Foundations to FrontierPart V: Calculus IIBezhig

Cumulative assessment: Calculus II

12 exercises, each with a complete solution.

Use this assessment after Module 32, retaining Calculus I prerequisites. The method is not named in most statements. A convergence classification is not automatically an evaluation of a sum. A numerical approximation needs its own error interpretation. CII.09 is a synthesis problem and CII.12 is an optional introductory differential-equation extension.

CII.01CSolution

Evaluate ∫x2sin⁡x dx\int x^2\sin x\dd x and verify by differentiation.

CII.02CSolution

Evaluate ∫1/(x2−9) dx\int1/(x^2-9)\dd x on intervals where the integrand is defined. State the restrictions.

CII.03TSolution

Evaluate ∫011/(1+x2)2 dx\int_0^1 1/(1+x^2)^2\dd x. Choose a substitution or identity that makes the remaining integral elementary.

CII.04TSolution

Determine whether ∫1∞(ln⁡x)/x2 dx\int_1^\infty(\ln x)/x^2\dd x converges, and evaluate it if it does.

CII.05CSolution

Use Simpson’s rule with n=4n=4 for ∫01cos⁡x dx\int_0^1\cos x\dd x. Give the approximation and a rigorous absolute-error bound. A calculator may be used for the decimal evaluation.

CII.06TSolution

Prove that ∑n=1∞n2/3n\sum_{n=1}^{\infty}n^2/3^n converges, then find its sum using a justified power-series operation.

CII.07TSolution

Classify ∑n=1∞(−1)n−1/n+1\sum_{n=1}^{\infty}(-1)^{n-1}/\sqrt{n+1}. How many initial terms suffice to guarantee absolute error at most 0.020.02 by the alternating-series bound?

CII.08TSolution

Find the radius and interval of convergence of ∑n=1∞(x−2)n/(n4n)\sum_{n=1}^{\infty}(x-2)^n/(n4^n). Find its derivative as a function on the open interval of convergence, and test the derivative series at both endpoints.

CII.09SSolution

Use the degree-five Maclaurin polynomial for sin⁡(2x)\sin(2x) to approximate ∫01/5sin⁡(2x)/x dx\int_0^{1/5}\sin(2x)/x\dd x, defining the integrand continuously at zero. Bound the absolute error of the resulting integral using the next alternating term.

CII.10TSolution

One cycloid arch is x=t−sin⁡tx=t-\sin t, y=1−cos⁡ty=1-\cos t, 0≤t≤2π0\le t\le2\pi. Find its arc length and the area under the arch above the xx-axis.

CII.11TSolution

Find the area in the first quadrant that is inside the circle r=2r=2 and outside the cardioid r=1+cos⁡θr=1+\cos\theta.

CII.12CSolution

Optional ODE extension: solve y′+2y=4y'+2y=4, y(0)=5y(0)=5, verify your result, and identify its equilibrium and long-term limit.

Optional small hints

For CII.03, x=tan⁡θx=\tan\theta changes the denominator and differential together. For CII.06, apply r  d/ drr\,\dd/\dd r twice to a geometric series with ∣r∣<1|r|<1. For CII.09, bound the integrand’s error before integrating that bound. For CII.10, keep the absolute value in the square root until you know the sign of sin⁡(t/2)\sin(t/2).

Complete solutions: Calculus II assessment#

Compare the first step where your work differs. A corrected answer is not yet an independent success.

CII.01Show solution

Apply integration by parts twice

Take u=x2u=x^2,  dv=sin⁡x dx\dd v=\sin x\dd x, giving v=−cos⁡xv=-\cos x. Then

I=−x2cos⁡x+2∫xcos⁡x dx.I=-x^2\cos x+2\int x\cos x\dd x.

For the remaining integral, take u=xu=x,  dv=cos⁡x dx\dd v=\cos x\dd x, so it equals xsin⁡x+cos⁡xx\sin x+\cos x. Thus

I=−x2cos⁡x+2xsin⁡x+2cos⁡x+C.\boxed{I=-x^2\cos x+2x\sin x+2\cos x+C}.

Differentiation gives −2xcos⁡x+x2sin⁡x+2sin⁡x+2xcos⁡x−2sin⁡x=x2sin⁡x-2x\cos x+x^2\sin x+2\sin x+2x\cos x-2\sin x=x^2\sin x. This check confirms both correction terms and their signs.

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CII.02Show solution

Factor the denominator and solve for constants

The domain excludes x=±3x=\pm3. Write

1(x−3)(x+3)=Ax−3+Bx+3.\frac1{(x-3)(x+3)}=\frac{A}{x-3}+\frac{B}{x+3}.

Multiplying through gives 1=A(x+3)+B(x−3)1=A(x+3)+B(x-3). Evaluating at 33 and −3-3 gives A=1/6A=1/6, B=−1/6B=-1/6. Therefore

16ln⁡∣x−3∣−16ln⁡∣x+3∣+C\boxed{\frac16\ln|x-3|-\frac16\ln|x+3|+C}

is an antiderivative on each interval avoiding the singularities. Constants may differ between disconnected intervals. Differentiating recovers [(x+3)−(x−3)]/[6(x2−9)]=1/(x2−9)[(x+3)-(x-3)]/[6(x^2-9)]=1/(x^2-9).

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CII.03Show solution

A trigonometric substitution removes a quadratic denominator

Set x=tan⁡θx=\tan\theta on 0≤θ≤π/40\le\theta\le\pi/4. Then  dx=sec⁡2θ dθ\dd x=\sec^2\theta\dd\theta and (1+x2)2=sec⁡4θ(1+x^2)^2=\sec^4\theta, so

I=∫0π/4cos⁡2θ dθ=[θ2+sin⁡2θ4]0π/4=π8+14.I=\int_0^{\pi/4}\cos^2\theta\dd\theta =\left[\frac\theta2+\frac{\sin2\theta}{4}\right]_0^{\pi/4} =\boxed{\frac\pi8+\frac14}.

The original integrand lies between 1/41/4 and 11 on an interval of length one, and the answer lies between those bounds. No sign ambiguity arises because the chosen tangent branch is one-to-one here.

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CII.04Show solution

Integration by parts leaves a vanishing tail

For a finite upper endpoint bb, take u=ln⁡xu=\ln x,  dv=x−2 dx\dd v=x^{-2}\dd x, giving v=−1/xv=-1/x. Then

∫1bln⁡xx2 dx=[−ln⁡xx]1b+∫1b1x2 dx=1−ln⁡b+1b.\int_1^b\frac{\ln x}{x^2}\dd x =\left[-\frac{\ln x}{x}\right]_1^b+\int_1^b\frac1{x^2}\dd x =1-\frac{\ln b+1}{b}.

Since ln⁡b/b→0\ln b/b\to0 and 1/b→01/b\to0, the improper integral converges to 1\boxed1. The boundary expression is evaluated through its limit, not by treating infinity as an ordinary argument.

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CII.05Show solution

Report a computable estimate and a theorem-based guarantee

With h=1/4h=1/4,

S4=112[1+4cos⁡(1/4)+2cos⁡(1/2)+4cos⁡(3/4)+cos⁡1]≈0.841489383.S_4=\frac1{12}\left[1+4\cos(1/4)+2\cos(1/2)+4\cos(3/4)+\cos1\right] \approx\boxed{0.841489383}.

The fourth derivative of cosine is cosine, so ∣f(4)∣≤1|f^{(4)}|\le1 on [0,1][0,1]. The error bound is

∣I−S4∣≤1180⋅44=146080≈2.171×10−5.\boxed{|I-S_4|\le\frac1{180\cdot4^4}=\frac1{46080}\approx2.171\times10^{-5}}.

The exact integral is sin⁡1\sin1, whose comparison confirms an actual error of about 1.84×10−51.84\times10^{-5}. The numerical comparison is a check; the derivative bound is what supplies the guarantee without already knowing the exact integral.

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CII.06Show solution

First convergence, then evaluation

For an=n2/3na_n=n^2/3^n, the ratio is an+1/an=(n+1)2/(3n2)→1/3<1a_{n+1}/a_n=(n+1)^2/(3n^2)\to1/3<1, so the series converges. For ∣r∣<1|r|<1, the geometric-series identity and legitimate termwise differentiation give

∑n=1∞nrn=r(1−r)2.\sum_{n=1}^{\infty}nr^n=\frac{r}{(1-r)^2}.

Apply r  d/ drr\,\dd/\dd r again:

∑n=1∞n2rn=r(1(1−r)2+2r(1−r)3)=r(1+r)(1−r)3.\sum_{n=1}^{\infty}n^2r^n =r\left(\frac1{(1-r)^2}+\frac{2r}{(1-r)^3}\right) =\frac{r(1+r)}{(1-r)^3}.

At r=1/3r=1/3, the sum is 3/2\boxed{3/2}. The ratio test alone does not produce that value; the power-series identity is a separate argument.

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CII.07Show solution

A valid bound may demand many terms

The positive terms 1/n+11/\sqrt{n+1} decrease to zero, so the alternating series converges. The absolute series diverges by comparison with the pp-series of exponent 1/21/2 (or by an index shift). Thus convergence is conditional. After NN terms, ∣RN∣≤1/N+2|R_N|\le1/\sqrt{N+2}. Requiring this to be at most 0.02=1/500.02=1/50 gives N+2≥2500N+2\ge2500, or N≥2498\boxed{N\ge2498}. This sufficient count shows how slowly this bound improves. A rapidly convergent reformulation, when available, may be preferable for computation.

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CII.08Show solution

The radius does not decide the endpoints

The absolute ratio tends to ∣x−2∣/4|x-2|/4, giving radius R=4\boxed{R=4}. At x=−2x=-2, the series is ∑(−1)n/n\sum(-1)^n/n, which converges conditionally. At x=6x=6, it is harmonic and diverges. Thus the interval is [−2,6)\boxed{[-2,6)}. Inside ∣x−2∣<4|x-2|<4, termwise differentiation gives

∑n=1∞(x−2)n−14n=14∑k=0∞(x−24)k=16−x.\sum_{n=1}^{\infty}\frac{(x-2)^{n-1}}{4^n} =\frac14\sum_{k=0}^{\infty}\left(\frac{x-2}4\right)^k =\boxed{\frac1{6-x}}.

At either endpoint, the derivative-series terms have magnitude 1/41/4 and do not tend to zero. Therefore its interval is (−2,6)(-2,6), even though the original series converges at the left endpoint. An interior derivative identity does not automatically extend termwise to an endpoint.

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CII.09Show solution

Integrate an approximation together with a remainder bound

The polynomial is P5(x)=2x−(2x)3/3!+(2x)5/5!=2x−4x3/3+4x5/15P_5(x)=2x-(2x)^3/3!+(2x)^5/5!=2x-4x^3/3+4x^5/15. The original quotient tends to 22 at zero, so its continuous extension poses no improper singularity. Dividing the polynomial by xx and integrating gives

∫01/5(2−43x2+415x4) dx=[2x−49x3+475x5]01/5=278762703125≈0.3964615111.\int_0^{1/5}\left(2-\frac43x^2+\frac4{15}x^4\right)\dd x =\left[2x-\frac49x^3+\frac4{75}x^5\right]_0^{1/5} =\boxed{\frac{278762}{703125}}\approx0.3964615111.

On 0≤x≤1/50\le x\le1/5, the sine-series term magnitudes decrease; the next omitted term bounds the error by (2x)7/7!(2x)^7/7!. After division by x>0x>0, the quotient error is at most 8x6/3158x^6/315, and the bound extends continuously as zero at x=0x=0. Therefore the integral error is at most

∫01/58x6315 dx=8172265625≈4.644×10−8.\int_0^{1/5}\frac{8x^6}{315}\dd x =\boxed{\frac{8}{172265625}}\approx4.644\times10^{-8}.

The omitted sine term is negative, so this particular polynomial integral is an overestimate. The bound and direction have been justified on the whole integration interval, not only at its endpoint.

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CII.10Show solution

Use parameter speed for length and horizontal motion for area

Differentiate: x′=1−cos⁡tx'=1-\cos t, y′=sin⁡ty'=\sin t. Speed is

(1−cos⁡t)2+sin⁡2t=2−2cos⁡t=2∣sin⁡(t/2)∣.\sqrt{(1-\cos t)^2+\sin^2t} =\sqrt{2-2\cos t}=2|\sin(t/2)|.

On [0,2π][0,2\pi], sin⁡(t/2)≥0\sin(t/2)\ge0, so length is L=∫02π2sin⁡(t/2) dt=[−4cos⁡(t/2)]02π=8L=\int_0^{2\pi}2\sin(t/2)\dd t=[-4\cos(t/2)]_0^{2\pi}=\boxed8. For area, x′≥0x'\ge0 and y≥0y\ge0, so

A=∫y dx=∫02π(1−cos⁡t)2 dt=∫02π(1−2cos⁡t+cos⁡2t) dt=3π.A=\int y\dd x=\int_0^{2\pi}(1-\cos t)^2\dd t =\int_0^{2\pi}(1-2\cos t+\cos^2t)\dd t=\boxed{3\pi}.

The endpoints have zero parameter velocity, but the curve is smooth inside and the speed integral remains valid. Length and area require different differential factors.

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CII.11Show solution

Subtract radial sector areas on the stated angle interval

In the first quadrant 0≤θ≤π/20\le\theta\le\pi/2, the cardioid radius 1+cos⁡θ1+\cos\theta lies between 11 and 22, so the region has 1+cos⁡θ≤r≤21+\cos\theta\le r\le2. Hence

A=12∫0π/2[4−(1+cos⁡θ)2] dθ=12∫0π/2(3−2cos⁡θ−cos⁡2θ) dθ=12(3π2−2−π4)=5π8−1.\begin{align*} A&=\frac12\int_0^{\pi/2}\left[4-(1+\cos\theta)^2\right]\dd\theta\\ &=\frac12\int_0^{\pi/2}(3-2\cos\theta-\cos^2\theta)\dd\theta\\ &=\frac12\left(\frac{3\pi}{2}-2-\frac\pi4\right) =\boxed{\frac{5\pi}{8}-1}. \end{align*}

The answer is positive and less than the first-quadrant disk area π\pi. The area is not one-half the integral of a plain difference of radii.

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CII.12Show solution

Verify both the equation and the initial value

An integrating factor is e2te^{2t}. Multiplication gives (e2ty)′=4e2t(e^{2t}y)'=4e^{2t}, so e2ty=2e2t+Ce^{2t}y=2e^{2t}+C and y=2+Ce−2ty=2+Ce^{-2t}. The initial condition gives C=3C=3: y=2+3e−2t\boxed{y=2+3e^{-2t}}. Then y′=−6e−2ty'=-6e^{-2t} and y′+2y=−6e−2t+4+6e−2t=4y'+2y=-6e^{-2t}+4+6e^{-2t}=4, while y(0)=5y(0)=5. The equilibrium is y=2y=2 and this solution tends toward it from above as t→∞t\to\infty. The differential equation determines a family until an initial condition selects one member.

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Retention and readiness#

A strong Calculus II review includes one unnamed integration problem, one improper-integral condition check, one positive-series test, one alternating or endpoint problem, one approximation with a bound, and one parametric or polar setup. Keep a method-choice entry in your log whenever you could execute a rule but selected it for the wrong structure.