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.
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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)=x2−43x2−2x+1, without its asymptotes.
a) Compute limx→+∞f(x) and limx→−∞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=3 on both sides
a) General method: divide top and bottom by the highest power present, here x2: f(x)=1−x243−x2+x21. As x→±∞, all the terms in x1 and x21 vanish: the limit is 13=3 on BOTH sides. Horizontal asymptote: y=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 13.
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), naming the three layers.
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Answer
a)2cos(2x)esin(2x)
a) Three layers: the exponential, then the sine, then 2x. f′(x)=esin(2x)⋅cos(2x)⋅2=2cos(2x)esin(2x). The factor 2 from the innermost layer is the one that gets forgotten: check at x=0, f′(0)=2⋅1⋅e0=2, whereas without the factor you would find 1, a slope half as large as it should be.
Chapter 1 · Antiderivatives and the indefinite integral
Two situations where the “+C” hides a subtlety: when the integrand has a corner, and when the domain is in two pieces.
a) Compute ∫∣x∣dx by treating x≥0 and x<0 separately, then join the two pieces.
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Answer
a)±2x2+C, a single constant by continuity
a) For x≥0, ∣x∣=x, so an antiderivative is 2x2+C1. For x<0, ∣x∣=−x, so an antiderivative is −2x2+C2. These two pieces must JOIN UP: an antiderivative is differentiable, hence continuous, and continuity at 0 forces 20+C1=−20+C2, that is, C1=C2. So there is only one constant, not two: F(x)=2x2+C for x≥0, F(x)=−2x2+C for x<0.
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 2x−53, of x2+92x, of 2x2−8x1 and of (x−3)22.
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Answer
a)R∖{25}, R, R∖{0,4}, R∖{3}
a) Exclude the roots of the denominator. 2x−5=0 gives x=25, so the domain is R∖{25}. x2+9 never vanishes on R, so the domain is all of R: an irreducible denominator creates no excluded value, which is the first visible sign that it is irreducible. 2x2−8x=2x(x−4) vanishes at 0 and at 4, so the domain is R∖{0,4}. Finally (x−3)2 vanishes only at 3, domain R∖{3}.
Every rational function can be integrated: you take it apart into elementary pieces whose antiderivatives are logarithms, powers and arctangents.
a) Compute ∫x2+x−2x+5dx (two simple factors).
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Answer
a)−ln∣x+2∣+2ln∣x−1∣+C
a) x2+x−2=(x+2)(x−1). Set (x+2)(x−1)x+5=x+2A+x−1B, that is x+5=A(x−1)+B(x+2). Method of convenient values: x=1: 6=3B, B=2; x=−2: 3=−3A, A=−1. Hence ∫=−ln∣x+2∣+2ln∣x−1∣+C=ln∣x+2∣(x−1)2+C.
Every rational function of sinx and cosx becomes a rational function of t under t=tan2x. 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 ∫02π2+cosxdx, and what is the true value?
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Answer
d)Wrong 0; true value 32π≈3.628
d) The substitution requires t=tan2x to be continuous, so 2x must avoid 2π: it is only legitimate on an interval contained in (−π,π), up to a shift by a multiple of 2π. On [0,2π], t starts at 0, tends to +∞ at x=π, reappears at −∞ and climbs back to 0: blindly applying the antiderivative 32arctan3t gives F(2π)−F(0)=0−0=0. Yet the integrand 2+cosx1 is everywhere greater than 31: the integral is at least 32π. The true value, obtained by splitting at x=π and doubling by symmetry, is 32π≈3.628. Remember: a zero for the integral of a strictly positive function is not a computation error, it is a DOMAIN error.
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+3x as x→+∞, then as x→−∞. The two answers are different: explain precisely where the difference comes from.
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Answer
a)y=x+23 at +∞, y=−x−23 at −∞
a) As x→+∞: the oblique asymptote is written y=mx+p with m=limxf(x) and p=lim(f(x)−mx). Here xx2+3x=1+x3→1, so m=1; then p=limx→∞(x2+3x−x)=23 by the conjugate, a computation already done in exercise 3d. The asymptote is y=x+23. As x→−∞: careful, x2=∣x∣=−x since x is negative. Then xx2+3x=x∣x∣1+x3=−1+x3→−1, so m=−1; and p=limx→−∞(x2+3x+x)=−23 by the same conjugate. The asymptote is y=−x−23. The difference comes ENTIRELY from the simplification x2=∣x∣: writing x2=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=106, f(x)−x≈1.4999989; for x=−106, f(x)+x≈−1.5000011.
Chapter 6 · Definite and improper integrals, 201-SN3-RE (201-NYB)
The figure gives the graph of a piecewise linear function f on [0,8]. Let F(x)=∫0xf(t)dt: the area accumulated from 0, counted positively above the axis and negatively below it. The whole study of F can be read from this picture, with no formula for f.
b) Find the intervals on which F increases and decreases, and locate its maximum on [0,8]. A student answers that F is largest where f is largest, so at x=2: correct this and explain the confusion.
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Answer
b)F increases on [0,4], decreases on [4,8]; maximum 8 at x=4
b) The Fundamental Theorem gives F′=f: the sign of f drives the variations of F. Now f>0 on (0,4) and f<0 on (4,8). So F INCREASES on [0,4] and DECREASES on [4,8], with a maximum at x=4, of value F(4)=8. The student's confusion is reading the graph as if it were F: what is drawn is f, that is, the DERIVATIVE of F. At x=2, f reaches its maximum, which means F is increasing FASTEST there, not that it is highest. F peaks where its derivative is zero and changes sign, so at x=4, exactly when f crosses the axis from positive to negative.
Chapter 7 · Area between curves, 201-SN3-RE (201-NYB)
Let f(x)=x3−4x on the interval [−2,2].
b) Compute the AREA between the curve and the x-axis on the same interval.
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Answer
b)Splitting at the zeros: 4+4=8
b) The area cannot be zero: the curve clearly moves away from the axis. You must split at the ZEROS of f, that is where x(x−2)(x+2)=0, so at −2, 0 and 2. On (−2,0), f>0 (for example f(−1)=3); on (0,2), f<0 (for example f(1)=−3). So A=∫−20f(x)dx−∫02f(x)dx. The first piece equals [4x4−2x2]−20=0−(4−8)=4 and the second [4x4−2x2]02=−4. Hence A=4−(−4)=8.
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=8 (even)
b) We require 180n4M(b−a)5<10−4 with M=24, that is 180n424<10−4, so n4>18024×104=1333.33, so n>6.04. The next integer would be 7, but n must be EVEN for Simpson: so take n=8. Check: 180×409624=3.26×10−5<10−4 ✓. Note in passing that n=6 would not be enough, since 180×129624=1.03×10−4, 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.
Chapter 9 · Applications of integration, 201-SN3-RE (201-NYB)
The slice of curve is a hypotenuse: ds=dx2+dy2=1+[f′(x)]2dx. When rotated, it sweeps out a band of area 2πf(x)ds.
a) Justify the arc length formula by applying Pythagoras to the slice, then compute the length of y=x3/2 on [0,4].
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Answer
a)278(103/2−1)≈9.07
a) Over one slice, the curve moves forward by dx and up by dy=f′(x)dx: its length is the hypotenuse dx2+dy2=1+[f′(x)]2dx, which you add up. Here f′(x)=23x1/2: L=∫041+49xdx=[278(1+49x)3/2]04=278(103/2−1)≈9.07: a little more than the chord 42+82≈8.94, as it should be.
Let C be the curve defined by x=t2 and y=t3−3t, t∈R. It is the archetype of the chapter: it has a vertical tangent line, two horizontal tangent lines, and it crosses itself.
a) Compute x′(t), y′(t) and dxdy in terms of t. For which value of t does the quotient make no sense?
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Answer
a)dxdy=2t3t2−3, t=0
a) x′(t)=2t and y′(t)=3t2−3, so dxdy=2t3t2−3 for t=0. The quotient makes no sense at t=0, precisely where the tangent line will be vertical.
Going from Cartesian to polar takes two computations: a modulus, which never causes trouble, and an angle, which almost always does. The calculator returns arctanxy, a value between −2π and 2π: it can therefore NEVER designate a point in the second or third quadrant.
a) Give a polar representation of (−1,3) with r>0 and θ∈[0,2π). Compare with what arctanxy returns.
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Answer
a)(2,32π); arctan gives −3π, wrong
a) r=1+3=2. The point is in the SECOND quadrant (x<0, y>0). The calculator gives arctan(−13)=arctan(−3)=−3π, which designates a point in the fourth quadrant: that is wrong. You must add π: θ=−3π+π=32π. Check: 2cos32π=−1 and 2sin32π=3.
A sum whose number of terms GROWS with n 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 n1∑f(nk), it is a Riemann sum, and its limit is an integral.
b) Why can we NOT conclude that limn→∞∑k=1nn+k1=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)ln2≈0.693
b) The reasoning is wrong because the NUMBER of terms grows while each term shrinks. Each term n+k1 is of order n1, but there are n of them: the total stays of order n⋅n1=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=1nn+k1=∑k=1nn(1+nk)1=n1∑k=1n1+nk1, which is the Riemann sum of f(x)=1+x1 on [0,1]. The limit is therefore ∫011+xdx=[ln(1+x)]01=ln2≈0.693. Numerical check: the sum is 0.6688 for n=10 and 0.69314 for n=105, the convergence is slow and from below.
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)nn+1n and ∑n=1∞n4+1n2: convergence of each.
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Answer
b)Divergent; absolute
b) (−1)nn+1n: the general term does not tend to 0 (it oscillates between values close to +1 and −1): DIVERGENT by the divergence test: Leibniz does not apply (bn→1=0) and should not even be invoked. n4+1n2: positive, compares with n4n2=n21: n4+1n2≤n21, p-series with p=2: CONVERGENT (absolutely, since it is positive).
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≥1n2(−1)n+1 converges. Given that its sum is 12π2, how many terms are needed to approximate it to within 10−3?
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Answer
a)Converges; N=31 terms
a) The sequence n21 is positive, decreasing and tends to 0: the Alternating Series Test applies and the series converges. The remainder after N terms satisfies ∣RN∣≤(N+1)21. We want (N+1)21<10−3, that is (N+1)2>1000, so N+1>31.6 and N≥31. Check: with 31 terms, the actual gap with 12π2≈0.8224670 is 5.0×10−4, indeed below the bound.
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≥1n(n+2)1. Careful: here the telescoping leaves TWO terms.
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Answer
b)43
b) n(n+2)1=21(n1−n+21). Since the shift is 2, the terms cancel two indices apart, and TWO terms REMAIN at the start: SN=21(1+21−N+11−N+21)⟶21⋅23=43. The general rule: a shift of k leaves k terms on each side.
Chapter 16 · Power series and Taylor series, 201-SN3-RE (201-NYB)
A power series ∑cn(x−a)n converges on an interval centred at a: 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∞nxn (endpoints included).
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Answer
a)R=1, interval [−1,1)
a) Ratio Test: n+1xn+1⋅xnn=∣x∣n+1n→∣x∣: convergence for ∣x∣<1, so R=1. Endpoints: at x=1, the harmonic series ∑n1 DIVERGES; at x=−1, the alternating harmonic series CONVERGES (Alternating Series Test). Interval: [−1,1): closed on one side, open on the other, and it took both tests to know it.
None of these equations comes in its textbook form. Before any computation, rewrite it until you recognize its TYPE: separable dxdy=f(x)g(y), linear y′+P(x)y=Q(x), homogeneous y′=F(xy), or linear if x is viewed as a function of y. Then solve through the given point: the point (x0,y0) means y(x0)=y0.
a) dxdy=e2x+y+ey, through the point (0,0). Compute y(−21) and the right endpoint of the interval on which the solution exists.
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Answer
a)Separable: y=−ln(23−x−2e2x), y(−21)≈−0.597, right endpoint ≈0.396
a) The trap is in the exponent: e2x+y=e2xey, not e2x+ey. Factor out ey: dxdy=ey(e2x+1), a SEPARABLE equation. e−ydy=(e2x+1)dx, so −e−y=2e2x+x+C. At the point (0,0): −1=21+C, C=−23. Hence e−y=23−x−2e2x and y=−ln(23−x−2e2x). At x=−21: 23+21−2e−1=2−2e1≈1.816, so y≈−0.597. The solution exists only as long as the argument of the logarithm is positive: 3−2x−e2x>0. This function is strictly decreasing, equals 1 at 0 and vanishes between 0.39 and 0.40; by bisection, the right endpoint is about 0.396. As you approach it, e−y→0 and y→+∞: the solution blows up in finite time, although the right-hand side looked harmless.
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