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Chapter 4

Basic Mathematics

TU BIT past exam questions

Past questions and answers

76 questions set from this chapter, 1 of them more than once. Most repeated first.

  • Asked 2 times
  • 2077 · 10 marks
  • 2080 · 5 marks

Find the Taylor series of f(x)=1xf(x)=\frac{1}{x} at a=2a=2. Where, if anywhere, does the series converge to 1x\frac{1}{x}?

Answer

Taylor series of f(x)=1/xf(x)=1/x at a=2a=2

The Taylor series is ∑n=0∞f(n)(2)n!(x−2)n\displaystyle\sum_{n=0}^\infty \frac{f^{(n)}(2)}{n!}(x-2)^n.

Derivatives:

f(x)=x−1, f′(x)=−x−2, f′′(x)=2x−3, f′′′(x)=−6x−4, …f(x)=x^{-1},\ f'(x)=-x^{-2},\ f''(x)=2x^{-3},\ f'''(x)=-6x^{-4},\ \dots

f(n)(x)=(−1)n n!xn+1 ⇒ f(n)(2)=(−1)nn!2n+1f^{(n)}(x)=\frac{(-1)^n\,n!}{x^{n+1}}\ \Rightarrow\ f^{(n)}(2)=\frac{(-1)^n n!}{2^{n+1}}

Therefore

f(n)(2)n!=(−1)n2n+1\frac{f^{(n)}(2)}{n!}=\frac{(-1)^n}{2^{n+1}}

1x=∑n=0∞(−1)n2n+1(x−2)n=12−x−24+(x−2)28−(x−2)316+⋯\frac1x=\sum_{n=0}^{\infty}\frac{(-1)^n}{2^{n+1}}(x-2)^n=\frac12-\frac{x-2}{4}+\frac{(x-2)^2}{8}-\frac{(x-2)^3}{16}+\cdots

Convergence

This is a geometric series. To check this, write

1x=12+(x−2)=12⋅11+x−22=12∑n=0∞(−x−22)n\frac1x=\frac{1}{2+(x-2)}=\frac{1}{2}\cdot\frac{1}{1+\frac{x-2}{2}}=\frac12\sum_{n=0}^\infty\left(-\frac{x-2}{2}\right)^n

with common ratio r=−x−22r=-\dfrac{x-2}{2}. It converges when ∣r∣<1|r|<1, that is

∣x−2∣<2  ⟺  0<x<4|x-2|<2\iff 0<x<4

For xx in (0,4)(0,4) the series converges to 1/x1/x (the sum of the geometric series is 12⋅11+(x−2)/2=1x\frac12\cdot\frac{1}{1+(x-2)/2}=\frac1x). At the end points x=0x=0 and x=4x=4 the series diverges (the terms do not tend to 0). So the radius of convergence is 2, and the series represents 1/x1/x exactly on (0,4)(0,4).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 5 marks

Solve the initial value problem dydx+2y=3\frac{dy}{dx}+2y=3, y(0)=1y(0)=1.

Similar questions: What is an initial value problem? (2081)

Answer

Solve dydx+2y=3\dfrac{dy}{dx}+2y=3, y(0)=1y(0)=1.

This is a first-order linear equation y′+Py=Qy'+P y=Q with P=2P=2, Q=3Q=3.

Integrating factor

μ(x)=e∫2 dx=e2x\mu(x)=e^{\int2\,dx}=e^{2x}

Multiplying through:

ddx(e2xy)=3e2x\frac{d}{dx}\left(e^{2x}y\right)=3e^{2x}

e2xy=32e2x+C ⇒ y=32+Ce−2xe^{2x}y=\frac32e^{2x}+C\ \Rightarrow\ y=\frac32+Ce^{-2x}

Initial condition

y(0)=1y(0)=1:  1=32+C⇒C=−12\ 1=\frac32+C\Rightarrow C=-\frac12.

y=32−12e−2x=3−e−2x2y=\frac32-\frac12e^{-2x}=\frac{3-e^{-2x}}{2}

Check: y′=e−2xy'=e^{-2x} and 2y=3−e−2x2y=3-e^{-2x}, so y′+2y=3y'+2y=3, and y(0)=(3−1)/2=1y(0)=(3-1)/2=1.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 1+4 marks

State the Mean Value Theorem and verify it for f(x)=x2+2x−1f(x)=x^2+2x-1 on [0,1][0,1].

Similar questions: Verify the Mean Value Theorem for (2081)

Answer

Mean Value Theorem. If ff is continuous on [a,b][a,b] and differentiable on (a,b)(a,b), there exists c∈(a,b)c\in(a,b) such that

f′(c)=f(b)−f(a)b−af'(c)=\frac{f(b)-f(a)}{b-a}

Verification. f(x)=x2+2x−1f(x)=x^2+2x-1 is a polynomial, hence continuous on [0,1][0,1] and differentiable on (0,1)(0,1).

f(0)=−1f(0)=-1, f(1)=1+2−1=2f(1)=1+2-1=2, so f(1)−f(0)1−0=3\dfrac{f(1)-f(0)}{1-0}=3.

f′(x)=2x+2f'(x)=2x+2. Setting 2c+2=32c+2=3 gives c=12∈(0,1)c=\tfrac12\in(0,1).

So the theorem is verified with c=12c=\tfrac12.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Draw the graph of f(x)=x2+4f(x)=x^2+4 and find its domain and range.

Similar questions: Sketch the graph of $f(x)=\sqrt{x}$. Also (2081.2)

Answer

f(x)=x2+4f(x)=x^2+4 is the parabola y=x2y=x^2 shifted 44 units upward.

Graph. It has vertex (0,4)(0,4) and axis of symmetry x=0x=0, and opens upward. Some points are (±1,5)(\pm1,5), (±2,8)(\pm2,8) and (±3,13)(\pm3,13). It crosses the y-axis at (0,4)(0,4) and never meets the x-axis, since x2+4>0x^2+4>0.

Domain: (−∞,∞)(-\infty,\infty), since any real xx can be squared.

Range: x2≥0x^2\ge0, so f(x)≥4f(x)\ge4 and every value ≥4\ge4 is attained. The range is [4,∞)[4,\infty).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 1+4+5 marks

What is an initial value problem? Solve xdydx−y=x2x\dfrac{dy}{dx}-y=x^2, with y(2)=5y(2)=5. Evaluate lim⁡x→∞3x2−5x+25x2+8x+7\lim_{x\to\infty}\dfrac{3x^2-5x+2}{5x^2+8x+7}.

Similar questions: Solve the initial value problem $\frac{dy}{dx}+2y=3$, (2077)

Answer

Initial value problem. A differential equation together with one or more conditions on the unknown function at a given point (such as y(x0)=y0y(x_0)=y_0), used to pick out a single particular solution from the general solution.

Solution. Rewrite xdydx−y=x2x\frac{dy}{dx}-y=x^2 as

dydx−1xy=x\frac{dy}{dx}-\frac1xy=x

The integrating factor is e−ln⁡x=1xe^{-\ln x}=\frac1x, so

ddx(yx)=1 ⇒ yx=x+C ⇒ y=x2+Cx\frac{d}{dx}\left(\frac yx\right)=1\ \Rightarrow\ \frac yx=x+C\ \Rightarrow\ y=x^2+Cx

From y(2)=5y(2)=5: 4+2C=54+2C=5, so C=12C=\frac12.

y=x2+x2y=x^2+\frac x2

Limit. Divide numerator and denominator by x2x^2:

lim⁡x→∞3x2−5x+25x2+8x+7=lim⁡x→∞3−5/x+2/x25+8/x+7/x2=35\lim_{x\to\infty}\frac{3x^2-5x+2}{5x^2+8x+7}=\lim_{x\to\infty}\frac{3-5/x+2/x^2}{5+8/x+7/x^2}=\frac35

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Verify the Mean Value Theorem for f(x)=x2+3x+1f(x)=x^2+3x+1 on [−1,1][-1,1].

Similar questions: State the Mean Value Theorem and (2078)

Answer

Statement. If ff is continuous on [a,b][a,b] and differentiable on (a,b)(a,b), there is c∈(a,b)c\in(a,b) with f′(c)=f(b)−f(a)b−af'(c)=\dfrac{f(b)-f(a)}{b-a}.

Verification. f(x)=x2+3x+1f(x)=x^2+3x+1 is a polynomial, so it is continuous on [−1,1][-1,1] and differentiable on (−1,1)(-1,1).

f(1)=5,f(−1)=1−3+1=−1,f(1)−f(−1)1−(−1)=62=3f(1)=5,\quad f(-1)=1-3+1=-1,\quad \frac{f(1)-f(-1)}{1-(-1)}=\frac{6}{2}=3

f′(x)=2x+3f'(x)=2x+3. Setting 2c+3=32c+3=3 gives c=0c=0, and 0∈(−1,1)0\in(-1,1). So the Mean Value Theorem is verified, with c=0c=0.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Sketch the graph of f(x)=xf(x)=\sqrt{x}. Also find its domain and range.

Similar questions: Draw the graph of $f(x)=x^2+4$ and (2081)

Answer

Graph: f(x)=xf(x)=\sqrt{x} is the upper half of the parabola y2=xy^2=x. It starts at the origin and rises slowly, curving to the right (increasing and concave down).

Key points:

xx0149
yy0123

Plot these points and join them with a smooth curve starting at (0,0)(0,0) with a vertical tangent, lying entirely in the first quadrant.

Domain: the square root needs x≥0x\ge0, so the domain is [0,∞)[0,\infty).

Range: x≥0\sqrt{x}\ge 0 and takes every non-negative value, so the range is [0,∞)[0,\infty).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 6+4 marks

(a) Define even and odd functions, give an example of each, and state their symmetry. (b) Find the domain and range of f(x)=5x+10f(x)=\sqrt{5x+10} and f(x)=x2−3x−4x+1f(x)=\frac{x^2-3x-4}{x+1}.

Answer

(a) Even and odd functions

  • Even function: f(−x)=f(x)f(-x)=f(x) for every xx in the domain. Its graph is symmetric about the yy-axis. Example: f(x)=x2f(x)=x^2, since f(−x)=(−x)2=x2=f(x)f(-x)=(-x)^2=x^2=f(x).
  • Odd function: f(−x)=−f(x)f(-x)=-f(x) for every xx in the domain. Its graph is symmetric about the origin (rotating by 180∘180^\circ leaves it unchanged). Example: f(x)=x3f(x)=x^3, since f(−x)=−x3=−f(x)f(-x)=-x^3=-f(x).

(b) Domain and range

  1. f(x)=5x+10f(x)=\sqrt{5x+10}

    Need 5x+10≥0⇒x≥−25x+10\ge0\Rightarrow x\ge-2.

    Domain: [−2,∞)[-2,\infty). As xx goes from −2-2 upwards, 5x+105x+10 takes all values in [0,∞)[0,\infty), so Range: [0,∞)[0,\infty).

  2. f(x)=x2−3x−4x+1f(x)=\dfrac{x^2-3x-4}{x+1}

    The denominator is zero at x=−1x=-1, so domain: all real xx with x≠−1x\ne-1, i.e. (−∞,−1)∪(−1,∞)(-\infty,-1)\cup(-1,\infty).

    Factorising: x2−3x−4=(x−4)(x+1)x^2-3x-4=(x-4)(x+1), so f(x)=x−4f(x)=x-4 for x≠−1x\neq-1. This is a line with a hole at x=−1x=-1, where the value would be −1−4=−5-1-4=-5.

    Range: all real numbers except −5-5, i.e. (−∞,−5)∪(−5,∞)(-\infty,-5)\cup(-5,\infty).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 5+5 marks

(a) Sketch f(x)=x2f(x)=x^2, shifted vertically by +1+1 and −2-2, and horizontally by +3+3 and −2-2. (b) Algebraically find δ\delta for lim⁡x→5x−1\lim_{x\to5}\sqrt{x-1} with L=2L=2, ϵ=1\epsilon=1, and for lim⁡x→2(2x−2)\lim_{x\to2}(2x-2) with L=6L=6, ϵ=0.02\epsilon=0.02.

Answer

(a) Shifts of f(x)=x2f(x)=x^2

The base graph is a parabola with vertex at the origin, opening upwards, symmetric about the yy-axis.

  • Vertical shift +1+1: y=x2+1y=x^2+1. The graph moves up 1 unit; vertex (0,1)(0,1).
  • Vertical shift −2-2: y=x2−2y=x^2-2. The graph moves down 2 units; vertex (0,−2)(0,-2).
  • Horizontal shift +3+3: y=(x−3)2y=(x-3)^2. The graph moves right 3 units; vertex (3,0)(3,0).
  • Horizontal shift −2-2: y=(x+2)2y=(x+2)^2. The graph moves left 2 units; vertex (−2,0)(-2,0).

In every case the shape is unchanged. In the sketch, draw all five parabolas on the same axes, each with the vertex listed above and opening upwards.

(b) Finding δ\delta

(i) lim⁡x→5x−1=2\lim_{x\to5}\sqrt{x-1}=2, with ϵ=1\epsilon=1.

We need ∣x−1−2∣<1|\sqrt{x-1}-2|<1:

1<x−1<3  ⟺  1<x−1<9  ⟺  2<x<101<\sqrt{x-1}<3\iff 1<x-1<9\iff 2<x<10

The distance from x0=5x_0=5 to the ends of the interval is 5−2=35-2=3 on the left and 10−5=510-5=5 on the right. Take the smaller:

δ=3\delta=3

So 0<∣x−5∣<30<|x-5|<3 guarantees ∣x−1−2∣<1|\sqrt{x-1}-2|<1.

(ii) f(x)=2x−2f(x)=2x-2, ϵ=0.02\epsilon=0.02. With L=6L=6 the limit point is x0=4x_0=4, because 2(4)−2=62(4)-2=6 (at x0=2x_0=2 the value of 2x−22x-2 is 2).

For L=6L=6:

∣2x−2−6∣<0.02  ⟺  2∣x−4∣<0.02  ⟺  ∣x−4∣<0.01|2x-2-6|<0.02\iff 2|x-4|<0.02\iff |x-4|<0.01

so δ=0.01\delta=0.01.

For the limit at x=2x=2 (where L=2L=2):

∣2x−2−2∣=2∣x−2∣<0.02  ⟺  ∣x−2∣<0.01|2x-2-2|=2|x-2|<0.02\iff |x-2|<0.01

so again δ=0.01\delta=0.01. In both cases δ=ϵ/2\delta=\epsilon/2.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 5 marks

Determine whether ∑n=1∞n2e−n\sum_{n=1}^{\infty} n^2e^{-n} converges or diverges.

Answer

Test ∑n=1∞n2e−n\displaystyle\sum_{n=1}^\infty n^2e^{-n}.

Ratio test. Let an=n2e−n=n2ena_n=n^2e^{-n}=\dfrac{n^2}{e^n}. Then

an+1an=(n+1)2e−(n+1)n2e−n=(n+1n)2⋅1e\frac{a_{n+1}}{a_n}=\frac{(n+1)^2e^{-(n+1)}}{n^2e^{-n}}=\left(\frac{n+1}{n}\right)^2\cdot\frac1e

lim⁡n→∞an+1an=1⋅1e=1e<1\lim_{n\to\infty}\frac{a_{n+1}}{a_n}=1\cdot\frac1e=\frac1e<1

Since the limit 1/e≈0.368<11/e\approx0.368<1, the series converges (absolutely, as all terms are positive).

Alternative check with the integral test: ∫1∞x2e−xdx=[−e−x(x2+2x+2)]1∞=5e−1\int_1^\infty x^2e^{-x}dx=\left[-e^{-x}(x^2+2x+2)\right]_1^\infty=5e^{-1}, which is finite, and x2e−xx^2e^{-x} is positive and decreasing for x≥2x\ge2, which also shows convergence.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 5 marks

Show that f(x)=x2+x−6x2−4f(x)=\frac{x^2+x-6}{x^2-4}, xeq2x eq2, has a continuous extension to x=2x=2.

Answer

f(x)=x2+x−6x2−4f(x)=\dfrac{x^2+x-6}{x^2-4}, x≠2x\ne2 (the function is also undefined at x=−2x=-2).

Factorise

x2+x−6=(x+3)(x−2),x2−4=(x−2)(x+2)x^2+x-6=(x+3)(x-2),\qquad x^2-4=(x-2)(x+2)

For x≠2x\ne2 (and x≠−2x\neq-2):

f(x)=(x+3)(x−2)(x−2)(x+2)=x+3x+2f(x)=\frac{(x+3)(x-2)}{(x-2)(x+2)}=\frac{x+3}{x+2}

Limit at x=2x=2

lim⁡x→2f(x)=lim⁡x→2x+3x+2=54\lim_{x\to2}f(x)=\lim_{x\to2}\frac{x+3}{x+2}=\frac{5}{4}

The limit exists and is finite. Hence ff can be given the value 5/45/4 at x=2x=2 and become continuous there. The continuous extension is

F(x)=x+3x+2,F(2)=54F(x)=\frac{x+3}{x+2},\qquad F(2)=\frac54

This agrees with ff for x≠2x\ne2 and is continuous at x=2x=2, since lim⁡x→2F(x)=F(2)\lim_{x\to2}F(x)=F(2).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 2.5+2.5 marks

Evaluate: (a) lim⁡x→∞(x−x2+16)\lim_{x\to\infty}\left(x-\sqrt{x^2+16}\right); (b) lim⁡x→16x+10−5x2\lim_{x\to1}\frac{\sqrt{6x+10}-5}{x^2}.

Answer

(a) lim⁡x→∞(x−x2+16)\displaystyle\lim_{x\to\infty}\left(x-\sqrt{x^2+16}\right)

This has the form ∞−∞\infty-\infty. Multiply and divide by the conjugate:

x−x2+16=(x−x2+16)(x+x2+16)x+x2+16=x2−(x2+16)x+x2+16=−16x+x2+16x-\sqrt{x^2+16}=\frac{(x-\sqrt{x^2+16})(x+\sqrt{x^2+16})}{x+\sqrt{x^2+16}}=\frac{x^2-(x^2+16)}{x+\sqrt{x^2+16}}=\frac{-16}{x+\sqrt{x^2+16}}

As x→∞x\to\infty the denominator tends to ∞\infty, so

lim⁡x→∞(x−x2+16)=0\lim_{x\to\infty}\left(x-\sqrt{x^2+16}\right)=0

(b) lim⁡x→16x+10−5x2\displaystyle\lim_{x\to1}\frac{\sqrt{6x+10}-5}{x^2}

The function is continuous at x=1x=1 and the denominator is not zero there, so substitute directly:

6+10−51=4−51=−1\frac{\sqrt{6+10}-5}{1}=\frac{4-5}{1}=-1

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 5 marks

Find the derivative of f(x,y)=x3−xy2+x2y−y3f(x,y)=x^3-xy^2+x^2y-y^3 at p0(5,5)p_0(5,5) in the direction of u⃗=4i⃗+3j⃗\vec{u}=4\vec{i}+3\vec{j}.

Answer

f(x,y)=x3−xy2+x2y−y3f(x,y)=x^3-xy^2+x^2y-y^3, p0=(5,5)p_0=(5,5), u⃗=4i⃗+3j⃗\vec u=4\vec i+3\vec j.

Gradient

fx=3x2−y2+2xy,fy=−2xy+x2−3y2f_x=3x^2-y^2+2xy,\qquad f_y=-2xy+x^2-3y^2

At (5,5)(5,5):

fx=75−25+50=100,fy=−50+25−75=−100f_x=75-25+50=100,\qquad f_y=-50+25-75=-100

∇f(5,5)=100i⃗−100j⃗\nabla f(5,5)=100\vec i-100\vec j

Unit vector

∣u⃗∣=16+9=5,u^=45i⃗+35j⃗|\vec u|=\sqrt{16+9}=5,\qquad \hat u=\frac45\vec i+\frac35\vec j

Directional derivative

Du^f=∇f⋅u^=100⋅45−100⋅35=80−60=20D_{\hat u}f=\nabla f\cdot\hat u=100\cdot\frac45-100\cdot\frac35=80-60=20

So the derivative of ff at (5,5)(5,5) in the direction of u⃗\vec u is 2020.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 5 marks

Integrate ∫0π/4dx1−sin⁡x\int_{0}^{\pi/4}\frac{dx}{1-\sin x}.

Answer

I=∫0π/4dx1−sin⁡xI=\int_0^{\pi/4}\frac{dx}{1-\sin x}

Multiply numerator and denominator by 1+sin⁡x1+\sin x:

11−sin⁡x⋅1+sin⁡x1+sin⁡x=1+sin⁡x1−sin⁡2x=1+sin⁡xcos⁡2x=sec⁡2x+sec⁡xtan⁡x\frac{1}{1-\sin x}\cdot\frac{1+\sin x}{1+\sin x}=\frac{1+\sin x}{1-\sin^2x}=\frac{1+\sin x}{\cos^2x}=\sec^2x+\sec x\tan x

Integrate:

I=[tan⁡x+sec⁡x]0π/4I=\Big[\tan x+\sec x\Big]_0^{\pi/4}

At π/4\pi/4: tan⁡=1\tan=1, sec⁡=2\sec=\sqrt2, giving 1+21+\sqrt2.

At 00: tan⁡0+sec⁡0=0+1=1\tan0+\sec0=0+1=1.

I=(1+2)−1=2I=(1+\sqrt2)-1=\sqrt2

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 5 marks

Find the area of the surface generated by revolving y=2xy=2\sqrt{x}, 1≤x≤21\le x\le2, about the x-axis.

Answer

Surface area of revolution about the xx-axis:

S=∫ab2πy1+(dydx)2 dxS=\int_a^b2\pi y\sqrt{1+\left(\frac{dy}{dx}\right)^2}\,dx

For y=2xy=2\sqrt x: dydx=1x\dfrac{dy}{dx}=\dfrac{1}{\sqrt x}, so

1+1x=x+1x\sqrt{1+\frac1x}=\sqrt{\frac{x+1}{x}}

y1+y′2=2x⋅x+1x=2x+1y\sqrt{1+y'^2}=2\sqrt x\cdot\frac{\sqrt{x+1}}{\sqrt x}=2\sqrt{x+1}

S=∫122π⋅2x+1 dx=4π∫12(x+1)1/2dx=4π⋅23[(x+1)3/2]12S=\int_1^2 2\pi\cdot2\sqrt{x+1}\,dx=4\pi\int_1^2(x+1)^{1/2}dx=4\pi\cdot\frac23\Big[(x+1)^{3/2}\Big]_1^2

S=8π3(33/2−23/2)=8π3(33−22)≈19.84 square unitsS=\frac{8\pi}{3}\left(3^{3/2}-2^{3/2}\right)=\frac{8\pi}{3}\left(3\sqrt3-2\sqrt2\right)\approx19.84\text{ square units}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 5 marks

Determine the concavity and find the inflection point(s) of f(x)=x3−3x2+2f(x)=x^3-3x^2+2.

Answer

f(x)=x3−3x2+2f(x)=x^3-3x^2+2

Derivatives

f′(x)=3x2−6x,f′′(x)=6x−6=6(x−1)f'(x)=3x^2-6x,\qquad f''(x)=6x-6=6(x-1)

Concavity

f′′(x)=0f''(x)=0 at x=1x=1.

  • For x<1x<1: f′′(x)<0f''(x)<0, so the graph is concave down on (−∞,1)(-\infty,1).
  • For x>1x>1: f′′(x)>0f''(x)>0, so the graph is concave up on (1,∞)(1,\infty).

Inflection point

The concavity changes at x=1x=1, and

f(1)=1−3+2=0f(1)=1-3+2=0

So the inflection point is (1,0)(1,0).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2077 · 5 marks

Find dydx\frac{dy}{dx} for y=2u3y=2u^3, u=8x−1u=8x-1, and for y=sin⁡uy=\sin u, u=x−xcos⁡xu=x-x\cos x.

Answer

Use the chain rule: dydx=dydu⋅dudx\dfrac{dy}{dx}=\dfrac{dy}{du}\cdot\dfrac{du}{dx}.

(i) y=2u3y=2u^3, u=8x−1u=8x-1

dydu=6u2,dudx=8\frac{dy}{du}=6u^2,\qquad \frac{du}{dx}=8

dydx=6u2⋅8=48u2=48(8x−1)2\frac{dy}{dx}=6u^2\cdot8=48u^2=48(8x-1)^2

(ii) y=sin⁡uy=\sin u, u=x−xcos⁡xu=x-x\cos x

dydu=cos⁡u,dudx=1−(cos⁡x−xsin⁡x)=1−cos⁡x+xsin⁡x\frac{dy}{du}=\cos u,\qquad \frac{du}{dx}=1-\left(\cos x-x\sin x\right)=1-\cos x+x\sin x

dydx=cos⁡(x−xcos⁡x)(1−cos⁡x+xsin⁡x)\frac{dy}{dx}=\cos\left(x-x\cos x\right)\left(1-\cos x+x\sin x\right)

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 4+5+1 marks

Define asymptotes and name their types. Find the vertical and horizontal asymptotes of f(x)=−8x2−4f(x)=\dfrac{-8}{x^2-4}, and state whether any other asymptotes exist.

Answer

Definition. An asymptote of a curve is a line to which the curve comes arbitrarily close as the point on the curve moves to infinity (or approaches a point where the function becomes unbounded).

Types:

  1. Vertical asymptote: x=ax=a where f(x)→±∞f(x)\to\pm\infty as x→ax\to a.
  2. Horizontal asymptote: y=Ly=L where f(x)→Lf(x)\to L as x→±∞x\to\pm\infty.
  3. Oblique (slant) asymptote: y=mx+cy=mx+c with f(x)−(mx+c)→0f(x)-(mx+c)\to0 as x→±∞x\to\pm\infty.

For f(x)=−8x2−4f(x)=\dfrac{-8}{x^2-4}:

Vertical: the denominator x2−4=(x−2)(x+2)x^2-4=(x-2)(x+2) is zero at x=±2x=\pm2 while the numerator is −8≠0-8\ne0. Hence lim⁡x→±2∣f(x)∣=∞\lim_{x\to\pm2}|f(x)|=\infty, and the vertical asymptotes are x=2x=2 and x=−2x=-2.

Horizontal: lim⁡x→±∞−8x2−4=0\displaystyle\lim_{x\to\pm\infty}\frac{-8}{x^2-4}=0, so y=0y=0 (the x-axis) is the horizontal asymptote.

Other: the degree of the numerator (0) is less than the degree of the denominator (2), so there is no oblique asymptote. The vertical and horizontal ones are the only asymptotes.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 1+3+6 marks

Define the area between two curves and find the area enclosed by y=2−x2y=2-x^2 and y=−xy=-x. Define a volume integral and find the volume generated by revolving the region bounded by y2=xy^2=x, y=1y=1, and x=4x=4 about y=1y=1.

Answer

Area between two curves. If f(x)≥g(x)f(x)\ge g(x) on [a,b][a,b], the area enclosed is A=∫ab[f(x)−g(x)]dxA=\int_a^b\bigl[f(x)-g(x)\bigr]dx.

Area between y=2−x2y=2-x^2 and y=−xy=-x. Intersection: 2−x2=−x⇒x2−x−2=0⇒(x−2)(x+1)=02-x^2=-x\Rightarrow x^2-x-2=0\Rightarrow(x-2)(x+1)=0, so x=−1, 2x=-1,\,2. On (−1,2)(-1,2) the parabola is above the line.

A=∫−12(2−x2+x) dx=[2x−x33+x22]−12A=\int_{-1}^{2}(2-x^2+x)\,dx=\left[2x-\frac{x^3}{3}+\frac{x^2}{2}\right]_{-1}^{2}

At x=2x=2: 4−83+2=1034-\tfrac83+2=\tfrac{10}{3}. At x=−1x=-1: −2+13+12=−76-2+\tfrac13+\tfrac12=-\tfrac76.

A=103+76=276=92 square unitsA=\frac{10}{3}+\frac76=\frac{27}{6}=\frac92\ \text{square units}

Volume integral. The volume of a solid is the integral of its cross-sectional area A(x)A(x) over the interval: V=∫abA(x) dxV=\int_a^bA(x)\,dx. For a solid of revolution this is V=∫πR2 dxV=\int\pi R^2\,dx (disc/washer) or V=∫2πr h dyV=\int2\pi r\,h\,dy (shell).

Volume. The region is bounded by y2=xy^2=x (that is y=xy=\sqrt x), y=1y=1 and x=4x=4, so 1≤x≤41\le x\le4 and 1≤y≤x1\le y\le\sqrt x. Revolve about the line y=1y=1. The radius of a disc at xx is x−1\sqrt x-1:

V=π∫14(x−1)2dx=π∫14(x−2x+1) dx=π[x22−43x3/2+x]14V=\pi\int_1^4(\sqrt x-1)^2dx=\pi\int_1^4(x-2\sqrt x+1)\,dx=\pi\left[\frac{x^2}{2}-\frac43x^{3/2}+x\right]_1^4

At x=4x=4: 8−323+4=438-\tfrac{32}{3}+4=\tfrac43. At x=1x=1: 12−43+1=16\tfrac12-\tfrac43+1=\tfrac16.

V=π(43−16)=7π6 cubic unitsV=\pi\left(\frac43-\frac16\right)=\frac{7\pi}{6}\ \text{cubic units}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 2+8 marks

Define the Newton-Raphson method and give its formula. A square tin sheet of side 12 inches has congruent squares cut from its corners, and the sides are bent up to form an open-top box. Find the size of the corner squares that maximizes the box's volume.

Answer

Newton-Raphson method. It is an iterative method for finding a root of f(x)=0f(x)=0. Starting from an initial guess x0x_0, the tangent to the curve at (xn,f(xn))(x_n,f(x_n)) is drawn and the point where it cuts the x-axis is taken as the next approximation:

xn+1=xn−f(xn)f′(xn),f′(xn)≠0x_{n+1}=x_n-\frac{f(x_n)}{f'(x_n)},\qquad f'(x_n)\ne0

Box problem. Let each cut-out square have side xx inches. The box has base (12−2x)×(12−2x)(12-2x)\times(12-2x) and height xx, with 0<x<60<x<6:

V=x(12−2x)2=4x3−48x2+144xV=x(12-2x)^2=4x^3-48x^2+144x

V′=12x2−96x+144=12(x2−8x+12)=12(x−2)(x−6)V'=12x^2-96x+144=12(x^2-8x+12)=12(x-2)(x-6)

Critical points x=2x=2 and x=6x=6; x=6x=6 is an end point (volume 0). Second derivative: V′′=24x−96V''=24x-96, and V′′(2)=−48<0V''(2)=-48<0, so x=2x=2 gives a maximum.

The corner squares should be 2 inches by 2 inches, giving a maximum volume V=2(8)2=128V=2(8)^2=128 cubic inches.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 5 marks

Graph y=−x3y=-x^3 and y=x2y=x^2. State their symmetry and the intervals where each is increasing or decreasing.

Answer

y=−x3y=-x^3

  • Symmetry: f(−x)=x3=−f(x)f(-x)=x^3=-f(x), so it is an odd function, symmetric about the origin.
  • y′=−3x2≤0y'=-3x^2\le0, so it is decreasing on (−∞,∞)(-\infty,\infty) (never increasing), passing through the origin with a horizontal tangent there. The graph falls from the upper left to the lower right (concave up for x<0x<0, concave down for x>0x>0).

y=x2y=x^2

  • Symmetry: f(−x)=f(x)f(-x)=f(x), an even function, symmetric about the yy-axis.
  • y′=2xy'=2x: decreasing on (−∞,0)(-\infty,0) and increasing on (0,∞)(0,\infty). It is a parabola opening upwards with its vertex (minimum) at the origin.

The two curves intersect where −x3=x2-x^3=x^2, i.e. at x=0x=0 and x=−1x=-1, at (0,0)(0,0) and (−1,1)(-1,1).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 5 marks

Find the equations of the tangent and normal to x3+y3−9xy=0x^3+y^3-9xy=0 at (2,4)(2,4).

Answer

The point (2,4)(2,4) lies on the curve: 8+64−72=08+64-72=0.

Differentiate x3+y3−9xy=0x^3+y^3-9xy=0 implicitly:

3x2+3y2y′−9y−9xy′=0 ⇒ y′=3y−x2y2−3x3x^2+3y^2y'-9y-9xy'=0\ \Rightarrow\ y'=\frac{3y-x^2}{y^2-3x}

At (2,4)(2,4): y′=12−416−6=810=45y'=\dfrac{12-4}{16-6}=\dfrac{8}{10}=\dfrac45.

Tangent: y−4=45(x−2)y-4=\tfrac45(x-2), that is

4x−5y+12=04x-5y+12=0

Normal (slope −54-\tfrac54): y−4=−54(x−2)y-4=-\tfrac54(x-2), that is

5x+4y=265x+4y=26

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 1+4 marks

State L'Hopital's rule and use it to evaluate lim⁡x→0(sec⁡x)1/x2\lim_{x\to 0}(\sec x)^{1/x^2} and lim⁡x→0x−sin⁡xx3\lim_{x\to 0}\dfrac{x-\sin x}{x^3}.

Answer

L'Hopital's rule. If lim⁡f(x)/g(x)\lim f(x)/g(x) is of the form 00\frac00 or ∞∞\frac\infty\infty at x=ax=a, and f,gf,g are differentiable near aa, then lim⁡x→af(x)g(x)=lim⁡x→af′(x)g′(x)\displaystyle\lim_{x\to a}\frac{f(x)}{g(x)}=\lim_{x\to a}\frac{f'(x)}{g'(x)}, provided the latter limit exists.

(i) L=lim⁡x→0(sec⁡x)1/x2L=\lim_{x\to0}(\sec x)^{1/x^2} has form 1∞1^\infty. Take logs:

ln⁡L=lim⁡x→0ln⁡sec⁡xx2 (00)=lim⁡x→0tan⁡x2x (00)=lim⁡x→0sec⁡2x2=12\ln L=\lim_{x\to0}\frac{\ln\sec x}{x^2}\ \left(\tfrac00\right)=\lim_{x\to0}\frac{\tan x}{2x}\ \left(\tfrac00\right)=\lim_{x\to0}\frac{\sec^2x}{2}=\frac12

L=e1/2=eL=e^{1/2}=\sqrt e

(ii)

lim⁡x→0x−sin⁡xx3=lim⁡1−cos⁡x3x2=lim⁡sin⁡x6x=16\lim_{x\to0}\frac{x-\sin x}{x^3}=\lim\frac{1-\cos x}{3x^2}=\lim\frac{\sin x}{6x}=\frac16

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 1+4 marks

Define integration and evaluate ∫dx(x−1)(x−2)\displaystyle\int \frac{dx}{(x-1)(x-2)} and ∫−113x2x3+1 dx\displaystyle\int_{-1}^{1} 3x^2\sqrt{x^3+1}\,dx.

Answer

Integration is the reverse of differentiation: ∫f(x) dx=F(x)+C\int f(x)\,dx=F(x)+C where F′(x)=f(x)F'(x)=f(x). The definite integral ∫abf(x)dx\int_a^bf(x)dx gives the (signed) area under the curve.

(i) Partial fractions:

1(x−1)(x−2)=1x−2−1x−1\frac{1}{(x-1)(x-2)}=\frac{1}{x-2}-\frac{1}{x-1}

∫dx(x−1)(x−2)=ln⁡∣x−2∣−ln⁡∣x−1∣+C=ln⁡∣x−2x−1∣+C\int\frac{dx}{(x-1)(x-2)}=\ln|x-2|-\ln|x-1|+C=\ln\left|\frac{x-2}{x-1}\right|+C

(ii) Let u=x3+1u=x^3+1, du=3x2dxdu=3x^2dx. When x=−1x=-1, u=0u=0; when x=1x=1, u=2u=2.

∫−113x2x3+1 dx=∫02u1/2du=23u3/2∣02=23⋅22=423\int_{-1}^{1}3x^2\sqrt{x^3+1}\,dx=\int_0^2u^{1/2}du=\frac23u^{3/2}\Big|_0^2=\frac23\cdot2\sqrt2=\frac{4\sqrt2}{3}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 1+4 marks

Define the integral test and determine whether ∑n=1∞1n2+4\displaystyle\sum_{n=1}^{\infty}\frac{1}{n^2+4} converges or diverges.

Answer

Integral test. Let ff be positive, continuous and decreasing on [N,∞)[N,\infty) with an=f(n)a_n=f(n). Then ∑n=N∞an\sum_{n=N}^\infty a_n and ∫N∞f(x) dx\int_N^\infty f(x)\,dx either both converge or both diverge.

Application. f(x)=1x2+4f(x)=\dfrac{1}{x^2+4} is positive, continuous and decreasing for x≥1x\ge1.

∫1∞dxx2+4=lim⁡b→∞12tan⁡−1x2∣1b=12(π2−tan⁡−112)≈0.5268\int_1^\infty\frac{dx}{x^2+4}=\lim_{b\to\infty}\frac12\tan^{-1}\frac x2\Big|_1^b=\frac12\left(\frac\pi2-\tan^{-1}\frac12\right)\approx0.5268

The integral is finite, so the series ∑n=1∞1n2+4\displaystyle\sum_{n=1}^\infty\frac1{n^2+4} converges.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 5 marks

Solve xdydx=x2+3yx\dfrac{dy}{dx}=x^2+3y for x>0x>0.

Answer

Write in standard linear form (for x>0x>0):

dydx−3xy=x\frac{dy}{dx}-\frac3xy=x

Integrating factor: e∫−3/x dx=e−3ln⁡x=x−3e^{\int-3/x\,dx}=e^{-3\ln x}=x^{-3}.

ddx(x−3y)=x−3⋅x=x−2\frac{d}{dx}\left(x^{-3}y\right)=x^{-3}\cdot x=x^{-2}

x−3y=−1x+Cx^{-3}y=-\frac1x+C

y=−x2+Cx3y=-x^2+Cx^3

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 5 marks

Find the directional derivative of f(x,y,z)=x3−xy2−zf(x,y,z)=x^3-xy^2-z at P(1,1,0)P(1,1,0) in the direction of v=2i−3j+6kv=2\mathbf{i}-3\mathbf{j}+6\mathbf{k}.

Answer

f=x3−xy2−zf=x^3-xy^2-z:

∇f=(3x2−y2, −2xy, −1)\nabla f=(3x^2-y^2,\ -2xy,\ -1)

At P(1,1,0)P(1,1,0): ∇f=(2,−2,−1)\nabla f=(2,-2,-1).

∣v∣=4+9+36=7|v|=\sqrt{4+9+36}=7, so the unit vector is u^=17(2,−3,6)\hat u=\tfrac17(2,-3,6).

Du^f=∇f⋅u^=2(2)+(−2)(−3)+(−1)(6)7=4+6−67=47D_{\hat u}f=\nabla f\cdot\hat u=\frac{2(2)+(-2)(-3)+(-1)(6)}{7}=\frac{4+6-6}{7}=\frac47

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2078 · 2.5+2.5 marks

Find dydx\dfrac{dy}{dx} if y2−x2=sin⁡xy^2-x^2=\sin x. Find the slope of the circle x2+y2=25x^2+y^2=25 at (3,4)(3,4).

Answer

(a) Differentiate y2−x2=sin⁡xy^2-x^2=\sin x implicitly:

2ydydx−2x=cos⁡x ⇒ dydx=2x+cos⁡x2y2y\frac{dy}{dx}-2x=\cos x\ \Rightarrow\ \frac{dy}{dx}=\frac{2x+\cos x}{2y}

(b) For x2+y2=25x^2+y^2=25: 2x+2y y′=02x+2y\,y'=0, so y′=−xyy'=-\dfrac xy. At (3,4)(3,4):

slope=−34\text{slope}=-\frac34

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 5+5 marks

Evaluate the piecewise function f(x)f(x) at x=−3,−1,0x=-3, -1, 0 and sketch its graph. Define the types of discontinuity, then find the points of continuity of f(x)=x−2x2−7x+10f(x)=\frac{x-2}{x^2-7x+10}.

Answer

Piecewise function. To evaluate a piecewise function at a point, identify which interval contains the point and use the formula of that piece only. So f(−3)f(-3), f(−1)f(-1) and f(0)f(0) are each computed from the rule whose domain includes −3-3, −1-1 and 00 respectively. For the graph, plot each piece over its own interval, using a filled dot where an end point is included and an open dot where it is excluded.

Types of discontinuity.

  1. Removable: lim⁡x→af(x)\lim_{x\to a}f(x) exists but f(a)f(a) is undefined or differs from the limit.
  2. Jump: the left and right limits exist but are unequal.
  3. Infinite: f(x)→±∞f(x)\to\pm\infty near aa (vertical asymptote).
  4. Oscillating: the function oscillates and has no limit.

Continuity of f(x)=x−2x2−7x+10f(x)=\dfrac{x-2}{x^2-7x+10}. Factor: x2−7x+10=(x−2)(x−5)x^2-7x+10=(x-2)(x-5).

ff is a rational function, so it is continuous at every point where the denominator is non-zero, that is, for all x≠2, 5x\ne2,\,5.

  • At x=2x=2: f(x)=1x−5→−13f(x)=\dfrac{1}{x-5}\to-\dfrac13, a finite limit, so this is a removable discontinuity.
  • At x=5x=5: f(x)→±∞f(x)\to\pm\infty, an infinite discontinuity.

Hence ff is continuous on (−∞,2)∪(2,5)∪(5,∞)(-\infty,2)\cup(2,5)\cup(5,\infty).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 5+2+3 marks

Define the gradient vector and the directional derivative. For f(x,y)=x22+y22f(x,y)=\frac{x^2}{2}+\frac{y^2}{2} at (1,1)(1,1), find the directions of fastest increase and decrease and the direction of zero change. Find the directional derivative along v=3i−4jv=3i-4j.

Answer

Gradient vector. For f(x,y)f(x,y), ∇f=(∂f∂x,∂f∂y)\nabla f=\left(\dfrac{\partial f}{\partial x},\dfrac{\partial f}{\partial y}\right). It points in the direction of the greatest rate of increase of ff, and its magnitude is that rate.

Directional derivative. The rate of change of ff at a point in the direction of a unit vector u^\hat u: Du^f=∇f⋅u^D_{\hat u}f=\nabla f\cdot\hat u.

For f=x22+y22f=\dfrac{x^2}2+\dfrac{y^2}2: ∇f=(x,y)\nabla f=(x,y), so at (1,1)(1,1), ∇f=(1,1)\nabla f=(1,1), ∣∇f∣=2|\nabla f|=\sqrt2.

  • Fastest increase: direction (1,1)2\dfrac{(1,1)}{\sqrt2}, with rate 2\sqrt2.
  • Fastest decrease: direction −(1,1)2-\dfrac{(1,1)}{\sqrt2}, with rate −2-\sqrt2.
  • Zero change: directions perpendicular to the gradient, ±(1,−1)2\pm\dfrac{(1,-1)}{\sqrt2} (along the level curve).

Along v=3i−4jv=3\mathbf i-4\mathbf j: ∣v∣=5|v|=5, u^=(35,−45)\hat u=\left(\tfrac35,-\tfrac45\right).

Du^f=1⋅35+1⋅(−45)=−15D_{\hat u}f=1\cdot\frac35+1\cdot\left(-\frac45\right)=-\frac15

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 2+3+3+2 marks

Define concavity. For f(x)=x4−4x3+10f(x)=x^4-4x^3+10, find the intervals of increase and decrease, the intervals of concavity, and any local maxima or minima.

Answer

Concavity. A graph is concave up on an interval if f′f' is increasing there (f′′>0f''>0), so the curve lies above its tangents; it is concave down if f′f' is decreasing (f′′<0f''<0).

f(x)=x4−4x3+10f(x)=x^4-4x^3+10

f′(x)=4x3−12x2=4x2(x−3)f'(x)=4x^3-12x^2=4x^2(x-3)

Critical points: x=0x=0 and x=3x=3.

  • f′<0f'<0 for x<0x<0 and for 0<x<30<x<3: decreasing on (−∞,3)(-\infty,3).
  • f′>0f'>0 for x>3x>3: increasing on (3,∞)(3,\infty).

f′′(x)=12x2−24x=12x(x−2)f''(x)=12x^2-24x=12x(x-2)

  • f′′>0f''>0 for x<0x<0 and x>2x>2: concave up on (−∞,0)∪(2,∞)(-\infty,0)\cup(2,\infty).
  • f′′<0f''<0 for 0<x<20<x<2: concave down on (0,2)(0,2).

Extrema. At x=3x=3, f′f' changes from negative to positive: a local minimum with f(3)=81−108+10=−17f(3)=81-108+10=-17. At x=0x=0, f′f' does not change sign, so there is no extremum. There is no local maximum.

The inflection points are (0,10)(0,10) and (2,−6)(2,-6).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 2+3 marks

Find the domain and range of f(x)=5x+10f(x)=\sqrt{5x+10}. Sketch y=x2y=x^2 after the specified shifts.

Answer

Domain and range. We need 5x+10≥05x+10\ge 0, so x≥−2x\ge -2.

Domain=[−2,∞)\text{Domain}=[-2,\infty)

The square root takes every value from 00 upward (it is 00 at x=−2x=-2 and increases without bound), so

Range=[0,∞)\text{Range}=[0,\infty)

Shifts of y=x2y=x^2. The graph of y=x2y=x^2 is a parabola with vertex (0,0)(0,0) opening upward.

  • y=(x−h)2y=(x-h)^2 shifts it hh units right (left if h<0h<0).
  • y=x2+ky=x^2+k shifts it kk units up (down if k<0k<0).
  • y=(x−h)2+ky=(x-h)^2+k is the parabola with vertex (h,k)(h,k) and the same shape.

For example, y=(x−2)2+3y=(x-2)^2+3 is y=x2y=x^2 moved 2 units right and 3 units up, with vertex (2,3)(2,3) and axis x=2x=2. It crosses the y-axis at (0,7)(0,7) and never touches the x-axis.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 2+3 marks

Define horizontal and vertical asymptotes. Find the asymptotes of f(x)=x−x2+16f(x)=x-\sqrt{x^2+16}.

Answer

Definitions. The line y=Ly=L is a horizontal asymptote of y=f(x)y=f(x) if lim⁡x→∞f(x)=L\lim_{x\to\infty}f(x)=L or lim⁡x→−∞f(x)=L\lim_{x\to-\infty}f(x)=L. The line x=ax=a is a vertical asymptote if f(x)→±∞f(x)\to\pm\infty as x→a+x\to a^{+} or x→a−x\to a^{-}.

Asymptotes of f(x)=x−x2+16f(x)=x-\sqrt{x^2+16}.

Vertical: x2+16>0x^2+16>0 for all xx, so ff is defined and continuous everywhere. There is no vertical asymptote.

Horizontal, x→∞x\to\infty: multiply by the conjugate.

f(x)=x2−(x2+16)x+x2+16=−16x+x2+16→0f(x)=\frac{x^2-(x^2+16)}{x+\sqrt{x^2+16}}=\frac{-16}{x+\sqrt{x^2+16}}\to 0

So y=0y=0 is a horizontal asymptote.

As x→−∞x\to-\infty: x2+16=∣x∣1+16/x2≈−x\sqrt{x^2+16}=|x|\sqrt{1+16/x^2}\approx -x, so f(x)≈2x→−∞f(x)\approx 2x\to-\infty. There is no horizontal asymptote on this side. In fact f(x)−2x→0f(x)-2x\to 0, so y=2xy=2x is a slant asymptote there.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 5 marks

Find the area between the x-axis and f(x)=x3−x2−2xf(x)=x^3-x^2-2x for 1≤x≤21\le x\le 2.

Answer

Factor: f(x)=x(x−2)(x+1)f(x)=x(x-2)(x+1). On 1≤x≤21\le x\le 2 we have x>0x>0, x−2≤0x-2\le0, x+1>0x+1>0, so f(x)≤0f(x)\le 0. The graph lies below the x-axis, so the area is −∫12f(x) dx-\int_1^2 f(x)\,dx.

∫12(x3−x2−2x) dx=[x44−x33−x2]12\int_1^2 (x^3-x^2-2x)\,dx=\left[\frac{x^4}{4}-\frac{x^3}{3}-x^2\right]_1^2

At x=2x=2: 4−83−4=−834-\tfrac83-4=-\tfrac83. At x=1x=1: 14−13−1=−1312\tfrac14-\tfrac13-1=-\tfrac{13}{12}.

∫12f dx=−83+1312=−1912\int_1^2 f\,dx=-\frac83+\frac{13}{12}=-\frac{19}{12}

Area=1912 square units\text{Area}=\frac{19}{12}\text{ square units}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 1+4 marks

Define arc length. Find the length of y=(x2)2/3y=\left(\frac{x}{2}\right)^{2/3} from x=0x=0 to x=2x=2.

Answer

Arc length. The length of the curve y=f(x)y=f(x) from x=ax=a to x=bx=b is the limit of the total length of inscribed line segments, given by

L=∫ab1+(dydx)2 dxL=\int_a^b\sqrt{1+\left(\frac{dy}{dx}\right)^2}\,dx

Solution. The curve is y=(x/2)2/3y=(x/2)^{2/3}, i.e. x=2y3/2x=2y^{3/2}. At x=0x=0, y=0y=0; at x=2x=2, y=1y=1. Since dy/dxdy/dx is unbounded at x=0x=0, integrate with respect to yy.

dxdy=3y1/2,L=∫011+9y dy=227[(1+9y)3/2]01\frac{dx}{dy}=3y^{1/2},\qquad L=\int_0^1\sqrt{1+9y}\,dy=\frac{2}{27}\Big[(1+9y)^{3/2}\Big]_0^1

L=227(1010−1)≈2.268L=\frac{2}{27}\left(10\sqrt{10}-1\right)\approx 2.268

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 5 marks

Evaluate ∫0π/41+cos⁡x dx\int_0^{\pi/4}\sqrt{1+\cos x}\,dx and ∫3x2−7x+13x dx\int \frac{3x^2-7x+1}{3x}\,dx.

Answer

First integral. Use 1+cos⁡x=2cos⁡2(x/2)1+\cos x=2\cos^2(x/2), so 1+cos⁡x=2cos⁡(x/2)\sqrt{1+\cos x}=\sqrt2\cos(x/2) for 0≤x≤π/40\le x\le\pi/4.

∫0π/41+cos⁡x dx=2[2sin⁡x2]0π/4=22 sin⁡π8≈1.082\int_0^{\pi/4}\sqrt{1+\cos x}\,dx=\sqrt2\Big[2\sin\tfrac{x}{2}\Big]_0^{\pi/4}=2\sqrt2\,\sin\frac{\pi}{8}\approx 1.082

Second integral. Divide term by term:

∫3x2−7x+13x dx=∫(x−73+13x)dx=x22−7x3+13ln⁡∣x∣+C\int\frac{3x^2-7x+1}{3x}\,dx=\int\left(x-\frac73+\frac{1}{3x}\right)dx=\frac{x^2}{2}-\frac{7x}{3}+\frac13\ln|x|+C

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 1+4 marks

Define a first-order linear differential equation. Solve tdydt+2y=t3t\frac{dy}{dt}+2y=t^3, t>0t>0, y(2)=1y(2)=1.

Answer

Definition. A first-order linear differential equation is one that can be written as

dydx+P(x) y=Q(x)\frac{dy}{dx}+P(x)\,y=Q(x)

where yy and y′y' appear only to the first power and are not multiplied together.

Solution. For t>0t>0, divide by tt:

dydt+2ty=t2\frac{dy}{dt}+\frac{2}{t}y=t^2

The integrating factor is e∫2/t dt=t2e^{\int 2/t\,dt}=t^2. Then

ddt(t2y)=t4 ⇒ t2y=t55+C\frac{d}{dt}(t^2y)=t^4\ \Rightarrow\ t^2y=\frac{t^5}{5}+C

Using y(2)=1y(2)=1: 4=325+C4=\frac{32}{5}+C, so C=−125C=-\frac{12}{5}.

y=t35−125t2y=\frac{t^3}{5}-\frac{12}{5t^2}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 5 marks

Determine whether ∑n=1∞55n−1\sum_{n=1}^{\infty}\frac{5}{5n-1} and ∑n=0∞1n!\sum_{n=0}^{\infty}\frac{1}{n!} converge or diverge.

Answer

(a) ∑n=1∞55n−1\sum_{n=1}^\infty \frac{5}{5n-1} diverges. For n≥1n\ge1, 55n−1>55n=1n\frac{5}{5n-1}>\frac{5}{5n}=\frac1n. The harmonic series ∑1n\sum\frac1n diverges, so by direct comparison this series diverges. (The limit comparison test with 1n\frac1n gives limit 11, with the same conclusion.)

(b) ∑n=0∞1n!\sum_{n=0}^\infty \frac1{n!} converges. By the ratio test,

lim⁡n→∞1/(n+1)!1/n!=lim⁡n→∞1n+1=0<1\lim_{n\to\infty}\frac{1/(n+1)!}{1/n!}=\lim_{n\to\infty}\frac{1}{n+1}=0<1

so the series converges (its sum is ee).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 1+4 marks

State the chain rule for w=f(x,y)w=f(x,y). For w=xyw=xy with x=cos⁡tx=\cos t, y=sin⁡ty=\sin t, find dwdt\frac{dw}{dt} and its value at t=π2t=\frac{\pi}{2}.

Answer

Chain rule. If w=f(x,y)w=f(x,y) has continuous partial derivatives and x=x(t)x=x(t), y=y(t)y=y(t) are differentiable, then

dwdt=∂w∂xdxdt+∂w∂ydydt\frac{dw}{dt}=\frac{\partial w}{\partial x}\frac{dx}{dt}+\frac{\partial w}{\partial y}\frac{dy}{dt}

Example. For w=xyw=xy: wx=yw_x=y, wy=xw_y=x. With x=cos⁡tx=\cos t, y=sin⁡ty=\sin t, we have dxdt=−sin⁡t\frac{dx}{dt}=-\sin t and dydt=cos⁡t\frac{dy}{dt}=\cos t.

dwdt=sin⁡t(−sin⁡t)+cos⁡t(cos⁡t)=cos⁡2t−sin⁡2t=cos⁡2t\frac{dw}{dt}=\sin t(-\sin t)+\cos t(\cos t)=\cos^2 t-\sin^2 t=\cos 2t

At t=π2t=\frac{\pi}{2}: cos⁡π=−1\cos\pi=-1.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2079 · 5 marks

Find dydx\frac{dy}{dx} for y2−x2=cos⁡(xy)y^2-x^2=\cos(xy) and for x2=9y2x^2=\frac{9}{y^2}.

Answer

(a) Differentiate y2−x2=cos⁡(xy)y^2-x^2=\cos(xy) with respect to xx:

2yy′−2x=−sin⁡(xy) (y+xy′)2yy'-2x=-\sin(xy)\,(y+xy')

y′(2y+xsin⁡(xy))=2x−ysin⁡(xy)y'\big(2y+x\sin(xy)\big)=2x-y\sin(xy)

dydx=2x−ysin⁡(xy)2y+xsin⁡(xy)\frac{dy}{dx}=\frac{2x-y\sin(xy)}{2y+x\sin(xy)}

(b) Write x2y2=9x^2y^2=9 and differentiate:

2xy2+2x2y y′=0 ⇒ dydx=−yx2xy^2+2x^2y\,y'=0\ \Rightarrow\ \frac{dy}{dx}=-\frac{y}{x}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5+5 marks

(a) Define the gradient of a scalar function f(x,y,z)f(x,y,z). Find the derivative of f=x3−xy2+zf=x^3-xy^2+z at P(1,0,0)P(1,0,0) in the direction of v⃗=2i⃗−j⃗+k⃗\vec{v}=2\vec{i}-\vec{j}+\vec{k}. (b) Define the volume of a solid. Find the volume generated by revolving the region bounded by y=xy=\sqrt{x}, y=1y=1, and x=4x=4 about the line y=1y=1.

Answer

(a) Gradient. For a scalar function f(x,y,z)f(x,y,z),

∇f=∂f∂xi⃗+∂f∂yj⃗+∂f∂zk⃗\nabla f=\frac{\partial f}{\partial x}\vec i+\frac{\partial f}{\partial y}\vec j+\frac{\partial f}{\partial z}\vec k

It points in the direction of greatest increase of ff, and the directional derivative along a unit vector u⃗\vec u is ∇f⋅u⃗\nabla f\cdot\vec u.

For f=x3−xy2+zf=x^3-xy^2+z: ∇f=(3x2−y2, −2xy, 1)\nabla f=(3x^2-y^2,\,-2xy,\,1), so ∇f(1,0,0)=(3,0,1)\nabla f(1,0,0)=(3,0,1).

∣v⃗∣=4+1+1=6,Du⃗f=(3,0,1)⋅(2,−1,1)6=76≈2.86|\vec v|=\sqrt{4+1+1}=\sqrt6,\qquad D_{\vec u}f=\frac{(3,0,1)\cdot(2,-1,1)}{\sqrt6}=\frac{7}{\sqrt6}\approx 2.86

(b) Volume. The volume of a solid is the integral of its cross-sectional area A(x)A(x) over the interval: V=∫abA(x) dxV=\int_a^bA(x)\,dx. For a solid of revolution, each cross-section is a disc or washer.

The curves y=xy=\sqrt x and y=1y=1 meet at x=1x=1. The region is bounded by x=4x=4, so 1≤x≤41\le x\le4. Rotating about y=1y=1, each disc has radius x−1\sqrt x-1.

V=π∫14(x−1)2dx=π∫14(x−2x+1) dx=π[x22−43x3/2+x]14V=\pi\int_1^4(\sqrt x-1)^2dx=\pi\int_1^4(x-2\sqrt x+1)\,dx=\pi\left[\frac{x^2}{2}-\frac43x^{3/2}+x\right]_1^4

At x=4x=4: 8−323+4=438-\frac{32}{3}+4=\frac43. At x=1x=1: 12−43+1=16\frac12-\frac43+1=\frac16.

V=π(43−16)=7π6 cubic unitsV=\pi\left(\frac43-\frac16\right)=\frac{7\pi}{6}\text{ cubic units}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5+5 marks

Evaluate ∫0π/4dx1−sin⁡x\int_0^{\pi/4}\frac{dx}{1-\sin x} and ∫x2sin⁡x dx\int x^2\sin x\,dx. Solve dydx−3yx=x\frac{dy}{dx}-\frac{3y}{x}=x, x>0x>0.

Answer

(a) Multiply the numerator and denominator by 1+sin⁡x1+\sin x:

11−sin⁡x=1+sin⁡xcos⁡2x=sec⁡2x+sec⁡xtan⁡x\frac{1}{1-\sin x}=\frac{1+\sin x}{\cos^2x}=\sec^2x+\sec x\tan x

∫0π/4dx1−sin⁡x=[tan⁡x+sec⁡x]0π/4=(1+2)−(0+1)=2\int_0^{\pi/4}\frac{dx}{1-\sin x}=\Big[\tan x+\sec x\Big]_0^{\pi/4}=(1+\sqrt2)-(0+1)=\sqrt2

(b) Integrate by parts twice for ∫x2sin⁡x dx\int x^2\sin x\,dx:

∫x2sin⁡x dx=−x2cos⁡x+2∫xcos⁡x dx=−x2cos⁡x+2xsin⁡x+2cos⁡x+C\int x^2\sin x\,dx=-x^2\cos x+2\int x\cos x\,dx=-x^2\cos x+2x\sin x+2\cos x+C

(c) The equation dydx−3xy=x\frac{dy}{dx}-\frac3x y=x is linear with integrating factor e−3ln⁡x=x−3e^{-3\ln x}=x^{-3}.

ddx(x−3y)=x−2 ⇒ x−3y=−1x+C\frac{d}{dx}\left(x^{-3}y\right)=x^{-2}\ \Rightarrow\ x^{-3}y=-\frac1x+C

y=−x2+Cx3y=-x^2+Cx^3

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5+5 marks

State Rolle's Theorem and show that x3+3x+1=0x^3+3x+1=0 has exactly one real solution. Find the area enclosed by y=2−x2y=2-x^2 and y=−xy=-x.

Answer

Rolle's Theorem. If ff is continuous on [a,b][a,b], differentiable on (a,b)(a,b) and f(a)=f(b)f(a)=f(b), then there is at least one c∈(a,b)c\in(a,b) with f′(c)=0f'(c)=0.

Exactly one real root of x3+3x+1=0x^3+3x+1=0.

Existence: f(x)=x3+3x+1f(x)=x^3+3x+1 is continuous, with f(−1)=−3<0f(-1)=-3<0 and f(0)=1>0f(0)=1>0. By the Intermediate Value Theorem there is a root in (−1,0)(-1,0).

Uniqueness: Suppose there were two roots a<ba<b. Then f(a)=f(b)=0f(a)=f(b)=0, and Rolle's Theorem would give cc with f′(c)=0f'(c)=0. But f′(x)=3x2+3≥3>0f'(x)=3x^2+3\ge3>0 for all xx, a contradiction. Hence there is exactly one real root.

Area. Setting 2−x2=−x2-x^2=-x gives x2−x−2=0x^2-x-2=0, so x=−1x=-1 or x=2x=2. On [−1,2][-1,2] the parabola y=2−x2y=2-x^2 lies above the line y=−xy=-x.

A=∫−12(2−x2+x) dx=[2x−x33+x22]−12=103−(−76)=92A=\int_{-1}^{2}(2-x^2+x)\,dx=\left[2x-\frac{x^3}{3}+\frac{x^2}{2}\right]_{-1}^{2}=\frac{10}{3}-\left(-\frac76\right)=\frac92

The area is 92\frac92 square units.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5 marks

Define the absolute value function and sketch its graph.

Answer

Definition. The absolute value function is

∣x∣={x,x≥0−x,x<0|x|=\begin{cases}x,&x\ge0\\-x,&x<0\end{cases}

It gives the distance of xx from 00, so ∣x∣=x2≥0|x|=\sqrt{x^2}\ge0.

Graph. It is the line y=xy=x for x≥0x\ge0 and the line y=−xy=-x for x<0x<0. Together these form a "V" shape with its vertex at the origin (0,0)(0,0). The graph is symmetric about the y-axis (so ∣x∣|x| is an even function), passing through points such as (±1,1)(\pm1,1) and (±2,2)(\pm2,2).

  • Domain: R\mathbb R
  • Range: [0,∞)[0,\infty)
  • It is continuous everywhere but not differentiable at x=0x=0, where there is a sharp corner.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5 marks

Find lim⁡h→∞6h+25−5h2\lim_{h\to\infty}\frac{\sqrt{6h+25}-5}{h^2}.

Answer

For large hh the numerator behaves like 6h\sqrt{6h}, which grows far more slowly than h2h^2. To show this rigorously, rationalise:

6h+25−5h2=6hh2(6h+25+5)=6h(6h+25+5)\frac{\sqrt{6h+25}-5}{h^2}=\frac{6h}{h^2\left(\sqrt{6h+25}+5\right)}=\frac{6}{h\left(\sqrt{6h+25}+5\right)}

As h→∞h\to\infty the denominator tends to ∞\infty, so

lim⁡h→∞6h+25−5h2=0\lim_{h\to\infty}\frac{\sqrt{6h+25}-5}{h^2}=0

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5 marks

State the integral test and use it to test the convergence of ∑n=1∞1n2+1\sum_{n=1}^{\infty}\frac{1}{n^2+1}.

Answer

Integral test. Let an=f(n)a_n=f(n) where ff is positive, continuous and decreasing on [N,∞)[N,\infty). Then ∑n=N∞an\sum_{n=N}^\infty a_n and ∫N∞f(x) dx\int_N^\infty f(x)\,dx either both converge or both diverge.

Application. Take f(x)=1x2+1f(x)=\frac{1}{x^2+1}. It is positive, continuous and decreasing for x≥1x\ge1.

∫1∞dxx2+1=lim⁡b→∞[tan⁡−1x]1b=π2−π4=π4\int_1^\infty\frac{dx}{x^2+1}=\lim_{b\to\infty}\Big[\tan^{-1}x\Big]_1^b=\frac\pi2-\frac\pi4=\frac\pi4

The integral is finite, so ∑n=1∞1n2+1\sum_{n=1}^\infty\frac{1}{n^2+1} converges.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5 marks

Define implicit differentiation and find the slope of x2+y2=25x^2+y^2=25 at (3,−4)(3,-4).

Answer

Implicit differentiation. When yy is defined implicitly by an equation in xx and yy, we differentiate both sides with respect to xx, treating yy as a function of xx (so ddxyn=nyn−1dydx\frac{d}{dx}y^n=ny^{n-1}\frac{dy}{dx}), and then solve for dydx\frac{dy}{dx}. This avoids having to solve for yy explicitly.

For x2+y2=25x^2+y^2=25:

2x+2ydydx=0 ⇒ dydx=−xy2x+2y\frac{dy}{dx}=0\ \Rightarrow\ \frac{dy}{dx}=-\frac xy

At (3,−4)(3,-4):

slope=−3−4=34\text{slope}=-\frac{3}{-4}=\frac34

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5 marks

Define a partial derivative and find ∂f∂x\frac{\partial f}{\partial x} and ∂f∂y\frac{\partial f}{\partial y} at (4,−5)(4,-5) for f(x,y)=x3+3xy+y−1f(x,y)=x^3+3xy+y-1.

Answer

Definition. The partial derivative of f(x,y)f(x,y) with respect to xx is the derivative found by treating yy as a constant:

∂f∂x=lim⁡h→0f(x+h,y)−f(x,y)h\frac{\partial f}{\partial x}=\lim_{h\to0}\frac{f(x+h,y)-f(x,y)}{h}

and similarly for ∂f∂y\frac{\partial f}{\partial y} with xx held constant.

For f(x,y)=x3+3xy+y−1f(x,y)=x^3+3xy+y-1:

∂f∂x=3x2+3y,∂f∂y=3x+1\frac{\partial f}{\partial x}=3x^2+3y,\qquad \frac{\partial f}{\partial y}=3x+1

At (4,−5)(4,-5):

fx=3(16)+3(−5)=33,fy=3(4)+1=13f_x=3(16)+3(-5)=33,\qquad f_y=3(4)+1=13

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5 marks

Evaluate ∫0π/2(sin⁡2xcos⁡3x+cos⁡2xsin⁡3x) dx\int_0^{\pi/2}(\sin 2x\cos 3x+\cos 2x\sin 3x)\,dx and ∫0π/4dx1−sin⁡x\int_0^{\pi/4}\frac{dx}{1-\sin x}.

Answer

First integral. Using sin⁡Acos⁡B+cos⁡Asin⁡B=sin⁡(A+B)\sin A\cos B+\cos A\sin B=\sin(A+B), the integrand is sin⁡5x\sin5x.

∫0π/2sin⁡5x dx=[−cos⁡5x5]0π/2=−cos⁡(5π/2)+cos⁡05=0+15=15\int_0^{\pi/2}\sin5x\,dx=\left[-\frac{\cos5x}{5}\right]_0^{\pi/2}=\frac{-\cos(5\pi/2)+\cos0}{5}=\frac{0+1}{5}=\frac15

Second integral. Since 11−sin⁡x=1+sin⁡xcos⁡2x=sec⁡2x+sec⁡xtan⁡x\frac{1}{1-\sin x}=\frac{1+\sin x}{\cos^2x}=\sec^2x+\sec x\tan x,

∫0π/4dx1−sin⁡x=[tan⁡x+sec⁡x]0π/4=(1+2)−1=2\int_0^{\pi/4}\frac{dx}{1-\sin x}=\Big[\tan x+\sec x\Big]_0^{\pi/4}=(1+\sqrt2)-1=\sqrt2

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5 marks

Determine the concavity of y=3+sin⁡xy=3+\sin x on [0,2π][0,2\pi].

Answer

Concavity is determined by the sign of y′′y''.

y′=cos⁡x,y′′=−sin⁡xy'=\cos x,\qquad y''=-\sin x

  • On (0,π)(0,\pi): sin⁡x>0\sin x>0, so y′′<0y''<0 and the graph is concave down.
  • On (π,2π)(\pi,2\pi): sin⁡x<0\sin x<0, so y′′>0y''>0 and the graph is concave up.

The concavity changes at x=πx=\pi, so (π,3)(\pi,3) is a point of inflection.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2080 · 5 marks

Test the convergence of ∑n=1∞(1n+1)n\sum_{n=1}^{\infty}\left(\frac{1}{n+1}\right)^n.

Answer

Use the root test with an=(1n+1)na_n=\left(\frac{1}{n+1}\right)^n.

lim⁡n→∞ann=lim⁡n→∞1n+1=0<1\lim_{n\to\infty}\sqrt[n]{a_n}=\lim_{n\to\infty}\frac{1}{n+1}=0<1

Since the limit is less than 11, the series ∑n=1∞(1n+1)n\sum_{n=1}^\infty\left(\frac1{n+1}\right)^n converges.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Explain the meaning of lim⁡x→2f(x)=5\lim_{x\to 2} f(x)=5. Can this hold while f(2)=3f(2)=3? Explain.

Answer

Meaning. lim⁡x→2f(x)=5\lim_{x\to2}f(x)=5 means that f(x)f(x) can be made as close to 55 as we like by taking xx sufficiently close to 22 (but x≠2x\ne2). Formally, for every ε>0\varepsilon>0 there is δ>0\delta>0 such that 0<∣x−2∣<δ0<|x-2|<\delta implies ∣f(x)−5∣<ε|f(x)-5|<\varepsilon. The values from both the left and the right approach 55.

Can f(2)=3f(2)=3? Yes. A limit depends only on the values of ff near 22, not at 22 itself (the condition 0<∣x−2∣0<|x-2| excludes x=2x=2). For example,

f(x)={5,x≠23,x=2f(x)=\begin{cases}5,&x\neq2\\3,&x=2\end{cases}

has lim⁡x→2f(x)=5\lim_{x\to2}f(x)=5 but f(2)=3f(2)=3. In this case ff is not continuous at 22, since continuity would require f(2)=5f(2)=5.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Find dydx\dfrac{dy}{dx} for y=tan⁡−1xxy=\dfrac{\tan^{-1}x}{\sqrt{x}}.

Answer

Write y=tan⁡−1x⋅x−1/2y=\tan^{-1}x\cdot x^{-1/2} and use the product rule.

dydx=11+x2⋅x−1/2−12x−3/2tan⁡−1x\frac{dy}{dx}=\frac{1}{1+x^2}\cdot x^{-1/2}-\frac12x^{-3/2}\tan^{-1}x

dydx=1x (1+x2)−tan⁡−1x2xx=2x−(1+x2)tan⁡−1x2x3/2(1+x2)\frac{dy}{dx}=\frac{1}{\sqrt x\,(1+x^2)}-\frac{\tan^{-1}x}{2x\sqrt x}=\frac{2x-(1+x^2)\tan^{-1}x}{2x^{3/2}(1+x^2)}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Find the area of the region bounded by y=−xy=-x and x=y2+3yx=y^2+3y.

Answer

Treat xx as a function of yy. Equate −y=y2+3y-y=y^2+3y:

y2+4y=0 ⇒ y=−4 or y=0y^2+4y=0\ \Rightarrow\ y=-4\text{ or }y=0

For −4<y<0-4<y<0 (test y=−1y=-1): the line gives x=1x=1 and the parabola gives x=−2x=-2, so the line x=−yx=-y is on the right.

A=∫−40[−y−(y2+3y)]dy=∫−40(−4y−y2) dy=[−2y2−y33]−40A=\int_{-4}^{0}\big[-y-(y^2+3y)\big]dy=\int_{-4}^{0}(-4y-y^2)\,dy=\left[-2y^2-\frac{y^3}{3}\right]_{-4}^{0}

A=0−(−32+643)=323 square unitsA=0-\left(-32+\frac{64}{3}\right)=\frac{32}{3}\text{ square units}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Evaluate ∫4−x2 dx\int \sqrt{4-x^2}\,dx.

Answer

Let x=2sin⁡θx=2\sin\theta, so dx=2cos⁡θ dθdx=2\cos\theta\,d\theta and 4−x2=2cos⁡θ\sqrt{4-x^2}=2\cos\theta (for ∣θ∣≤π/2|\theta|\le\pi/2).

∫4−x2 dx=∫4cos⁡2θ dθ=2θ+sin⁡2θ+C=2θ+2sin⁡θcos⁡θ+C\int\sqrt{4-x^2}\,dx=\int4\cos^2\theta\,d\theta=2\theta+\sin2\theta+C=2\theta+2\sin\theta\cos\theta+C

With sin⁡θ=x2\sin\theta=\frac x2, cos⁡θ=4−x22\cos\theta=\frac{\sqrt{4-x^2}}{2}:

∫4−x2 dx=2sin⁡−1x2+x4−x22+C\int\sqrt{4-x^2}\,dx=2\sin^{-1}\frac x2+\frac{x\sqrt{4-x^2}}{2}+C

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Find the volume of the solid formed by rotating about the y-axis the region bounded by y=xy=x and y=x2y=x^2.

Answer

The curves y=xy=x and y=x2y=x^2 meet at x=0x=0 and x=1x=1, and x≥x2x\ge x^2 on [0,1][0,1]. Using cylindrical shells about the y-axis (radius xx, height x−x2x-x^2):

V=2π∫01x(x−x2) dx=2π∫01(x2−x3) dx=2π[x33−x44]01=2π⋅112V=2\pi\int_0^1x(x-x^2)\,dx=2\pi\int_0^1(x^2-x^3)\,dx=2\pi\left[\frac{x^3}{3}-\frac{x^4}{4}\right]_0^1=2\pi\cdot\frac1{12}

V=π6 cubic unitsV=\frac{\pi}{6}\text{ cubic units}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Evaluate ∫05dxx−2\int_0^5 \dfrac{dx}{\sqrt{x-2}}, if it exists.

Answer

The integrand 1x−2\frac1{\sqrt{x-2}} is defined only for x>2x>2. On the part 0≤x<20\le x<2 of the interval of integration, x−2<0x-2<0 and the square root is not a real number. Moreover, the function is unbounded at x=2x=2 (an infinite discontinuity inside [0,5][0,5]).

Hence ∫05dxx−2\int_0^5\frac{dx}{\sqrt{x-2}} does not exist as a real integral.

For comparison, the part on which the function is defined converges:

∫25dxx−2=lim⁡a→2+[2x−2]a5=23\int_2^5\frac{dx}{\sqrt{x-2}}=\lim_{a\to2^+}\Big[2\sqrt{x-2}\Big]_a^5=2\sqrt3

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Test whether ∑n=2∞2n2−1\sum_{n=2}^{\infty}\dfrac{2}{n^2-1} converges or diverges.

Answer

Use partial fractions:

2n2−1=1n−1−1n+1\frac{2}{n^2-1}=\frac{1}{n-1}-\frac1{n+1}

The partial sum telescopes:

SN=∑n=2N(1n−1−1n+1)=1+12−1N−1N+1S_N=\sum_{n=2}^{N}\left(\frac1{n-1}-\frac1{n+1}\right)=1+\frac12-\frac1N-\frac1{N+1}

lim⁡N→∞SN=32\lim_{N\to\infty}S_N=\frac32

The series converges, with sum 32\frac32. (This also follows by comparison with ∑1n2\sum\frac1{n^2}.)

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Use Newton's method to find 104\sqrt[4]{10} correct to four decimal places.

Answer

We want the root of f(x)=x4−10=0f(x)=x^4-10=0. Newton's formula is

xn+1=xn−xn4−104xn3=3xn+10/xn34x_{n+1}=x_n-\frac{x_n^4-10}{4x_n^3}=\frac{3x_n+10/x_n^3}{4}

Since 1.74<10<1.841.7^4<10<1.8^4 (that is, 8.35<10<10.58.35<10<10.5), start with x0=1.8x_0=1.8.

  • x1=5.4+10/5.8324=5.4+1.714684=1.77867x_1=\dfrac{5.4+10/5.832}{4}=\dfrac{5.4+1.71468}{4}=1.77867
  • x2=5.33601+10/5.627124=5.33601+1.777084=1.77827x_2=\dfrac{5.33601+10/5.62712}{4}=\dfrac{5.33601+1.77708}{4}=1.77827
  • x3≈1.77828x_3\approx1.77828

The values agree to four decimal places, so

104≈1.7783\sqrt[4]{10}\approx1.7783

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Find fxf_x, fyf_y and fxyf_{xy} for f(x,y)=x y3+x4yf(x,y)=\sqrt{x}\,y^3+x^4y at (−4,1)(-4,1).

Answer

Treat the other variable as a constant.

fx=y32x+4x3y,fy=3x y2+x4,fxy=3y22x+4x3f_x=\frac{y^3}{2\sqrt x}+4x^3y,\qquad f_y=3\sqrt x\,y^2+x^4,\qquad f_{xy}=\frac{3y^2}{2\sqrt x}+4x^3

The term x\sqrt x is not a real number at x=−4x=-4, so ff is only defined for x≥0x\ge0 over the reals and these derivatives do not exist as real numbers at (−4,1)(-4,1). Taking −4=2i\sqrt{-4}=2i formally gives

fx=−256−i4,fy=256+6i,fxy=−256−3i4f_x=-256-\frac i4,\qquad f_y=256+6i,\qquad f_{xy}=-256-\frac{3i}{4}

If the point is (4,1)(4,1) (where everything is real):

fx=14+256=256.25,fy=6+256=262,fxy=34+256=256.75f_x=\frac14+256=256.25,\qquad f_y=6+256=262,\qquad f_{xy}=\frac34+256=256.75

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Test whether f(x)={x2−2xx−2,xeq21,x=2f(x)=\begin{cases}\dfrac{x^2-2x}{x-2}, & x eq 2\\ 1, & x=2\end{cases} is continuous at x=2x=2. Explain.

Answer

Three conditions are needed for continuity at x=2x=2: f(2)f(2) exists, lim⁡x→2f(x)\lim_{x\to2}f(x) exists, and they are equal.

  • f(2)=1f(2)=1.
  • For x≠2x\neq2: x2−2xx−2=x(x−2)x−2=x\dfrac{x^2-2x}{x-2}=\dfrac{x(x-2)}{x-2}=x, so lim⁡x→2f(x)=2\lim_{x\to2}f(x)=2.

The limit exists but lim⁡x→2f(x)=2≠1=f(2)\lim_{x\to2}f(x)=2\neq1=f(2). Hence ff is not continuous at x=2x=2. It has a removable discontinuity, which would be removed by defining f(2)=2f(2)=2.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081 · 5 marks

Evaluate ∫0πxsin⁡x dx\int_0^{\pi} x\sin x\,dx.

Answer

Integrate by parts with u=xu=x, dv=sin⁡x dxdv=\sin x\,dx, so du=dxdu=dx, v=−cos⁡xv=-\cos x.

∫0πxsin⁡x dx=[−xcos⁡x]0π+∫0πcos⁡x dx=π+[sin⁡x]0π=π+0\int_0^\pi x\sin x\,dx=\Big[-x\cos x\Big]_0^\pi+\int_0^\pi\cos x\,dx=\pi+\Big[\sin x\Big]_0^\pi=\pi+0

∫0πxsin⁡x dx=π\int_0^\pi x\sin x\,dx=\pi

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Show that f(x)=1−1−x2f(x)=1-\sqrt{1-x^2} is continuous on [−1,1][-1,1].

Answer

Let g(x)=1−x2g(x)=1-x^2, a polynomial, hence continuous everywhere. On [−1,1][-1,1], g(x)≥0g(x)\ge0, and  \sqrt{\ } is continuous on [0,∞)[0,\infty). So 1−x2\sqrt{1-x^2} is continuous at every c∈(−1,1)c\in(-1,1) as a composition of continuous functions, and so is f(x)=1−1−x2f(x)=1-\sqrt{1-x^2}.

At the endpoints we need one-sided continuity:

lim⁡x→1−f(x)=1−1−1=0=f(1),lim⁡x→−1+f(x)=1−1−1=0=f(−1)\lim_{x\to1^-}f(x)=1-\sqrt{1-1}=0=f(1),\qquad \lim_{x\to-1^+}f(x)=1-\sqrt{1-1}=0=f(-1)

Hence ff is continuous on the closed interval [−1,1][-1,1].

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Evaluate lim⁡x→∞x(x−2−x)\lim_{x\to\infty}\sqrt{x}\left(\sqrt{x-2}-\sqrt{x}\right).

Answer

Rationalise by multiplying by the conjugate of x−2−x\sqrt{x-2}-\sqrt x.

x(x−2−x)=x⋅(x−2)−xx−2+x=−2xx−2+x\sqrt x\left(\sqrt{x-2}-\sqrt x\right)=\sqrt x\cdot\frac{(x-2)-x}{\sqrt{x-2}+\sqrt x}=\frac{-2\sqrt x}{\sqrt{x-2}+\sqrt x}

Divide numerator and denominator by x\sqrt x:

=−21−2/x+1→−21+1=−1=\frac{-2}{\sqrt{1-2/x}+1}\to\frac{-2}{1+1}=-1

lim⁡x→∞x(x−2−x)=−1\lim_{x\to\infty}\sqrt{x}\left(\sqrt{x-2}-\sqrt{x}\right)=-1

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

If f(x)=x2+2x−1f(x)=x^2+2x-1 and g(x)=2x−3g(x)=2x-3, find fog(x)fog(x) and gof(x)gof(x).

Answer

f∘gf\circ g:

(f∘g)(x)=f(g(x))=(2x−3)2+2(2x−3)−1=4x2−12x+9+4x−6−1=4x2−8x+2(f\circ g)(x)=f(g(x))=(2x-3)^2+2(2x-3)-1=4x^2-12x+9+4x-6-1=4x^2-8x+2

g∘fg\circ f:

(g∘f)(x)=g(f(x))=2(x2+2x−1)−3=2x2+4x−5(g\circ f)(x)=g(f(x))=2(x^2+2x-1)-3=2x^2+4x-5

Note that f∘g≠g∘ff\circ g\neq g\circ f in general.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Find the local maxima and local minima of f(x)=3x4−4x3−12x2+5f(x)=3x^4-4x^3-12x^2+5.

Answer

f′(x)=12x3−12x2−24x=12x(x2−x−2)=12x(x−2)(x+1)f'(x)=12x^3-12x^2-24x=12x(x^2-x-2)=12x(x-2)(x+1)

The critical points are x=−1, 0, 2x=-1,\,0,\,2.

Sign of f′f': negative on (−∞,−1)(-\infty,-1), positive on (−1,0)(-1,0), negative on (0,2)(0,2), positive on (2,∞)(2,\infty).

  • At x=−1x=-1, f′f' changes from −- to ++: local minimum, f(−1)=3+4−12+5=0f(-1)=3+4-12+5=0.
  • At x=0x=0, f′f' changes from ++ to −-: local maximum, f(0)=5f(0)=5.
  • At x=2x=2, f′f' changes from −- to ++: local minimum, f(2)=48−32−48+5=−27f(2)=48-32-48+5=-27.

Check with f′′(x)=36x2−24x−24f''(x)=36x^2-24x-24: f′′(−1)=36>0f''(-1)=36>0, f′′(0)=−24<0f''(0)=-24<0, f′′(2)=72>0f''(2)=72>0, which agrees.

So the local maximum is 55 at x=0x=0, and the local minima are 00 at x=−1x=-1 and −27-27 at x=2x=2.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Find the area enclosed by the ellipse x29+y24=1\frac{x^2}{9}+\frac{y^2}{4}=1.

Answer

By symmetry, the area is 44 times the area in the first quadrant. From the ellipse, y=239−x2y=\frac23\sqrt{9-x^2} for y≥0y\ge0.

A=4∫03239−x2 dx=83∫039−x2 dxA=4\int_0^3\frac23\sqrt{9-x^2}\,dx=\frac83\int_0^3\sqrt{9-x^2}\,dx

The integral ∫039−x2 dx\int_0^3\sqrt{9-x^2}\,dx is the area of a quarter circle of radius 33, namely 9π4\frac{9\pi}{4} (or, with x=3sin⁡θx=3\sin\theta, it equals 92⋅π2\frac92\cdot\frac\pi2).

A=83⋅9π4=6πA=\frac83\cdot\frac{9\pi}{4}=6\pi

This agrees with the general formula A=πab=π(3)(2)=6πA=\pi ab=\pi(3)(2)=6\pi square units.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Evaluate ∫02xx2+4 dx\int_0^2 \frac{x}{\sqrt{x^2+4}}\,dx.

Answer

Let u=x2+4u=x^2+4, so du=2x dxdu=2x\,dx. When x=0x=0, u=4u=4; when x=2x=2, u=8u=8.

∫02xx2+4 dx=12∫48u−1/2 du=[u]48=22−2≈0.828\int_0^2\frac{x}{\sqrt{x^2+4}}\,dx=\frac12\int_4^8u^{-1/2}\,du=\Big[\sqrt u\Big]_4^8=2\sqrt2-2\approx0.828

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Solve xy′=yxy'=y, given y(1)=2y(1)=2.

Answer

Separate the variables:

dyy=dxx\frac{dy}{y}=\frac{dx}{x}

Integrate both sides:

ln⁡∣y∣=ln⁡∣x∣+C1  ⇒  y=Cx\ln|y|=\ln|x|+C_1\;\Rightarrow\; y=Cx

Apply y(1)=2y(1)=2: 2=C⋅12=C\cdot 1, so C=2C=2.

y=2xy=2x

Check: xy′=x⋅2=2x=yxy'=x\cdot 2=2x=y. ✓

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Determine whether ∑n=1∞52n2+4n+3\sum_{n=1}^{\infty}\frac{5}{2n^2+4n+3} is convergent or divergent.

Answer

Compare with the p-series ∑1n2\sum \frac{1}{n^2}, which converges (p=2>1p=2>1).

For n≥1n\ge 1, 2n2+4n+3>2n22n^2+4n+3>2n^2, so

0<52n2+4n+3<52n2.0<\frac{5}{2n^2+4n+3}<\frac{5}{2n^2}.

Since ∑52n2=52∑1n2\sum \frac{5}{2n^2}=\frac52\sum\frac1{n^2} converges, by the Direct Comparison Test the given series also converges.

(Limit comparison: lim⁡n→∞5/(2n2+4n+3)1/n2=52\lim_{n\to\infty}\frac{5/(2n^2+4n+3)}{1/n^2}=\frac52, finite and positive, giving the same conclusion.)

The series is convergent.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Find a unit vector in the same direction as −3i+7j-3\mathbf{i}+7\mathbf{j}.

Answer

Let v=−3i+7j\mathbf{v}=-3\mathbf{i}+7\mathbf{j}.

∣v∣=(−3)2+72=58|\mathbf{v}|=\sqrt{(-3)^2+7^2}=\sqrt{58}

The unit vector is

u^=v∣v∣=−358i+758j.\hat{\mathbf{u}}=\frac{\mathbf{v}}{|\mathbf{v}|}=\frac{-3}{\sqrt{58}}\mathbf{i}+\frac{7}{\sqrt{58}}\mathbf{j}.

Check: 958+4958=1\frac{9}{58}+\frac{49}{58}=1. ✓

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Solve y′′−y′−6y=0y''-y'-6y=0.

Answer

Auxiliary equation:

m2−m−6=0  ⇒  (m−3)(m+2)=0  ⇒  m=3, −2.m^2-m-6=0\;\Rightarrow\;(m-3)(m+2)=0\;\Rightarrow\; m=3,\,-2.

The roots are real and distinct, so the general solution is

y=C1e3x+C2e−2x.y=C_1e^{3x}+C_2e^{-2x}.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Use the chain rule to find dzdt\frac{dz}{dt} when z=cos⁡(x+4y)z=\cos(x+4y), x=5t4x=5t^4, y=1ty=\frac{1}{t}.

Answer

By the chain rule:

dzdt=∂z∂xdxdt+∂z∂ydydt\frac{dz}{dt}=\frac{\partial z}{\partial x}\frac{dx}{dt}+\frac{\partial z}{\partial y}\frac{dy}{dt}

Here ∂z∂x=−sin⁡(x+4y)\frac{\partial z}{\partial x}=-\sin(x+4y), ∂z∂y=−4sin⁡(x+4y)\frac{\partial z}{\partial y}=-4\sin(x+4y), dxdt=20t3\frac{dx}{dt}=20t^3, dydt=−1t2\frac{dy}{dt}=-\frac{1}{t^2}.

dzdt=−sin⁡(x+4y)⋅20t3−4sin⁡(x+4y)⋅(−1t2)=(−20t3+4t2)sin⁡(x+4y)\frac{dz}{dt}=-\sin(x+4y)\cdot 20t^3-4\sin(x+4y)\cdot\left(-\frac1{t^2}\right)=\left(-20t^3+\frac{4}{t^2}\right)\sin(x+4y)

Substituting x=5t4x=5t^4, y=1/ty=1/t:

dzdt=(4t2−20t3)sin⁡ ⁣(5t4+4t).\frac{dz}{dt}=\left(\frac{4}{t^2}-20t^3\right)\sin\!\left(5t^4+\frac4t\right).

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Find ∂z∂x\frac{\partial z}{\partial x} and ∂z∂y\frac{\partial z}{\partial y} if x3+y3+z3+6xyz=1x^3+y^3+z^3+6xyz=1.

Answer

Let F(x,y,z)=x3+y3+z3+6xyz−1=0F(x,y,z)=x^3+y^3+z^3+6xyz-1=0.

Fx=3x2+6yz,Fy=3y2+6xz,Fz=3z2+6xy.F_x=3x^2+6yz,\quad F_y=3y^2+6xz,\quad F_z=3z^2+6xy.

Using implicit differentiation, ∂z∂x=−FxFz\frac{\partial z}{\partial x}=-\frac{F_x}{F_z} and ∂z∂y=−FyFz\frac{\partial z}{\partial y}=-\frac{F_y}{F_z}:

∂z∂x=−3x2+6yz3z2+6xy=−x2+2yzz2+2xy\frac{\partial z}{\partial x}=-\frac{3x^2+6yz}{3z^2+6xy}=-\frac{x^2+2yz}{z^2+2xy}

∂z∂y=−3y2+6xz3z2+6xy=−y2+2xzz2+2xy\frac{\partial z}{\partial y}=-\frac{3y^2+6xz}{3z^2+6xy}=-\frac{y^2+2xz}{z^2+2xy}

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Find the Maclaurin series expansion of f(x)=ln⁡xf(x)=\ln x.

Answer

ln⁡x\ln x is not defined at x=0x=0, so a Maclaurin series does not exist for it. The nearest valid expansion is about x=1x=1 (a Taylor series), which is equivalent to the Maclaurin series of ln⁡(1+t)\ln(1+t) with t=x−1t=x-1.

Derivatives of f(x)=ln⁡xf(x)=\ln x at x=1x=1:

f(1)=0f(1)=0, f′(x)=x−1⇒f′(1)=1f'(x)=x^{-1}\Rightarrow f'(1)=1, f′′(1)=−1f''(1)=-1, f′′′(1)=2f'''(1)=2, f(4)(1)=−6f^{(4)}(1)=-6; in general f(n)(1)=(−1)n−1(n−1)!f^{(n)}(1)=(-1)^{n-1}(n-1)!.

Taylor's formula f(x)=∑f(n)(1)n!(x−1)nf(x)=\sum \frac{f^{(n)}(1)}{n!}(x-1)^n gives

ln⁡x=(x−1)−(x−1)22+(x−1)33−(x−1)44+⋯=∑n=1∞(−1)n−1n(x−1)n\ln x=(x-1)-\frac{(x-1)^2}{2}+\frac{(x-1)^3}{3}-\frac{(x-1)^4}{4}+\cdots=\sum_{n=1}^{\infty}\frac{(-1)^{n-1}}{n}(x-1)^n

This is valid for 0<x≤20<x\le 2 (radius of convergence 11).

Equivalently, the Maclaurin series of ln⁡(1+x)\ln(1+x) is

ln⁡(1+x)=x−x22+x33−⋯ ,−1<x≤1.\ln(1+x)=x-\frac{x^2}{2}+\frac{x^3}{3}-\cdots,\quad -1<x\le1.

Answer checked by Claude Sonnet · Oct 21, 2026

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  • 2081.2 · 5 marks

Test whether f(x)={x2−4x−2xeq24x=2f(x)=\begin{cases}\frac{x^2-4}{x-2} & x eq 2\\ 4 & x=2\end{cases} is continuous or discontinuous at x=2x=2. Explain.

Answer

For x≠2x\ne2: f(x)=x2−4x−2=x+2f(x)=\frac{x^2-4}{x-2}=x+2.

Limit at x=2x=2:

lim⁡x→2f(x)=lim⁡x→2(x+2)=4.\lim_{x\to2}f(x)=\lim_{x\to2}(x+2)=4.

Value at x=2x=2: f(2)=4f(2)=4.

A function is continuous at x=ax=a if lim⁡x→af(x)=f(a)\lim_{x\to a}f(x)=f(a). Here lim⁡x→2f(x)=4=f(2)\lim_{x\to2}f(x)=4=f(2), so all three conditions (defined, limit exists, equal) hold.

Hence ff is continuous at x=2x=2. The value 44 given at x=2x=2 exactly fills the removable gap in x2−4x−2\frac{x^2-4}{x-2}.

Answer checked by Claude Sonnet · Oct 21, 2026

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