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Section A: Long Answer Questions

Attempt any TWO questions.

3 questions·10 marks each
1long10 marks

State and prove the mean value theorem (Lagrange's). Verify it for (f(x) = \sqrt{x}) on [1,4].

Lagrange's Mean Value Theorem (MVT)

Statement. If a function ff is

  1. continuous on the closed interval [a,b][a,b], and
  2. differentiable on the open interval (a,b)(a,b),

then there exists at least one point c(a,b)c \in (a,b) such that

f(c)=f(b)f(a)ba.f'(c) = \frac{f(b) - f(a)}{b - a}.

Proof (using Rolle's Theorem)

Define an auxiliary function

ϕ(x)=f(x)f(a)f(b)f(a)ba(xa).\phi(x) = f(x) - f(a) - \frac{f(b) - f(a)}{b - a}\,(x - a).
  • ϕ\phi is continuous on [a,b][a,b] (sum/difference of continuous functions).
  • ϕ\phi is differentiable on (a,b)(a,b).
  • At the endpoints:
ϕ(a)=f(a)f(a)0=0,\phi(a) = f(a) - f(a) - 0 = 0, ϕ(b)=f(b)f(a)f(b)f(a)ba(ba)=0.\phi(b) = f(b) - f(a) - \frac{f(b)-f(a)}{b-a}(b-a) = 0.

Since ϕ(a)=ϕ(b)=0\phi(a) = \phi(b) = 0, by Rolle's Theorem there exists c(a,b)c \in (a,b) with ϕ(c)=0\phi'(c) = 0. Now

ϕ(x)=f(x)f(b)f(a)ba,\phi'(x) = f'(x) - \frac{f(b) - f(a)}{b - a},

so ϕ(c)=0\phi'(c) = 0 gives

f(c)=f(b)f(a)ba.f'(c) = \frac{f(b) - f(a)}{b - a}. \qquad \blacksquare

Verification for f(x)=xf(x) = \sqrt{x} on [1,4][1,4]

f(x)=xf(x) = \sqrt{x} is continuous on [1,4][1,4] and differentiable on (1,4)(1,4), so MVT applies.

f(1)=1,f(4)=2,f(4)f(1)41=213=13.f(1) = 1, \quad f(4) = 2, \quad \frac{f(4)-f(1)}{4-1} = \frac{2-1}{3} = \frac{1}{3}.

Also f(x)=12xf'(x) = \dfrac{1}{2\sqrt{x}}. Set f(c)=13f'(c) = \tfrac{1}{3}:

12c=13    2c=3    c=32    c=94=2.25.\frac{1}{2\sqrt{c}} = \frac{1}{3} \;\Rightarrow\; 2\sqrt{c} = 3 \;\Rightarrow\; \sqrt{c} = \frac{3}{2} \;\Rightarrow\; c = \frac{9}{4} = 2.25.

Since c=2.25(1,4)c = 2.25 \in (1,4), the theorem is verified.

mean-value-theorem
2long10 marks

Evaluate (\int \frac{dx}{(x^2 + a^2)^2}) using a suitable substitution.

Evaluate dx(x2+a2)2\displaystyle \int \frac{dx}{(x^2 + a^2)^2}

Use the substitution x=atanθx = a\tan\theta, so that dx=asec2θdθdx = a\sec^2\theta\,d\theta and

x2+a2=a2tan2θ+a2=a2sec2θ.x^2 + a^2 = a^2\tan^2\theta + a^2 = a^2\sec^2\theta.

Then

dx(x2+a2)2=asec2θdθ(a2sec2θ)2=asec2θa4sec4θdθ=1a3cos2θdθ.\int \frac{dx}{(x^2+a^2)^2} = \int \frac{a\sec^2\theta\,d\theta}{(a^2\sec^2\theta)^2} = \int \frac{a\sec^2\theta}{a^4\sec^4\theta}\,d\theta = \frac{1}{a^3}\int \cos^2\theta\,d\theta.

Using cos2θ=1+cos2θ2\cos^2\theta = \dfrac{1 + \cos 2\theta}{2}:

=1a312(θ+sin2θ2)=12a3(θ+sin2θ2).= \frac{1}{a^3}\cdot \frac{1}{2}\left(\theta + \frac{\sin 2\theta}{2}\right) = \frac{1}{2a^3}\left(\theta + \frac{\sin 2\theta}{2}\right).

Now convert back. Since tanθ=xa\tan\theta = \dfrac{x}{a}, we have θ=tan1xa\theta = \tan^{-1}\dfrac{x}{a}, and

sinθ=xx2+a2,cosθ=ax2+a2,\sin\theta = \frac{x}{\sqrt{x^2+a^2}}, \quad \cos\theta = \frac{a}{\sqrt{x^2+a^2}}, sin2θ=2sinθcosθ=2axx2+a2.\sin 2\theta = 2\sin\theta\cos\theta = \frac{2ax}{x^2 + a^2}.

Therefore

dx(x2+a2)2=12a3tan1xa+x2a2(x2+a2)+C.\boxed{\int \frac{dx}{(x^2+a^2)^2} = \frac{1}{2a^3}\tan^{-1}\frac{x}{a} + \frac{x}{2a^2(x^2+a^2)} + C.}
integration
3long10 marks

Solve the differential equation (\frac{d^2y}{dx^2} + 4y = \cos 2x).

Solve d2ydx2+4y=cos2x\dfrac{d^2y}{dx^2} + 4y = \cos 2x

Complementary function (CF)

Auxiliary equation: m2+4=0m=±2im^2 + 4 = 0 \Rightarrow m = \pm 2i. Hence

yc=C1cos2x+C2sin2x.y_c = C_1\cos 2x + C_2\sin 2x.

Particular integral (PI)

yp=1D2+4cos2x.y_p = \frac{1}{D^2 + 4}\cos 2x.

The operator D2+4D^2 + 4 applied to cos2x\cos 2x gives 22+4=0-2^2 + 4 = 0 (failure case, since cos2x\cos 2x is part of the CF). Use the standard result for resonance:

1D2+a2cosax=x2asinax.\frac{1}{D^2 + a^2}\cos ax = \frac{x}{2a}\sin ax.

With a=2a = 2:

yp=x22sin2x=x4sin2x.y_p = \frac{x}{2\cdot 2}\sin 2x = \frac{x}{4}\sin 2x.

General solution

y=C1cos2x+C2sin2x+x4sin2x.\boxed{y = C_1\cos 2x + C_2\sin 2x + \frac{x}{4}\sin 2x.}
differential-equations
B

Section B: Short Answer Questions

Attempt any EIGHT questions.

9 questions·5 marks each
4short5 marks

Evaluate (\lim_{x \to 1}\frac{x^n - 1}{x - 1}).

Evaluate limx1xn1x1\displaystyle\lim_{x \to 1}\frac{x^n - 1}{x - 1}

This is a 00\tfrac{0}{0} form. Using the standard limit limxaxnanxa=nan1\displaystyle\lim_{x\to a}\frac{x^n - a^n}{x - a} = n a^{n-1} with a=1a = 1:

limx1xn1x1=n1n1=n.\lim_{x \to 1}\frac{x^n - 1}{x - 1} = n\cdot 1^{\,n-1} = n.

(Equivalently, factor xn1=(x1)(xn1+xn2++1)x^n - 1 = (x-1)(x^{n-1} + x^{n-2} + \cdots + 1), cancel (x1)(x-1), and put x=1x=1 in the nn-term sum to get nn.)

limx1xn1x1=n.\boxed{\lim_{x \to 1}\frac{x^n - 1}{x - 1} = n.}
limits
5short5 marks

If (y = e^{m\sin^{-1} x}), find (\frac{dy}{dx}).

If y=emsin1xy = e^{m\sin^{-1}x}, find dydx\dfrac{dy}{dx}

Differentiate using the chain rule. Let u=msin1xu = m\sin^{-1}x, so y=euy = e^{u} and dydx=eududx\dfrac{dy}{dx} = e^{u}\dfrac{du}{dx}.

Since ddxsin1x=11x2\dfrac{d}{dx}\sin^{-1}x = \dfrac{1}{\sqrt{1-x^2}},

dudx=m1x2.\frac{du}{dx} = \frac{m}{\sqrt{1 - x^2}}.

Therefore

dydx=memsin1x1x2=my1x2.\boxed{\frac{dy}{dx} = \frac{m\,e^{m\sin^{-1}x}}{\sqrt{1 - x^2}} = \frac{m\,y}{\sqrt{1 - x^2}}.}
differentiation
6short5 marks

Expand (\log(1 + x)) in a Maclaurin series.

Maclaurin expansion of log(1+x)\log(1 + x)

The Maclaurin series is f(x)=f(0)+f(0)x+f(0)2!x2+f(x) = f(0) + f'(0)x + \dfrac{f''(0)}{2!}x^2 + \cdots

For f(x)=log(1+x)f(x) = \log(1+x):

f(0)=0,  f(x)=11+xf(0)=1,  f(x)=1(1+x)2f(0)=1,f(0)=0,\; f'(x)=\tfrac{1}{1+x}\Rightarrow f'(0)=1,\; f''(x)=-\tfrac{1}{(1+x)^2}\Rightarrow f''(0)=-1, f(x)=2(1+x)3f(0)=2,f(4)(0)=6, f'''(x)=\tfrac{2}{(1+x)^3}\Rightarrow f'''(0)=2,\quad f^{(4)}(0)=-6,\ \dots

In general f(n)(0)=(1)n1(n1)!f^{(n)}(0) = (-1)^{n-1}(n-1)!, so the nn-th term is (1)n1(n1)!n!xn=(1)n1nxn\dfrac{(-1)^{n-1}(n-1)!}{n!}x^n = \dfrac{(-1)^{n-1}}{n}x^n. Hence

log(1+x)=xx22+x33x44+=n=1(1)n1nxn,\boxed{\log(1 + x) = x - \frac{x^2}{2} + \frac{x^3}{3} - \frac{x^4}{4} + \cdots = \sum_{n=1}^{\infty}\frac{(-1)^{n-1}}{n}x^n,}

valid for 1<x1-1 < x \le 1.

series-expansion
7short5 marks

Find the asymptotes of (y = \frac{2x^2 - 1}{x^2 - 4}).

Asymptotes of y=2x21x24y = \dfrac{2x^2 - 1}{x^2 - 4}

Vertical asymptotes

Set the denominator to zero: x24=0x=±2x^2 - 4 = 0 \Rightarrow x = \pm 2. The numerator is nonzero there, so

x=2andx=2x = 2 \quad\text{and}\quad x = -2

are the vertical asymptotes.

Horizontal asymptote

The degrees of numerator and denominator are equal, so

limx±y=21=2    y=2.\lim_{x\to\pm\infty} y = \frac{2}{1} = 2 \;\Rightarrow\; y = 2.

(There is no oblique asymptote since the degree of the numerator does not exceed that of the denominator.)

Asymptotes: x=2,  x=2,  y=2.\boxed{\text{Asymptotes: } x = 2,\; x = -2,\; y = 2.}
curve-tracing
8short5 marks

Evaluate (\int \frac{1}{1 + \cos x},dx).

Evaluate 11+cosxdx\displaystyle\int \frac{1}{1 + \cos x}\,dx

Use the half-angle identity 1+cosx=2cos2x21 + \cos x = 2\cos^2\dfrac{x}{2}:

dx1+cosx=dx2cos2x2=12sec2x2dx.\int \frac{dx}{1 + \cos x} = \int \frac{dx}{2\cos^2\frac{x}{2}} = \frac{1}{2}\int \sec^2\frac{x}{2}\,dx.

Since sec2x2dx=2tanx2\displaystyle\int \sec^2\frac{x}{2}\,dx = 2\tan\frac{x}{2},

=122tanx2+C.= \frac{1}{2}\cdot 2\tan\frac{x}{2} + C. dx1+cosx=tanx2+C.\boxed{\int \frac{dx}{1 + \cos x} = \tan\frac{x}{2} + C.}
integration
9short5 marks

Solve ((1 + x^2)\frac{dy}{dx} + 2xy = 4x^2).

Solve (1+x2)dydx+2xy=4x2(1 + x^2)\dfrac{dy}{dx} + 2xy = 4x^2

Notice the left side is an exact derivative. Dividing through is optional because

ddx[(1+x2)y]=(1+x2)dydx+2xy.\frac{d}{dx}\big[(1+x^2)y\big] = (1+x^2)\frac{dy}{dx} + 2xy.

So the equation becomes

ddx[(1+x2)y]=4x2.\frac{d}{dx}\big[(1+x^2)y\big] = 4x^2.

Integrating both sides:

(1+x2)y=4x2dx=4x33+C.(1+x^2)y = \int 4x^2\,dx = \frac{4x^3}{3} + C. y=11+x2(4x33+C).\boxed{y = \frac{1}{1+x^2}\left(\frac{4x^3}{3} + C\right).}

(Equivalently, in standard linear form dydx+2x1+x2y=4x21+x2\dfrac{dy}{dx} + \dfrac{2x}{1+x^2}y = \dfrac{4x^2}{1+x^2} the integrating factor is e2x1+x2dx=1+x2e^{\int \frac{2x}{1+x^2}dx} = 1+x^2, giving the same result.)

differential-equations
10short5 marks

If (\vec{a} \times \vec{b} = \vec{0}) and (\vec{a}\cdot\vec{b} = 0), what can you say about (\vec{a}) and (\vec{b})?

Given a×b=0\vec{a}\times\vec{b} = \vec{0} and ab=0\vec{a}\cdot\vec{b} = 0

  • a×b=0\vec{a}\times\vec{b} = \vec{0} means absinθ=0|\vec a||\vec b|\sin\theta = 0, so a\vec a and b\vec b are parallel (or one is the zero vector).
  • ab=0\vec{a}\cdot\vec{b} = 0 means abcosθ=0|\vec a||\vec b|\cos\theta = 0, so a\vec a and b\vec b are perpendicular (or one is the zero vector).

Two nonzero vectors cannot be simultaneously parallel and perpendicular. Hence both conditions hold together only if at least one of a\vec a, b\vec b is the zero vector:

a=0orb=0.\boxed{\vec a = \vec 0 \quad\text{or}\quad \vec b = \vec 0.}
vectors
11short5 marks

Find (\frac{\partial u}{\partial x}) if (u = x^y).

Find ux\dfrac{\partial u}{\partial x} if u=xyu = x^y

When taking the partial derivative with respect to xx, treat yy as a constant. Then u=xyu = x^y is a power function of xx, so by the power rule

ux=yxy1.\boxed{\frac{\partial u}{\partial x} = y\,x^{\,y-1}.}

(For contrast, uy=xylogx\dfrac{\partial u}{\partial y} = x^y \log x, where xx is held constant.)

partial-derivatives
12short5 marks

Change the order of integration in (\int_0^1 \int_x^1 f(x,y),dy,dx).

Change the order of integration in 01 ⁣x1f(x,y)dydx\displaystyle\int_0^1\!\int_x^1 f(x,y)\,dy\,dx

Identify the region

For the given limits: xx runs from 00 to 11, and for each xx, yy runs from y=xy = x up to y=1y = 1. The region RR is therefore the triangle bounded by

y=x,y=1,x=0,y = x,\quad y = 1,\quad x = 0,

i.e. {(x,y):0xy,  0y1}\{(x,y): 0 \le x \le y,\; 0 \le y \le 1\} — the triangle with vertices (0,0)(0,0), (0,1)(0,1) and (1,1)(1,1).

Reverse the order

Describing the same region with yy as the outer variable: yy ranges from 00 to 11, and for each fixed yy, xx ranges from 00 to yy (since yxy \ge x). Hence

01 ⁣x1f(x,y)dydx=01 ⁣0yf(x,y)dxdy.\boxed{\int_0^1\!\int_x^1 f(x,y)\,dy\,dx = \int_0^1\!\int_0^y f(x,y)\,dx\,dy.}
multiple-integrals

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