac{9x}{4}\right)^{3/2}\right]_{0}^{4}=\frac{8}{27}\left(10^{3/2}-1\right)\approx 9.07: a little more than the chord 42+82≈8.94\sqrt{4^{2}+8^{2}}\approx 8.94, as it should be.

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Chapter 10 · Parametric curves

Let CC be the curve defined by x=t2x=t^{2} and y=t3−3ty=t^{3}-3t, t∈Rt\in\mathbb{R}. It is the archetype of the chapter: it has a vertical tangent line, two horizontal tangent lines, and it crosses itself.

−112345−4−3−2−11234

a) Compute x′(t)x'(t), y′(t)y'(t) and dydx\dfrac{dy}{dx} in terms of tt. For which value of tt does the quotient make no sense?

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a) dydx=3t2−32t\frac{dy}{dx}=\frac{3t^{2}-3}{2t}, t≠0t\neq 0

a) x′(t)=2tx'(t)=2t and y′(t)=3t2−3y'(t)=3t^{2}-3, so dydx=3t2−32t\dfrac{dy}{dx}=\dfrac{3t^{2}-3}{2t} for t≠0t\neq 0. The quotient makes no sense at t=0t=0, precisely where the tangent line will be vertical.

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Chapter 11 · Polar coordinates, 201-SN3-RE (201-NYB)

Going from Cartesian to polar takes two computations: a modulus, which never causes trouble, and an angle, which almost always does. The calculator returns arctan⁡yx\arctan\frac{y}{x}, a value between −π2-\frac{\pi}{2} and π2\frac{\pi}{2}: it can therefore NEVER designate a point in the second or third quadrant.

a) Give a polar representation of (−1,3)\left(-1,\sqrt{3}\right) with r>0r>0 and θ∈[0,2π)\theta\in[0, 2\pi). Compare with what arctan⁡yx\arctan\frac{y}{x} returns.

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a) (2,2π3)\left(2, \frac{2\pi}{3}\right); arctan⁡\arctan gives −π3-\frac{\pi}{3}, wrong

a) r=1+3=2r=\sqrt{1+3}=2. The point is in the SECOND quadrant (x<0x<0, y>0y>0). The calculator gives arctan⁡(3−1)=arctan⁡(−3)=−π3\arctan\left(\frac{\sqrt{3}}{-1}\right)=\arctan\left(-\sqrt{3}\right)=-\frac{\pi}{3}, which designates a point in the fourth quadrant: that is wrong. You must add π\pi: θ=−π3+π=2π3\theta=-\frac{\pi}{3}+\pi=\frac{2\pi}{3}. Check: 2cos⁡2π3=−12\cos\frac{2\pi}{3}=-1 and 2sin⁡2π3=32\sin\frac{2\pi}{3}=\sqrt{3}.

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Chapter 12 · Sequences, 201-SN3-RE (201-NYB)

A sum whose number of terms GROWS with nn cannot be handled by any of the techniques of exercise 2: you cannot take the limit term by term, since the number of terms changes. The tool lies elsewhere, and it comes from integral calculus: if the sum has the form 1n∑f(kn)\frac{1}{n}\sum f\left(\frac{k}{n}\right), it is a Riemann sum, and its limit is an integral.

b) Why can we NOT conclude that lim⁡n→∞∑k=1n1n+k=0\lim_{n\to\infty}\sum_{k=1}^{n}\frac{1}{n+k}=0 on the grounds that each term tends to 0? Compute the true limit by recognizing a Riemann sum.

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Answer

b) ln⁡2≈0.693\ln 2\approx 0.693

b) The reasoning is wrong because the NUMBER of terms grows while each term shrinks. Each term 1n+k\frac{1}{n+k} is of order 1n\frac{1}{n}, but there are nn of them: the total stays of order n⋅1n=1n\cdot\frac{1}{n}=1, so nothing tends to 0. It is the same illusion as for the harmonic series: infinitely many tiny contributions can add up to a nonzero amount, and “taking the limit term by term” is only allowed if the number of terms is FIXED. Correct calculation: ∑k=1n1n+k=∑k=1n1n(1+kn)=1n∑k=1n11+kn\sum_{k=1}^{n}\frac{1}{n+k}=\sum_{k=1}^{n}\frac{1}{n\left(1+\frac{k}{n}\right)}=\frac{1}{n}\sum_{k=1}^{n}\frac{1}{1+\frac{k}{n}}, which is the Riemann sum of f(x)=11+xf(x)=\frac{1}{1+x} on [0,1][0,1]. The limit is therefore ∫01dx1+x=[ln⁡(1+x)]01=ln⁡2≈0.693\int_{0}^{1}\frac{dx}{1+x}=\left[\ln(1+x)\right]_{0}^{1}=\ln 2\approx 0.693. Numerical check: the sum is 0.66880.6688 for n=10n=10 and 0.693140.69314 for n=105n=10^{5}, the convergence is slow and from below.

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Chapter 13 · Infinite series, 201-SN3-RE (201-NYB)

The classic exam format: a list of series to classify (absolute convergence, conditional convergence or divergence) with the RIGHT test and a complete justification. Choosing the test is worth half the marks.

b) ∑n=1∞(−1)nnn+1\sum_{n=1}^{\infty}(-1)^{n}\frac{n}{n+1} and ∑n=1∞n2n4+1\sum_{n=1}^{\infty}\frac{n^{2}}{n^{4}+1}: convergence of each.

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Answer

b) Divergent; absolute

b) (−1)nnn+1(-1)^{n}\frac{n}{n+1}: the general term does not tend to 0 (it oscillates between values close to +1+1 and −1-1): DIVERGENT by the divergence test: Leibniz does not apply (bn→1≠0b_{n}\to 1\ne 0) and should not even be invoked. n2n4+1\frac{n^{2}}{n^{4}+1}: positive, compares with n2n4=1n2\frac{n^{2}}{n^{4}}=\frac{1}{n^{2}}: n2n4+1≤1n2\frac{n^{2}}{n^{4}+1}\le\frac{1}{n^{2}}, p-series with p=2p=2: CONVERGENT (absolutely, since it is positive).

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Chapter 14 · Series with sin, cos, exp and ln terms, 201-SN3-RE (201-NYB)

The Alternating Series Test requires THREE hypotheses: terms of alternating sign, decreasing absolute values, and a limit of zero. If a single one is missing, the test does not apply.

a) Show that ∑n≥1(−1)n+1n2\sum_{n\geq 1}\frac{(-1)^{n+1}}{n^{2}} converges. Given that its sum is π212\frac{\pi^{2}}{12}, how many terms are needed to approximate it to within 10−310^{-3}?

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Answer

a) Converges; N=31N=31 terms

a) The sequence 1n2\frac{1}{n^{2}} is positive, decreasing and tends to 0: the Alternating Series Test applies and the series converges. The remainder after NN terms satisfies ∣RN∣≤1(N+1)2|R_{N}|\leq\dfrac{1}{(N+1)^{2}}. We want 1(N+1)2<10−3\dfrac{1}{(N+1)^{2}}<10^{-3}, that is (N+1)2>1000(N+1)^{2}>1000, so N+1>31.6N+1>31.6 and N≥31N\geq 31. Check: with 31 terms, the actual gap with π212≈0.8224670\frac{\pi^{2}}{12}\approx 0.8224670 is 5.0×10−45.0\times 10^{-4}, indeed below the bound.

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Chapter 15 · Advanced tests: root, condensation, Raabe, Abel, 201-SN3-RE (201-NYB)

Deciding whether a series converges is one thing; computing its sum is another. For rational fractions, partial fraction decomposition often reveals a telescoping sum that gives the exact value.

b) Same work for ∑n≥11n(n+2)\sum_{n\geq 1}\frac{1}{n(n+2)}. Careful: here the telescoping leaves TWO terms.

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Answer

b) 34\frac{3}{4}

b) 1n(n+2)=12(1n−1n+2)\frac{1}{n(n+2)}=\frac{1}{2}\left(\frac{1}{n}-\frac{1}{n+2}\right). Since the shift is 2, the terms cancel two indices apart, and TWO terms REMAIN at the start: SN=12(1+12−1N+1−1N+2)⟶12⋅32=34S_{N}=\frac{1}{2}\left(1+\frac{1}{2}-\frac{1}{N+1}-\frac{1}{N+2}\right)\longrightarrow\frac{1}{2}\cdot\frac{3}{2}=\frac{3}{4}. The general rule: a shift of kk leaves kk terms on each side.

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Chapter 16 · Power series and Taylor series, 201-SN3-RE (201-NYB)

A power series ∑cn(x−a)n\sum c_{n}(x-a)^{n} converges on an interval centred at aa: the Ratio Test gives the radius, but each of the two endpoints needs its own analysis.

a) Find the radius AND the interval of convergence of ∑n=1∞xnn\sum_{n=1}^{\infty}\frac{x^{n}}{n} (endpoints included).

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a)
Interval ,
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Answer

a) R=1R=1, interval [−1,1)[-1, 1)

a) Ratio Test: ∣xn+1n+1⋅nxn∣=∣x∣nn+1→∣x∣\left|\frac{x^{n+1}}{n+1}\cdot\frac{n}{x^{n}}\right|=|x|\frac{n}{n+1}\to|x|: convergence for ∣x∣<1|x|<1, so R=1R=1. Endpoints: at x=1x=1, the harmonic series ∑1n\sum\frac{1}{n} DIVERGES; at x=−1x=-1, the alternating harmonic series CONVERGES (Alternating Series Test). Interval: [−1,1)[-1, 1): closed on one side, open on the other, and it took both tests to know it.

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Chapter 17 · Differential equations

None of these equations comes in its textbook form. Before any computation, rewrite it until you recognize its TYPE: separable dydx=f(x)g(y)\frac{dy}{dx}=f(x)g(y), linear y′+P(x)y=Q(x)y'+P(x)y=Q(x), homogeneous y′=F(yx)y'=F\left(\frac{y}{x}\right), or linear if xx is viewed as a function of yy. Then solve through the given point: the point (x0,y0)(x_{0}, y_{0}) means y(x0)=y0y(x_{0})=y_{0}.

a) dydx=e2x+y+ey\dfrac{dy}{dx}=e^{2x+y}+e^{y}, through the point (0,0)(0, 0). Compute y(−12)y\left(-\frac{1}{2}\right) and the right endpoint of the interval on which the solution exists.

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a)
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Answer

a) Separable: y=−ln⁡(32−x−e2x2)y=-\ln\left(\frac{3}{2}-x-\frac{e^{2x}}{2}\right), y(−12)≈−0.597y\left(-\frac{1}{2}\right)\approx -0.597, right endpoint ≈0.396\approx 0.396

a) The trap is in the exponent: e2x+y=e2x eye^{2x+y}=e^{2x}\,e^{y}, not e2x+eye^{2x}+e^{y}. Factor out eye^{y}: dydx=ey(e2x+1)\dfrac{dy}{dx}=e^{y}\left(e^{2x}+1\right), a SEPARABLE equation. e−y dy=(e2x+1)dxe^{-y}\,dy=\left(e^{2x}+1\right)dx, so −e−y=e2x2+x+C-e^{-y}=\dfrac{e^{2x}}{2}+x+C. At the point (0,0)(0, 0): −1=12+C-1=\frac{1}{2}+C, C=−32C=-\frac{3}{2}. Hence e−y=32−x−e2x2e^{-y}=\dfrac{3}{2}-x-\dfrac{e^{2x}}{2} and y=−ln⁡(32−x−e2x2)y=-\ln\left(\dfrac{3}{2}-x-\dfrac{e^{2x}}{2}\right). At x=−12x=-\frac{1}{2}: 32+12−e−12=2−12e≈1.816\frac{3}{2}+\frac{1}{2}-\frac{e^{-1}}{2}=2-\frac{1}{2e}\approx 1.816, so y≈−0.597y\approx -0.597. The solution exists only as long as the argument of the logarithm is positive: 3−2x−e2x>03-2x-e^{2x}>0. This function is strictly decreasing, equals 11 at 00 and vanishes between 0.390.39 and 0.400.40; by bisection, the right endpoint is about 0.3960.396. As you approach it, e−y→0e^{-y}\to 0 and y→+∞y\to+\infty: the solution blows up in finite time, although the right-hand side looked harmless.

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