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Section A: Long Answer Questions

Attempt any TWO questions.

3 questions·10 marks each
1long10 marks

State and prove that a differentiable function is continuous. Examine the continuity and differentiability of f(x) = |x| at x = 0.

Theorem: Every differentiable function is continuous

Statement. If a function ff is differentiable at a point x=cx = c, then ff is continuous at x=cx = c.

Proof. Since ff is differentiable at cc, the derivative

f(c)=limxcf(x)f(c)xcf'(c) = \lim_{x \to c} \frac{f(x) - f(c)}{x - c}

exists (is finite). For xcx \neq c write

f(x)f(c)=f(x)f(c)xc(xc).f(x) - f(c) = \frac{f(x) - f(c)}{x - c}\cdot (x - c).

Taking limits as xcx \to c,

limxc(f(x)f(c))=limxcf(x)f(c)xclimxc(xc)=f(c)0=0.\lim_{x\to c}\big(f(x) - f(c)\big) = \lim_{x\to c}\frac{f(x)-f(c)}{x-c}\cdot \lim_{x\to c}(x-c) = f'(c)\cdot 0 = 0.

Hence limxcf(x)=f(c)\lim_{x\to c} f(x) = f(c), which is exactly the condition that ff is continuous at cc. \blacksquare

The converse is not true: continuity does not imply differentiability, as the next example shows.

Continuity and differentiability of f(x)=xf(x) = |x| at x=0x = 0

Here f(x)=x={x,x0x,x<0f(x) = |x| = \begin{cases} x, & x \ge 0 \\ -x, & x < 0 \end{cases} and f(0)=0f(0) = 0.

Continuity at x=0x = 0:

limx0f(x)=limx0(x)=0,limx0+f(x)=limx0+x=0.\lim_{x\to 0^-} f(x) = \lim_{x\to 0^-}(-x) = 0,\qquad \lim_{x\to 0^+} f(x) = \lim_{x\to 0^+} x = 0.

Both one-sided limits equal f(0)=0f(0) = 0, so ff is continuous at x=0x = 0.

Differentiability at x=0x = 0: compute the left- and right-hand derivatives.

Lf(0)=limh0f(0+h)f(0)h=limh0hh=1,Lf'(0) = \lim_{h\to 0^-}\frac{f(0+h)-f(0)}{h} = \lim_{h\to 0^-}\frac{-h}{h} = -1, Rf(0)=limh0+f(0+h)f(0)h=limh0+hh=+1.Rf'(0) = \lim_{h\to 0^+}\frac{f(0+h)-f(0)}{h} = \lim_{h\to 0^+}\frac{h}{h} = +1.

Since Lf(0)=1+1=Rf(0)Lf'(0) = -1 \neq +1 = Rf'(0), the derivative does not exist; ff is not differentiable at x=0x = 0.

Conclusion. f(x)=xf(x)=|x| is continuous but not differentiable at x=0x=0, confirming that continuity does not guarantee differentiability (geometrically, the graph has a sharp corner at the origin).

continuity
2long10 marks

Evaluate the integral (\int \frac{dx}{a^2 + x^2}) and (\int \frac{dx}{\sqrt{a^2 - x^2}}). Hence find (\int \frac{dx}{x^2 + 4x + 8}).

Standard integral 1: dxa2+x2\displaystyle\int \frac{dx}{a^2 + x^2}

Put x=atanθx = a\tan\theta, so dx=asec2θdθdx = a\sec^2\theta\, d\theta and a2+x2=a2sec2θa^2 + x^2 = a^2\sec^2\theta.

asec2θdθa2sec2θ=1adθ=θa+C=1atan1 ⁣xa+C.\int \frac{a\sec^2\theta\, d\theta}{a^2\sec^2\theta} = \frac{1}{a}\int d\theta = \frac{\theta}{a} + C = \boxed{\frac{1}{a}\tan^{-1}\!\frac{x}{a} + C.}

Standard integral 2: dxa2x2\displaystyle\int \frac{dx}{\sqrt{a^2 - x^2}}

Put x=asinθx = a\sin\theta, so dx=acosθdθdx = a\cos\theta\, d\theta and a2x2=acosθ\sqrt{a^2 - x^2} = a\cos\theta.

acosθdθacosθ=dθ=θ+C=sin1 ⁣xa+C.\int \frac{a\cos\theta\, d\theta}{a\cos\theta} = \int d\theta = \theta + C = \boxed{\sin^{-1}\!\frac{x}{a} + C.}

Application: dxx2+4x+8\displaystyle\int \frac{dx}{x^2 + 4x + 8}

Complete the square in the denominator:

x2+4x+8=(x+2)2+4=(x+2)2+22.x^2 + 4x + 8 = (x+2)^2 + 4 = (x+2)^2 + 2^2.

Let t=x+2t = x + 2, dt=dxdt = dx, with a=2a = 2. Using result 1,

dtt2+22=12tan1 ⁣t2+C=12tan1 ⁣(x+22)+C.\int \frac{dt}{t^2 + 2^2} = \frac{1}{2}\tan^{-1}\!\frac{t}{2} + C = \boxed{\frac{1}{2}\tan^{-1}\!\left(\frac{x+2}{2}\right) + C.}
integration
3long10 marks

Find the area bounded by the parabola (y^2 = 4ax) and its latus rectum.

Area bounded by y2=4axy^2 = 4ax and its latus rectum

Setup. For the parabola y2=4axy^2 = 4ax (vertex at origin, opening to the right), the focus is at (a,0)(a, 0) and the latus rectum is the vertical chord through the focus, i.e. the line x=ax = a. We want the area enclosed between the parabola and this line.

By symmetry about the xx-axis, the required area is twice the area above the xx-axis. On the parabola y=4ax=2axy = \sqrt{4ax} = 2\sqrt{a}\,\sqrt{x}, with xx running from 00 (vertex) to aa (latus rectum).

A=20aydx=20a2ax  dx=4a0ax1/2dx.A = 2\int_0^a y\, dx = 2\int_0^a 2\sqrt{a}\,\sqrt{x}\; dx = 4\sqrt{a}\int_0^a x^{1/2}\, dx.

Evaluate:

A=4a[x3/23/2]0a=4a23a3/2=83aa3/2=83a2.A = 4\sqrt{a}\left[\frac{x^{3/2}}{3/2}\right]_0^a = 4\sqrt{a}\cdot \frac{2}{3}\,a^{3/2} = \frac{8}{3}\sqrt{a}\cdot a^{3/2} = \frac{8}{3}a^{2}.

Result.

A=83a2 square units.\boxed{A = \frac{8}{3}a^2 \text{ square units.}}

(Equivalently, since the length of the latus rectum is 4a4a and it spans height 22a=4a2\cdot 2a = 4a, the enclosed region is two-thirds of the bounding rectangle a×4a=4a2a \times 4a = 4a^2, giving 23(4a2)=83a2\frac{2}{3}(4a^2) = \frac{8}{3}a^2.)

applications-of-integration
B

Section B: Short Answer Questions

Attempt any EIGHT questions.

9 questions·5 marks each
4short5 marks

Evaluate (\lim_{x \to 0} \frac{\sin x}{x}) using the definition of limit.

Evaluate limx0sinxx\displaystyle\lim_{x\to 0}\frac{\sin x}{x}

Geometric (sandwich) argument. For 0<x<π20 < x < \dfrac{\pi}{2}, comparing the areas of triangle OABOAB, the circular sector OABOAB, and triangle OACOAC in a unit circle gives

sinx<x<tanx.\sin x < x < \tan x.

Dividing throughout by sinx>0\sin x > 0:

1<xsinx<1cosxcosx<sinxx<1.1 < \frac{x}{\sin x} < \frac{1}{\cos x} \quad\Longrightarrow\quad \cos x < \frac{\sin x}{x} < 1.

The function sinxx\frac{\sin x}{x} is even, so the same inequality holds for x<0x<0. As x0x\to 0, cosx1\cos x \to 1, and by the Squeeze (Sandwich) Theorem

limx0sinxx=1.\boxed{\lim_{x\to 0}\frac{\sin x}{x} = 1.}
limits
5short5 marks

If (y = e^{ax}\sin bx), find (\frac{dy}{dx}).

Differentiate y=eaxsinbxy = e^{ax}\sin bx

Use the product rule ddx(uv)=uv+uv\frac{d}{dx}(uv) = u'v + uv' with u=eaxu = e^{ax}, v=sinbxv = \sin bx:

dudx=aeax,dvdx=bcosbx.\frac{du}{dx} = a\,e^{ax},\qquad \frac{dv}{dx} = b\cos bx. dydx=aeaxsinbx+eaxbcosbx=eax(asinbx+bcosbx).\frac{dy}{dx} = a\,e^{ax}\sin bx + e^{ax}\,b\cos bx = \boxed{e^{ax}\big(a\sin bx + b\cos bx\big).}

(This can also be written as dydx=a2+b2  eaxsin(bx+ϕ)\frac{dy}{dx} = \sqrt{a^2+b^2}\;e^{ax}\sin(bx + \phi) where tanϕ=b/a\tan\phi = b/a.)

differentiation
6short5 marks

State and verify Rolle's theorem for (f(x) = x^2 - 4x + 3) on [1,3].

Rolle's Theorem

Statement. If ff is (i) continuous on [a,b][a,b], (ii) differentiable on (a,b)(a,b), and (iii) f(a)=f(b)f(a) = f(b), then there exists at least one point c(a,b)c \in (a,b) such that f(c)=0f'(c) = 0.

Verification for f(x)=x24x+3f(x) = x^2 - 4x + 3 on [1,3][1,3]

Condition (i): ff is a polynomial, hence continuous on [1,3][1,3]. ✓

Condition (ii): ff is a polynomial, hence differentiable on (1,3)(1,3). ✓

Condition (iii):

f(1)=14+3=0,f(3)=912+3=0.f(1) = 1 - 4 + 3 = 0,\qquad f(3) = 9 - 12 + 3 = 0.

So f(1)=f(3)=0f(1) = f(3) = 0. ✓

All three hypotheses hold, so Rolle's theorem applies. To find cc:

f(x)=2x4=0    x=2.f'(x) = 2x - 4 = 0 \;\Longrightarrow\; x = 2.

Since c=2(1,3)c = 2 \in (1,3), Rolle's theorem is verified, with f(2)=0f'(2) = 0.

mean-value-theorem
7short5 marks

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

Asymptotes of y=x2+1x1\displaystyle y = \frac{x^2 + 1}{x - 1}

Vertical asymptote. The denominator vanishes at x=1x = 1, where the numerator x2+1=20x^2+1 = 2 \neq 0. Hence y±y \to \pm\infty as x1x \to 1, giving the vertical asymptote

x=1.\boxed{x = 1.}

Oblique (slant) asymptote. Since the degree of the numerator exceeds that of the denominator by one, divide:

x2+1x1=x+1+2x1.\frac{x^2 + 1}{x - 1} = x + 1 + \frac{2}{x - 1}.

As x±x \to \pm\infty, the remainder 2x10\dfrac{2}{x-1} \to 0, so

y=x+1\boxed{y = x + 1}

is the oblique asymptote.

Horizontal asymptote: none (the curve grows without bound). The asymptotes of the curve are therefore x=1x = 1 and y=x+1y = x + 1.

curve-tracing
8short5 marks

Evaluate (\int_0^{\pi/2} \sin^4 x , dx) using the reduction formula.

Evaluate 0π/2sin4xdx\displaystyle\int_0^{\pi/2}\sin^4 x\, dx by reduction formula

The reduction formula for In=0π/2sinnxdxI_n = \displaystyle\int_0^{\pi/2}\sin^n x\, dx is

In=n1nIn2.I_n = \frac{n-1}{n}\,I_{n-2}.

With n=4n = 4:

I4=34I2,I2=12I0.I_4 = \frac{3}{4}\,I_2, \qquad I_2 = \frac{1}{2}\,I_0.

The base case is

I0=0π/2dx=π2.I_0 = \int_0^{\pi/2} dx = \frac{\pi}{2}.

Therefore

I2=12π2=π4,I4=34π4=3π16.I_2 = \frac{1}{2}\cdot\frac{\pi}{2} = \frac{\pi}{4},\qquad I_4 = \frac{3}{4}\cdot\frac{\pi}{4} = \frac{3\pi}{16}. 0π/2sin4xdx=3π16.\boxed{\int_0^{\pi/2}\sin^4 x\, dx = \frac{3\pi}{16}.}

(Equivalently, by Wallis' formula for even nn: 3142π2=3π16\dfrac{3\cdot 1}{4\cdot 2}\cdot\dfrac{\pi}{2} = \dfrac{3\pi}{16}.)

integration
9short5 marks

Solve the differential equation (\frac{dy}{dx} + y\tan x = \sec x).

Solve dydx+ytanx=secx\displaystyle\frac{dy}{dx} + y\tan x = \sec x

This is a linear first-order ODE dydx+P(x)y=Q(x)\dfrac{dy}{dx} + P(x)\,y = Q(x) with P=tanxP = \tan x, Q=secxQ = \sec x.

Integrating factor:

IF=ePdx=etanxdx=elnsecx=secx.\text{IF} = e^{\int P\, dx} = e^{\int \tan x\, dx} = e^{\ln|\sec x|} = \sec x.

Multiply through by the IF (or use ddx(yIF)=QIF\frac{d}{dx}(y\cdot\text{IF}) = Q\cdot\text{IF}):

ddx(ysecx)=secxsecx=sec2x.\frac{d}{dx}(y\sec x) = \sec x\cdot\sec x = \sec^2 x.

Integrate both sides:

ysecx=sec2xdx=tanx+C.y\sec x = \int \sec^2 x\, dx = \tan x + C.

General solution:

ysecx=tanx+C    y=sinx+Ccosx.y\sec x = \tan x + C \;\Longrightarrow\; \boxed{y = \sin x + C\cos x.}
differential-equations
10short5 marks

Find the angle between the vectors (\vec{a} = \hat{i} + 2\hat{j} + 3\hat{k}) and (\vec{b} = 3\hat{i} - 2\hat{j} + \hat{k}).

Angle between a=i^+2j^+3k^\vec a = \hat i + 2\hat j + 3\hat k and b=3i^2j^+k^\vec b = 3\hat i - 2\hat j + \hat k

Dot product:

ab=(1)(3)+(2)(2)+(3)(1)=34+3=2.\vec a\cdot\vec b = (1)(3) + (2)(-2) + (3)(1) = 3 - 4 + 3 = 2.

Magnitudes:

a=12+22+32=14,b=32+(2)2+12=14.|\vec a| = \sqrt{1^2 + 2^2 + 3^2} = \sqrt{14},\qquad |\vec b| = \sqrt{3^2 + (-2)^2 + 1^2} = \sqrt{14}.

Angle θ\theta from ab=abcosθ\vec a\cdot\vec b = |\vec a||\vec b|\cos\theta:

cosθ=abab=21414=214=17.\cos\theta = \frac{\vec a\cdot\vec b}{|\vec a||\vec b|} = \frac{2}{\sqrt{14}\cdot\sqrt{14}} = \frac{2}{14} = \frac{1}{7}. θ=cos1 ⁣(17)81.79.\boxed{\theta = \cos^{-1}\!\left(\frac{1}{7}\right) \approx 81.79^{\circ}.}
vectors
11short5 marks

If (u = x^2 + y^2), find (\frac{\partial u}{\partial x}) and (\frac{\partial u}{\partial y}).

Partial derivatives of u=x2+y2u = x^2 + y^2

With respect to xx (treat yy as constant):

ux=x(x2+y2)=2x+0=2x.\frac{\partial u}{\partial x} = \frac{\partial}{\partial x}(x^2 + y^2) = 2x + 0 = \boxed{2x.}

With respect to yy (treat xx as constant):

uy=y(x2+y2)=0+2y=2y.\frac{\partial u}{\partial y} = \frac{\partial}{\partial y}(x^2 + y^2) = 0 + 2y = \boxed{2y.}

Hence ux=2x\dfrac{\partial u}{\partial x} = 2x and uy=2y\dfrac{\partial u}{\partial y} = 2y.

partial-derivatives
12short5 marks

Evaluate the double integral (\int_0^1 \int_0^2 (x + y), dy, dx).

Evaluate 01 ⁣02(x+y)dydx\displaystyle\int_0^1\!\int_0^2 (x + y)\, dy\, dx

Inner integral (integrate w.r.t. yy from 00 to 22, xx constant):

02(x+y)dy=[xy+y22]02=2x+42=2x+2.\int_0^2 (x + y)\, dy = \left[xy + \frac{y^2}{2}\right]_0^2 = 2x + \frac{4}{2} = 2x + 2.

Outer integral (integrate w.r.t. xx from 00 to 11):

01(2x+2)dx=[x2+2x]01=1+2=3.\int_0^1 (2x + 2)\, dx = \left[x^2 + 2x\right]_0^1 = 1 + 2 = 3. 01 ⁣02(x+y)dydx=3.\boxed{\int_0^1\!\int_0^2 (x + y)\, dy\, dx = 3.}
multiple-integrals

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