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Integration -- Diagnostic Tests

flowchart TD
A[Diag Integration] --> B[Key Concepts]
A --> C[Core Principles]
A --> D[Practical Applications]
B --> E[Fundamental definitions]
C --> F[Design patterns]
D --> G[Real-world usage]

Mathematics is the language of patterns and logic, a tool for describing relationships and solving problems.

Tests edge cases, boundary conditions, and common misconceptions for integration.

UT-1: Integration by Parts, Choosing uu and dvdx\frac{dv}{dx} Correctly

Section titled “UT-1: Integration by Parts, Choosing uuu and dvdx\frac{dv}{dx}dxdv​ Correctly”

Question:

(a) Find ∫x3ln⁡x dx\int x^3 \ln x\, dx.

(b) A student chooses u=x3u = x^3 and dvdx=ln⁡x\frac{dv}{dx} = \ln x for integration by parts. Explain why this choice is problematic, and show what happens if the student persists with it.

(c) Using your result from part (a), evaluate ∫1ex3ln⁡x dx\int_1^e x^3 \ln x\, dx exactly.

[Difficulty: hard. Tests the LIATE priority rule for integration by parts, and the consequences of choosing the wrong assignment.]

Solution:

(a) By LIATE (Logarithmic, Inverse trig, Algebraic, Trigonometric, Exponential), ln⁡x\ln x is prioritised for uu.

Set u=ln⁡xu = \ln x, dvdx=x3\frac{dv}{dx} = x^3.

du=1x dxdu = \frac{1}{x}\, dx, v=x44v = \frac{x^4}{4}.

∫x3ln⁡x dx=x44ln⁡x−∫x44⋅1x dx\int x^3 \ln x\, dx = \frac{x^4}{4}\ln x - \int \frac{x^4}{4} \cdot \frac{1}{x}\, dx =x44ln⁡x−14∫x3 dx= \frac{x^4}{4}\ln x - \frac{1}{4}\int x^3\, dx =x44ln⁡x−x416+C= \frac{x^4}{4}\ln x - \frac{x^4}{16} + C =x416(4ln⁡x−1)+C= \frac{x^4}{16}(4\ln x - 1) + C

(b) If the student chooses u=x3u = x^3 and dvdx=ln⁡x\frac{dv}{dx} = \ln x:

du=3x2 dxdu = 3x^2\, dx But v=∫ln⁡x dx=xln⁡x−xv = \int \ln x\, dx = x\ln x - x (which itself requires integration by parts to find).

Then:

∫x3ln⁡x dx=x3(xln⁡x−x)−∫3x2(xln⁡x−x) dx\int x^3 \ln x\, dx = x^3(x\ln x - x) - \int 3x^2(x\ln x - x)\, dx =x4ln⁡x−x4−3∫x3ln⁡x dx+3∫x3 dx= x^4\ln x - x^4 - 3\int x^3\ln x\, dx + 3\int x^3\, dx =x4ln⁡x−x4−3∫x3ln⁡x dx+3x44= x^4\ln x - x^4 - 3\int x^3\ln x\, dx + \frac{3x^4}{4}

This produces an equation involving the original integral:

∫x3ln⁡x dx=x4ln⁡x−x44−3∫x3ln⁡x dx\int x^3\ln x\, dx = x^4\ln x - \frac{x^4}{4} - 3\int x^3\ln x\, dx 4∫x3ln⁡x dx=x4ln⁡x−x444\int x^3\ln x\, dx = x^4\ln x - \frac{x^4}{4} ∫x3ln⁡x dx=x44ln⁡x−x416\int x^3\ln x\, dx = \frac{x^4}{4}\ln x - \frac{x^4}{16}

This eventually works but requires more steps and an additional integration by parts just to find vv. The LIATE choice is more efficient.

(c) ∫1ex3ln⁡x dx=[x416(4ln⁡x−1)]1e\int_1^e x^3\ln x\, dx = \left[\frac{x^4}{16}(4\ln x - 1)\right]_1^e

At x=ex = e: e416(4−1)=3e416\frac{e^4}{16}(4 - 1) = \frac{3e^4}{16}

At x=1x = 1: 116(0−1)=−116\frac{1}{16}(0 - 1) = -\frac{1}{16}

=3e416−(−116)=3e4+116= \frac{3e^4}{16} - \left(-\frac{1}{16}\right) = \frac{3e^4 + 1}{16}

UT-2: Forgetting to Change Limits in Definite Integration by Substitution

Section titled “UT-2: Forgetting to Change Limits in Definite Integration by Substitution”

Question:

(a) Evaluate ∫01x1+x2 dx\int_0^1 x\sqrt{1 + x^2}\, dx using the substitution u=1+x2u = 1 + x^2.

(b) A student uses the substitution u=1+x2u = 1 + x^2 but forgets to change the limits. The student computes the indefinite integral, then substitutes x=0x = 0 and x=1x = 1 back into the xx-expression. Show that this approach gives the correct answer, and explain why this works in this particular case.

(c) A second student evaluates ∫0π2xcos⁡x dx\int_0^{\frac{\pi}{2}} x\cos x\, dx by integration by parts and obtains xsin⁡x+cos⁡x+Cx\sin x + \cos x + C. They then write ∫0π2xcos⁡x dx=[π2sin⁡π2+cos⁡π2]−[0+cos⁡0]=π2−1\int_0^{\frac{\pi}{2}} x\cos x\, dx = \left[\frac{\pi}{2}\sin\frac{\pi}{2} + \cos\frac{\pi}{2}\right] - [0 + \cos 0] = \frac{\pi}{2} - 1. A third student forgets to evaluate the lower limit and writes only π2+0=π2\frac{\pi}{2} + 0 = \frac{\pi}{2}. What percentage error does the third student make?

[Difficulty: hard. Tests the boundary between when forgetting to change limits produces errors versus when back-substitution rescues the answer, and lower-limit negligence.]

Solution:

(a) u=1+x2u = 1 + x^2, du=2x dxdu = 2x\, dx So x dx=12 dux\, dx = \frac{1}{2}\, du.

When x=0x = 0: u=1u = 1. When x=1x = 1: u=2u = 2.

∫01x1+x2 dx=∫12u⋅12 du=12∫12u1/2 du\int_0^1 x\sqrt{1+x^2}\, dx = \int_1^2 \sqrt{u} \cdot \frac{1}{2}\, du = \frac{1}{2}\int_1^2 u^{1/2}\, du =12[23u3/2]12=13(23/2−1)=13(22−1)= \frac{1}{2}\left[\frac{2}{3}u^{3/2}\right]_1^2 = \frac{1}{3}(2^{3/2} - 1) = \frac{1}{3}(2\sqrt{2} - 1)

(b) The indefinite integral (back-substituted) is:

13(1+x2)3/2+C\frac{1}{3}(1+x^2)^{3/2} + C

Evaluating from x=0x = 0 to x=1x = 1:

13(23/2)−13(13/2)=22−13\frac{1}{3}(2^{3/2}) - \frac{1}{3}(1^{3/2}) = \frac{2\sqrt{2} - 1}{3}

This gives the same answer as part (a). Back-substitution always works because it restores the original variable, and the Fundamental Theorem of Calculus applies regardless of which variable is used. The error of forgetting limits occurs only when the student evaluates in uu-space with the original xx-limits (e.g., evaluating 13u3/2\frac{1}{3}u^{3/2} from u=0u = 0 to u=1u = 1 Which is wrong).

(c) Correct answer: π2−1≈0.5708\frac{\pi}{2} - 1 \approx 0.5708.

Third student”s answer: π2≈1.5708\frac{\pi}{2} \approx 1.5708.

Percentage error=∣π2−(π2−1)∣∣π2−1∣×100%=1π2−1×100%≈175.2%\text{Percentage error} = \frac{\lvert\frac{\pi}{2} - (\frac{\pi}{2} - 1)\rvert}{\lvert\frac{\pi}{2} - 1\rvert} \times 100\% = \frac{1}{\frac{\pi}{2} - 1} \times 100\% \approx 175.2\%

The third student’s answer is 175.2%175.2\% too large, a catastrophic error from omitting a single term.


UT-3: Absolute Value in ∫1x dx=ln⁡∣x∣\int \frac{1}{x}\, dx = \ln\lvert x \rvert

Section titled “UT-3: Absolute Value in ∫1x dx=ln⁡∣x∣\int \frac{1}{x}\, dx = \ln\lvert x \rvert∫x1​dx=ln∣x∣”

Question:

(a) Evaluate ∫−2−12x dx\int_{-2}^{-1} \frac{2}{x}\, dx.

(b) A student writes ∫−2−12x dx=[2ln⁡x]−2−1\int_{-2}^{-1} \frac{2}{x}\, dx = [2\ln x]_{-2}^{-1} and concludes the integral is undefined. Explain the error and find the correct value.

(c) Evaluate ∫−33xx2+1 dx\int_{-3}^{3} \frac{x}{x^2 + 1}\, dx.

(d) Evaluate ∫−111x dx\int_{-1}^{1} \frac{1}{x}\, dx or show that it does not exist.

[Difficulty: hard. Tests the absolute value in the antiderivative of 1x\frac{1}{x} And the improper integral when the integrand has a singularity within the interval.]

Solution:

(a) ∫−2−12x dx=2∫−2−11x dx=2[ln⁡∣x∣]−2−1=2(ln⁡1−ln⁡2)=−2ln⁡2\int_{-2}^{-1} \frac{2}{x}\, dx = 2\int_{-2}^{-1} \frac{1}{x}\, dx = 2[\ln\lvert x \rvert]_{-2}^{-1} = 2(\ln 1 - \ln 2) = -2\ln 2.

The result is negative because the integrand 2x\frac{2}{x} is negative on [−2,−1][-2, -1] (since x<0x \lt 0).

(b) The student writes ln⁡x\ln x instead of ln⁡∣x∣\ln\lvert x \rvert. Since xx is negative in this interval, ln⁡x\ln x is undefined. The correct antiderivative is ln⁡∣x∣\ln\lvert x \rvert Which is defined for x≠0x \neq 0.

The correct answer is −2ln⁡2-2\ln 2 As computed in part (a).

(c) Note that f(x)=xx2+1f(x) = \frac{x}{x^2+1} is an odd function: f(−x)=−xx2+1=−f(x)f(-x) = \frac{-x}{x^2+1} = -f(x).

Since the integral of an odd function over [−a,a][-a, a] is zero:

∫−33xx2+1 dx=0\int_{-3}^{3} \frac{x}{x^2+1}\, dx = 0

Verification: ∫xx2+1 dx=12ln⁡(x2+1)+C\int \frac{x}{x^2+1}\, dx = \frac{1}{2}\ln(x^2+1) + C. Evaluating from −3-3 to 33:

12(ln⁡10−ln⁡10)=0\frac{1}{2}(\ln 10 - \ln 10) = 0

(d) ∫−111x dx\int_{-1}^{1} \frac{1}{x}\, dx has a singularity at x=0x = 0. We must split:

∫−111x dx=lim⁡a→0−∫−1a1x dx+lim⁡b→0+∫b11x dx\int_{-1}^{1} \frac{1}{x}\, dx = \lim_{a \to 0^-}\int_{-1}^{a}\frac{1}{x}\, dx + \lim_{b \to 0^+}\int_{b}^{1}\frac{1}{x}\, dx =lim⁡a→0−[ln⁡∣x∣]−1a+lim⁡b→0+[ln⁡∣x∣]b1= \lim_{a \to 0^-}[\ln\lvert x \rvert]_{-1}^{a} + \lim_{b \to 0^+}[\ln\lvert x \rvert]_{b}^{1} =lim⁡a→0−(ln⁡∣a∣−ln⁡1)+lim⁡b→0+(ln⁡1−ln⁡∣b∣)= \lim_{a \to 0^-}(\ln\lvert a \rvert - \ln 1) + \lim_{b \to 0^+}(\ln 1 - \ln\lvert b \rvert) =lim⁡a→0−ln⁡∣a∣+lim⁡b→0+(−ln⁡∣b∣)= \lim_{a \to 0^-}\ln\lvert a \rvert + \lim_{b \to 0^+}(-\ln\lvert b \rvert) =−∞+∞= -\infty + \infty

This is an indeterminate form. The integral does not converge; it is an improper integral that diverges. The answer is that ∫−111x dx\int_{-1}^{1} \frac{1}{x}\, dx does not exist.

A student who writes [ln⁡∣x∣]−11=0−0=0[\ln\lvert x \rvert]_{-1}^1 = 0 - 0 = 0 is making a serious error by applying the Fundamental Theorem of Calculus across a singularity.


Tests synthesis of integration with other topics. Requires combining concepts from multiple units.

IT-1: Velocity Vector Integration for Displacement and Distance (with Vectors)

Section titled “IT-1: Velocity Vector Integration for Displacement and Distance (with Vectors)”

Question:

A particle moves in a plane with velocity vector v=(t2−2t)i+2t j\mathbf{v} = (t^2 - 2t)\mathbf{i} + 2t\,\mathbf{j} m/s, where t≥0t \geq 0.

(a) Find the displacement of the particle from t=0t = 0 to t=3t = 3.

(b) Find the total distance travelled by the particle from t=0t = 0 to t=3t = 3.

[Difficulty: hard. Requires integrating a velocity vector component-by-component for displacement, and recognising that distance requires integrating the magnitude of velocity (not the velocity components).]

Solution:

(a) Displacement =∫03v dt= \int_0^3 \mathbf{v}\, dt.

∫03(t2−2t) dt=[t33−t2]03=9−9−0=0\int_0^3 (t^2 - 2t)\, dt = \left[\frac{t^3}{3} - t^2\right]_0^3 = 9 - 9 - 0 = 0 ∫032t dt=[t2]03=9\int_0^3 2t\, dt = [t^2]_0^3 = 9

Displacement =0i+9j=9j= 0\mathbf{i} + 9\mathbf{j} = 9\mathbf{j} metres.

(b) Distance travelled =∫03∣v∣ dt=∫03(t2−2t)2+(2t)2 dt= \int_0^3 \lvert\mathbf{v}\rvert\, dt = \int_0^3 \sqrt{(t^2-2t)^2 + (2t)^2}\, dt

=∫03t4−4t3+4t2+4t2 dt=∫03t4−4t3+8t2 dt= \int_0^3 \sqrt{t^4 - 4t^3 + 4t^2 + 4t^2}\, dt = \int_0^3 \sqrt{t^4 - 4t^3 + 8t^2}\, dt =∫03tt2−4t+8 dt= \int_0^3 t\sqrt{t^2 - 4t + 8}\, dt

Completing the square: t2−4t+8=(t−2)2+4t^2 - 4t + 8 = (t-2)^2 + 4.

Use the substitution u=t2−4t+8u = t^2 - 4t + 8, du=(2t−4) dtdu = (2t - 4)\, dt.

Then t dt=du+4 dt2t\, dt = \frac{du + 4\, dt}{2} Which is not directly useful. Instead, write:

∫03t(t−2)2+4 dt\int_0^3 t\sqrt{(t-2)^2 + 4}\, dt

Let w=t−2w = t - 2 So t=w+2t = w + 2, dt=dwdt = dw. When t=0t = 0: w=−2w = -2. When t=3t = 3: w=1w = 1.

=∫−21(w+2)w2+4 dw=∫−21ww2+4 dw+2∫−21w2+4 dw= \int_{-2}^{1} (w+2)\sqrt{w^2 + 4}\, dw = \int_{-2}^{1} w\sqrt{w^2+4}\, dw + 2\int_{-2}^{1}\sqrt{w^2+4}\, dw

First integral: substitute u=w2+4u = w^2 + 4, du=2w dwdu = 2w\, dw.

∫−21ww2+4 dw=12∫85u du=12[23u3/2]85=13(55−162)\int_{-2}^{1} w\sqrt{w^2+4}\, dw = \frac{1}{2}\int_{8}^{5}\sqrt{u}\, du = \frac{1}{2}\left[\frac{2}{3}u^{3/2}\right]_8^5 = \frac{1}{3}(5\sqrt{5} - 16\sqrt{2})

Second integral: ∫w2+4 dw\int\sqrt{w^2 + 4}\, dw. Using the standard formula ∫w2+a2 dw=w2w2+a2+a22ln⁡(w+w2+a2)+C\int\sqrt{w^2+a^2}\, dw = \frac{w}{2}\sqrt{w^2+a^2} + \frac{a^2}{2}\ln(w+\sqrt{w^2+a^2}) + C with a=2a = 2:

=[w2w2+4+2ln⁡(w+w2+4)]−21= \left[\frac{w}{2}\sqrt{w^2+4} + 2\ln(w + \sqrt{w^2+4})\right]_{-2}^{1}

At w=1w = 1: 125+2ln⁡(1+5)\frac{1}{2}\sqrt{5} + 2\ln(1+\sqrt{5})

At w=−2w = -2: 0+2ln⁡(−2+8)=2ln⁡(22−2)0 + 2\ln(-2+\sqrt{8}) = 2\ln(2\sqrt{2}-2)

2[52+2ln⁡(1+5)−2ln⁡(22−2)]=5+4ln⁡ ⁣(1+522−2)2\left[\frac{\sqrt{5}}{2} + 2\ln(1+\sqrt{5}) - 2\ln(2\sqrt{2}-2)\right] = \sqrt{5} + 4\ln\!\left(\frac{1+\sqrt{5}}{2\sqrt{2}-2}\right)

Total distance =13(55−162)+5+4ln⁡ ⁣(1+522−2)= \frac{1}{3}(5\sqrt{5} - 16\sqrt{2}) + \sqrt{5} + 4\ln\!\left(\frac{1+\sqrt{5}}{2\sqrt{2}-2}\right)

=853−1623+4ln⁡ ⁣(1+522−2)= \frac{8\sqrt{5}}{3} - \frac{16\sqrt{2}}{3} + 4\ln\!\left(\frac{1+\sqrt{5}}{2\sqrt{2}-2}\right)

IT-2: Integrating sin⁡2x\sin^2 x Using the Double Angle Identity (with Trigonometry)

Section titled “IT-2: Integrating sin⁡2x\sin^2 xsin2x Using the Double Angle Identity (with Trigonometry)”

Question:

(a) Find ∫sin⁡2x dx\int \sin^2 x\, dx using the double angle identity.

(b) Hence evaluate ∫0πsin⁡2x dx\int_0^{\pi} \sin^2 x\, dx and interpret the result geometrically.

(c) Evaluate ∫0π4sin⁡2xcos⁡2x dx\int_0^{\frac{\pi}{4}} \sin^2 x\cos^2 x\, dx using appropriate identities.

(d) Given that ∫0π2sin⁡nx dx=n−1n∫0π2sin⁡n−2x dx\int_0^{\frac{\pi}{2}} \sin^n x\, dx = \frac{n-1}{n} \int_0^{\frac{\pi}{2}} \sin^{n-2} x\, dx for n≥2n \geq 2 (Wallis’ reduction formula), find ∫0π2sin⁡6x dx\int_0^{\frac{\pi}{2}} \sin^6 x\, dx.

[Difficulty: hard. Combines trigonometric identities with integration, culminating in the Wallis reduction formula.]

Solution:

(a) Using sin⁡2x=1−cos⁡2x2\sin^2 x = \frac{1 - \cos 2x}{2}:

∫sin⁡2x dx=∫1−cos⁡2x2 dx=12x−14sin⁡2x+C\int \sin^2 x\, dx = \int \frac{1 - \cos 2x}{2}\, dx = \frac{1}{2}x - \frac{1}{4}\sin 2x + C

(b) ∫0πsin⁡2x dx=[12x−14sin⁡2x]0π=π2−0=π2\int_0^{\pi} \sin^2 x\, dx = \left[\frac{1}{2}x - \frac{1}{4}\sin 2x\right]_0^{\pi} = \frac{\pi}{2} - 0 = \frac{\pi}{2}.

Geometrically, this is the area between the curve y=sin⁡2xy = \sin^2 x and the xx-axis from x=0x = 0 to x=πx = \pi. Since sin⁡2x≥0\sin^2 x \geq 0 The area equals the integral. The result π2\frac{\pi}{2} equals the area of a semicircle of radius 1, which is a coincidence related to the fact that sin⁡2x\sin^2 x and cos⁡2x\cos^2 x each average to 12\frac{1}{2} over a full period.

(c) sin⁡2xcos⁡2x=14sin⁡22x=14⋅1−cos⁡4x2=18(1−cos⁡4x)\sin^2 x\cos^2 x = \frac{1}{4}\sin^2 2x = \frac{1}{4} \cdot \frac{1 - \cos 4x}{2} = \frac{1}{8}(1 - \cos 4x).

∫0π4sin⁡2xcos⁡2x dx=∫0π418(1−cos⁡4x) dx=18[x−14sin⁡4x]0π4\int_0^{\frac{\pi}{4}} \sin^2 x\cos^2 x\, dx = \int_0^{\frac{\pi}{4}} \frac{1}{8}(1 - \cos 4x)\, dx = \frac{1}{8}\left[x - \frac{1}{4}\sin 4x\right]_0^{\frac{\pi}{4}} =18(π4−0)=π32= \frac{1}{8}\left(\frac{\pi}{4} - 0\right) = \frac{\pi}{32}

(d) Applying Wallis’ reduction formula repeatedly:

∫0π2sin⁡6x dx=56∫0π2sin⁡4x dx=56⋅34∫0π2sin⁡2x dx=56⋅34⋅12∫0π21 dx\int_0^{\frac{\pi}{2}} \sin^6 x\, dx = \frac{5}{6}\int_0^{\frac{\pi}{2}} \sin^4 x\, dx = \frac{5}{6} \cdot \frac{3}{4}\int_0^{\frac{\pi}{2}} \sin^2 x\, dx = \frac{5}{6} \cdot \frac{3}{4} \cdot \frac{1}{2}\int_0^{\frac{\pi}{2}} 1\, dx =56⋅34⋅12⋅π2=15π96=5π32= \frac{5}{6} \cdot \frac{3}{4} \cdot \frac{1}{2} \cdot \frac{\pi}{2} = \frac{15\pi}{96} = \frac{5\pi}{32}

IT-3: Verifying an Integration Result by Differentiation (with Differentiation)

Section titled “IT-3: Verifying an Integration Result by Differentiation (with Differentiation)”

Question:

A student claims that ∫xx+1 dx=23(x−2)x+1+C\int \frac{x}{\sqrt{x+1}}\, dx = \frac{2}{3}(x-2)\sqrt{x+1} + C.

(a) Verify this result by differentiation.

(b) Find the integral ∫xx+1 dx\int \frac{x}{\sqrt{x+1}}\, dx using the substitution u=x+1u = \sqrt{x+1} And confirm the student’s answer.

(c) Hence evaluate ∫03xx+1 dx\int_0^3 \frac{x}{\sqrt{x+1}}\, dx exactly.

(d) A different student claims ∫1x+1 dx=2x+1+C\int \frac{1}{\sqrt{x+1}}\, dx = 2\sqrt{x+1} + C. Use differentiation to verify, then use this result together with part (b) to find ∫03x+1x+1 dx\int_0^3 \frac{x+1}{\sqrt{x+1}}\, dx without further integration.

[Difficulty: hard. Tests verification by differentiation, substitution technique, and decomposition of integrals using known results.]

Solution:

(a) Let F(x)=23(x−2)x+1=23(x−2)(x+1)1/2F(x) = \frac{2}{3}(x-2)\sqrt{x+1} = \frac{2}{3}(x-2)(x+1)^{1/2}.

By the product rule:

F′(x)=23[(x+1)1/2⋅1+(x−2)⋅12(x+1)−1/2]F'(x) = \frac{2}{3}\left[(x+1)^{1/2} \cdot 1 + (x-2) \cdot \frac{1}{2}(x+1)^{-1/2}\right] =23[(x+1)1/2+x−22(x+1)1/2]= \frac{2}{3}\left[(x+1)^{1/2} + \frac{x-2}{2(x+1)^{1/2}}\right] =23⋅2(x+1)+(x−2)2(x+1)1/2=23⋅3x2(x+1)1/2=x(x+1)1/2=xx+1= \frac{2}{3} \cdot \frac{2(x+1) + (x-2)}{2(x+1)^{1/2}} = \frac{2}{3} \cdot \frac{3x}{2(x+1)^{1/2}} = \frac{x}{(x+1)^{1/2}} = \frac{x}{\sqrt{x+1}}

Confirmed.

(b) u=x+1u = \sqrt{x+1} So u2=x+1u^2 = x + 1 Giving x=u2−1x = u^2 - 1 and dx=2u dudx = 2u\, du.

∫xx+1 dx=∫u2−1u⋅2u du=2∫(u2−1) du\int \frac{x}{\sqrt{x+1}}\, dx = \int \frac{u^2-1}{u} \cdot 2u\, du = 2\int(u^2 - 1)\, du =2(u33−u)+C=2u33−2u+C= 2\left(\frac{u^3}{3} - u\right) + C = \frac{2u^3}{3} - 2u + C

Substituting back u=x+1u = \sqrt{x+1}:

=23(x+1)3/2−2(x+1)1/2+C=23(x+1)1/2[(x+1)−3]+C=23(x−2)x+1+C= \frac{2}{3}(x+1)^{3/2} - 2(x+1)^{1/2} + C = \frac{2}{3}(x+1)^{1/2}[(x+1) - 3] + C = \frac{2}{3}(x-2)\sqrt{x+1} + C

Confirmed.

(c) ∫03xx+1 dx=[23(x−2)x+1]03\int_0^3 \frac{x}{\sqrt{x+1}}\, dx = \left[\frac{2}{3}(x-2)\sqrt{x+1}\right]_0^3

At x=3x = 3: 23(1)(2)=43\frac{2}{3}(1)(2) = \frac{4}{3}

At x=0x = 0: 23(−2)(1)=−43\frac{2}{3}(-2)(1) = -\frac{4}{3}

=43−(−43)=83= \frac{4}{3} - \left(-\frac{4}{3}\right) = \frac{8}{3}

(d) Verification: ddx[2(x+1)1/2]=2⋅12(x+1)−1/2=1x+1\frac{d}{dx}[2(x+1)^{1/2}] = 2 \cdot \frac{1}{2}(x+1)^{-1/2} = \frac{1}{\sqrt{x+1}}. Confirmed.

Decomposition: x+1x+1=x+1=(x+1)1/2\frac{x+1}{\sqrt{x+1}} = \sqrt{x+1} = (x+1)^{1/2}.

So ∫03x+1x+1 dx=∫03(x+1)1/2 dx=[23(x+1)3/2]03=23(8−1)=143\int_0^3 \frac{x+1}{\sqrt{x+1}}\, dx = \int_0^3 (x+1)^{1/2}\, dx = \left[\frac{2}{3}(x+1)^{3/2}\right]_0^3 = \frac{2}{3}(8 - 1) = \frac{14}{3}.

Alternatively, using linearity: ∫03x+1x+1 dx=∫03xx+1 dx+∫031x+1 dx=83+[2x+1]03=83+2(2−1)=83+2=143\int_0^3 \frac{x+1}{\sqrt{x+1}}\, dx = \int_0^3 \frac{x}{\sqrt{x+1}}\, dx + \int_0^3 \frac{1}{\sqrt{x+1}}\, dx = \frac{8}{3} + [2\sqrt{x+1}]_0^3 = \frac{8}{3} + 2(2-1) = \frac{8}{3} + 2 = \frac{14}{3}. Confirmed.

Forgetting the absolute value in ∫1x dx=ln⁡∣x∣+C\int \frac{1}{x}\,dx = \ln|x| + C: The antiderivative of 1x\frac{1}{x} is ln⁡∣x∣\ln|x|, not ln⁡x\ln x. Writing ln⁡x\ln x is only valid for x>0x > 0. When integrating over an interval that includes negative values (e.g., ∫−2−1\int_{-2}^{-1}), you must use ln⁡∣x∣\ln|x| to get the correct result.

Applying the Fundamental Theorem of Calculus across a singularity: If the integrand has a discontinuity within the interval of integration (e.g., 1x\frac{1}{x} at x=0x = 0), you must split the integral and treat it as a limit. Writing [ln⁡∣x∣]−11=0[\ln|x|]_{-1}^{1} = 0 is incorrect because the integral diverges at x=0x = 0.

Confusing displacement with distance travelled: Displacement is ∫v dt\int \mathbf{v}\,dt (can be positive or negative). Distance is ∫∣v∣ dt\int |\mathbf{v}|\,dt (always positive). Students often compute displacement when the question asks for distance, or vice versa. When the velocity changes sign, you must split the integral at the point where v=0v = 0.