Browse papers
A

Section A: Long Answer Questions

Attempt any TWO questions.

3 questions·10 marks each
1long10 marks

Define limit and continuity. Evaluate (\lim_{x \to 0}\frac{e^x - 1}{x}) and (\lim_{x \to 0}\frac{a^x - 1}{x}).

Definitions

Limit. A function f(x)f(x) has limit LL as xax \to a, written limxaf(x)=L\lim_{x\to a} f(x) = L, if for every ε>0\varepsilon > 0 there exists δ>0\delta > 0 such that 0<xa<δ    f(x)L<ε0 < |x - a| < \delta \implies |f(x) - L| < \varepsilon. Intuitively, f(x)f(x) can be made arbitrarily close to LL by taking xx sufficiently close (but not equal) to aa.

Continuity. A function ff is continuous at x=ax = a if:

  1. f(a)f(a) is defined,
  2. limxaf(x)\lim_{x\to a} f(x) exists, and
  3. limxaf(x)=f(a)\lim_{x\to a} f(x) = f(a).

A function is continuous on an interval if it is continuous at every point of the interval.

Evaluation 1: limx0ex1x\displaystyle\lim_{x\to 0}\frac{e^x - 1}{x}

Using the expansion ex=1+x+x22!+x33!+e^x = 1 + x + \dfrac{x^2}{2!} + \dfrac{x^3}{3!} + \cdots:

ex1x=x+x22!+x33!+x=1+x2!+x23!+\frac{e^x - 1}{x} = \frac{x + \frac{x^2}{2!} + \frac{x^3}{3!} + \cdots}{x} = 1 + \frac{x}{2!} + \frac{x^2}{3!} + \cdots

Taking x0x \to 0, all terms after the first vanish:

limx0ex1x=1.\boxed{\lim_{x\to 0}\frac{e^x - 1}{x} = 1.}

Evaluation 2: limx0ax1x\displaystyle\lim_{x\to 0}\frac{a^x - 1}{x} (a>0a>0)

Write ax=exlnaa^x = e^{x\ln a}. Put t=xlnat = x\ln a (so t0t\to 0 as x0x\to 0):

ax1x=exlna1x=lnaet1t.\frac{a^x - 1}{x} = \frac{e^{x\ln a} - 1}{x} = \ln a \cdot \frac{e^{t} - 1}{t}.

Using the previous result et1t1\dfrac{e^t-1}{t}\to 1:

limx0ax1x=lna.\boxed{\lim_{x\to 0}\frac{a^x - 1}{x} = \ln a.}

(As a check, putting a=ea = e gives lne=1\ln e = 1, consistent with the first limit.)

limits
2long10 marks

If (y = (\sin^{-1} x)^2), prove that ((1 - x^2)y_{n+2} - (2n+1)xy_{n+1} - n^2 y_n = 0).

To prove: (1x2)yn+2(2n+1)xyn+1n2yn=0(1-x^2)y_{n+2} - (2n+1)x\,y_{n+1} - n^2 y_n = 0, where y=(sin1x)2y = (\sin^{-1}x)^2.

Step 1 — First derivative.

y1=2sin1x11x2.y_1 = 2\sin^{-1}x \cdot \frac{1}{\sqrt{1-x^2}}.

Therefore 1x2y1=2sin1x\sqrt{1-x^2}\,y_1 = 2\sin^{-1}x, and squaring,

(1x2)y12=4(sin1x)2=4y.()(1-x^2)y_1^{\,2} = 4(\sin^{-1}x)^2 = 4y. \qquad (\ast)

Step 2 — Differentiate ()(\ast). Differentiating both sides with respect to xx:

(1x2)2y1y2+(2x)y12=4y1.(1-x^2)\cdot 2y_1 y_2 + (-2x)y_1^{\,2} = 4y_1.

Dividing throughout by 2y12y_1 (assuming y10y_1 \neq 0):

(1x2)y2xy1=2.()(1-x^2)y_2 - x\,y_1 = 2. \qquad (\ast\ast)

Step 3 — Apply Leibnitz's theorem. Differentiate ()(\ast\ast) nn times using Leibnitz's rule. For the product (1x2)y2(1-x^2)y_2:

Dn[(1x2)y2]=(1x2)yn+2+n(2x)yn+1+n(n1)2(2)yn.D^n\big[(1-x^2)y_2\big] = (1-x^2)y_{n+2} + n(-2x)y_{n+1} + \frac{n(n-1)}{2}(-2)y_n.

For the product xy1x\,y_1:

Dn[xy1]=xyn+1+nyn.D^n\big[x\,y_1\big] = x\,y_{n+1} + n\,y_n.

The right side 22 is constant, so its nn-th derivative (for n1n\ge 1) is 00.

Step 4 — Combine.

(1x2)yn+22nxyn+1n(n1)yn(xyn+1+nyn)=0.(1-x^2)y_{n+2} - 2nx\,y_{n+1} - n(n-1)y_n - \big(x\,y_{n+1} + n\,y_n\big) = 0.

Grouping like terms:

(1x2)yn+2(2n+1)xyn+1(n(n1)+n)yn=0.(1-x^2)y_{n+2} - (2n+1)x\,y_{n+1} - \big(n(n-1)+n\big)y_n = 0.

Since n(n1)+n=n2n(n-1)+n = n^2,

(1x2)yn+2(2n+1)xyn+1n2yn=0.\boxed{(1-x^2)y_{n+2} - (2n+1)x\,y_{n+1} - n^2 y_n = 0.}

Hence proved.

successive-differentiation
3long10 marks

Find the area enclosed between the curves (y = x^2) and (y = x).

Area enclosed between y=x2y = x^2 and y=xy = x.

Step 1 — Points of intersection. Set x2=xx2x=0x(x1)=0x^2 = x \Rightarrow x^2 - x = 0 \Rightarrow x(x-1)=0, so x=0x = 0 and x=1x = 1. The curves meet at (0,0)(0,0) and (1,1)(1,1).

Step 2 — Identify the upper curve. On 0<x<10 < x < 1, take x=12x = \tfrac12: line gives y=0.5y = 0.5, parabola gives y=0.25y = 0.25. So the line y=xy = x lies above the parabola y=x2y = x^2 on [0,1][0,1].

Step 3 — Set up the integral.

A=01(xx2)dx.A = \int_0^1 \big(x - x^2\big)\,dx.

Step 4 — Integrate.

A=[x22x33]01=1213=326=16.A = \left[\frac{x^2}{2} - \frac{x^3}{3}\right]_0^1 = \frac{1}{2} - \frac{1}{3} = \frac{3-2}{6} = \frac{1}{6}. A=16 square units.\boxed{A = \frac{1}{6}\ \text{square units}.}
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 3x}{\sin 5x}).

Use sinθθ1\dfrac{\sin\theta}{\theta}\to 1 as θ0\theta\to 0. Multiply and divide to introduce the angles:

sin3xsin5x=sin3x3x3xsin5x5x5x=sin3x3xsin5x5x3x5x.\frac{\sin 3x}{\sin 5x} = \frac{\dfrac{\sin 3x}{3x}\cdot 3x}{\dfrac{\sin 5x}{5x}\cdot 5x} = \frac{\dfrac{\sin 3x}{3x}}{\dfrac{\sin 5x}{5x}}\cdot\frac{3x}{5x}.

As x0x\to 0, both fractions tend to 11, leaving

limx0sin3xsin5x=1135=35.\lim_{x\to 0}\frac{\sin 3x}{\sin 5x} = 1\cdot 1\cdot\frac{3}{5} = \boxed{\dfrac{3}{5}}.
limits
5short5 marks

Differentiate (\tan^{-1}\left(\frac{2x}{1 - x^2}\right)) with respect to x.

Let y=tan1 ⁣(2x1x2)y = \tan^{-1}\!\left(\dfrac{2x}{1-x^2}\right). Substitute x=tanθx = \tan\theta, so θ=tan1x\theta = \tan^{-1}x. Then

2x1x2=2tanθ1tan2θ=tan2θ.\frac{2x}{1-x^2} = \frac{2\tan\theta}{1-\tan^2\theta} = \tan 2\theta.

Hence

y=tan1(tan2θ)=2θ=2tan1xy = \tan^{-1}(\tan 2\theta) = 2\theta = 2\tan^{-1}x

(valid for 1<x<1-1 < x < 1). Differentiating,

dydx=211+x2=21+x2.\frac{dy}{dx} = 2\cdot\frac{1}{1+x^2} = \boxed{\dfrac{2}{1+x^2}}.
differentiation
6short5 marks

State and verify Rolle's theorem for (f(x) = \sin x) on ([0, \pi]).

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)=sinxf(x) = \sin x on [0,π][0,\pi]

  • Continuity: sinx\sin x is continuous everywhere, hence on [0,π][0,\pi]. ✓
  • Differentiability: sinx\sin x is differentiable everywhere, hence on (0,π)(0,\pi). ✓
  • Equal endpoints: f(0)=sin0=0f(0) = \sin 0 = 0 and f(π)=sinπ=0f(\pi) = \sin\pi = 0, so f(0)=f(π)f(0)=f(\pi). ✓

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

f(x)=cosx=0    x=π2.f'(x) = \cos x = 0 \implies x = \frac{\pi}{2}.

Since c=π2(0,π)c = \dfrac{\pi}{2}\in(0,\pi), the theorem is verified. \blacksquare

mean-value-theorem
7short5 marks

Find the points of inflection of (y = x^3 - 6x^2 + 9x).

For y=x36x2+9xy = x^3 - 6x^2 + 9x:

y=3x212x+9,y=6x12.y' = 3x^2 - 12x + 9,\qquad y'' = 6x - 12.

Set y=0y'' = 0: 6x12=0x=26x - 12 = 0 \Rightarrow x = 2.

Check sign change of yy'': for x<2x<2, y<0y''<0 (concave down); for x>2x>2, y>0y''>0 (concave up). Concavity changes, so x=2x = 2 is a genuine point of inflection.

Find yy at x=2x = 2: y=824+18=2y = 8 - 24 + 18 = 2.

Point of inflection: (2,2).\boxed{\text{Point of inflection: } (2,\,2).}
applications-of-derivatives
8short5 marks

Evaluate (\int_0^{\pi/2} \cos^6 x , dx).

Use the Wallis reduction formula for 0π/2cosnxdx\displaystyle\int_0^{\pi/2}\cos^n x\,dx with even nn:

0π/2cosnxdx=(n1)(n3)1n(n2)2π2.\int_0^{\pi/2}\cos^n x\,dx = \frac{(n-1)(n-3)\cdots 1}{n(n-2)\cdots 2}\cdot\frac{\pi}{2}.

For n=6n = 6:

0π/2cos6xdx=531642π2=1548π2=516π2.\int_0^{\pi/2}\cos^6 x\,dx = \frac{5\cdot 3\cdot 1}{6\cdot 4\cdot 2}\cdot\frac{\pi}{2} = \frac{15}{48}\cdot\frac{\pi}{2} = \frac{5}{16}\cdot\frac{\pi}{2}. 0π/2cos6xdx=5π32.\boxed{\int_0^{\pi/2}\cos^6 x\,dx = \dfrac{5\pi}{32}.}
integration
9short5 marks

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

This is a linear first-order ODE dydx+P(x)y=Q(x)\dfrac{dy}{dx} + P(x)y = Q(x) with P=2xP = 2x, Q=xQ = x.

Integrating factor:

IF=e2xdx=ex2.\text{IF} = e^{\int 2x\,dx} = e^{x^2}.

Multiply through and integrate:

ddx(yex2)=xex2.\frac{d}{dx}\big(y\,e^{x^2}\big) = x\,e^{x^2}.

Integrate the right side with u=x2u = x^2, du=2xdxdu = 2x\,dx:

yex2=xex2dx=12ex2+C.y\,e^{x^2} = \int x e^{x^2}\,dx = \frac{1}{2}e^{x^2} + C.

Solve for yy:

y=12+Cex2.\boxed{y = \frac{1}{2} + C\,e^{-x^2}.}
differential-equations
10short5 marks

Find the projection of (\vec{a} = \hat{i} + 2\hat{j} - \hat{k}) on (\vec{b} = 2\hat{i} - \hat{j} + 3\hat{k}).

The (scalar) projection of a\vec a on b\vec b is abb\dfrac{\vec a\cdot\vec b}{|\vec b|}.

Dot product:

ab=(1)(2)+(2)(1)+(1)(3)=223=3.\vec a\cdot\vec b = (1)(2) + (2)(-1) + (-1)(3) = 2 - 2 - 3 = -3.

Magnitude of b\vec b:

b=22+(1)2+32=4+1+9=14.|\vec b| = \sqrt{2^2 + (-1)^2 + 3^2} = \sqrt{4+1+9} = \sqrt{14}.

Projection:

proj=abb=314=3140.802.\boxed{\text{proj} = \frac{\vec a\cdot\vec b}{|\vec b|} = \frac{-3}{\sqrt{14}} = -\frac{3}{\sqrt{14}}\approx -0.802.}

The negative sign indicates the projection is directed opposite to b\vec b.

vectors
11short5 marks

If (z = f(x/y)), show that (x\frac{\partial z}{\partial x} + y\frac{\partial z}{\partial y} = 0).

Let z=f(u)z = f(u) where u=xyu = \dfrac{x}{y}. By the chain rule:

zx=f(u)ux=f(u)1y,\frac{\partial z}{\partial x} = f'(u)\,\frac{\partial u}{\partial x} = f'(u)\cdot\frac{1}{y}, zy=f(u)uy=f(u)(xy2).\frac{\partial z}{\partial y} = f'(u)\,\frac{\partial u}{\partial y} = f'(u)\cdot\left(-\frac{x}{y^2}\right).

Now form the required combination:

xzx+yzy=xf(u)y+y(xf(u)y2)=xf(u)yxf(u)y=0.x\frac{\partial z}{\partial x} + y\frac{\partial z}{\partial y} = x\cdot\frac{f'(u)}{y} + y\cdot\left(-\frac{x f'(u)}{y^2}\right) = \frac{x f'(u)}{y} - \frac{x f'(u)}{y} = 0. xzx+yzy=0.\boxed{x\frac{\partial z}{\partial x} + y\frac{\partial z}{\partial y} = 0.}

Hence proved. (This is consistent with Euler's theorem, since f(x/y)f(x/y) is a homogeneous function of degree 00.)

partial-derivatives
12short5 marks

Evaluate (\int_0^a \int_0^b xy , dx , dy).

Evaluate the double integral (the limits are constants, so the order is immaterial):

I=0a0bxydxdy.I = \int_0^a\int_0^b xy\,dx\,dy.

Inner integral (over xx):

0bxydx=y[x22]0b=b2y2.\int_0^b xy\,dx = y\left[\frac{x^2}{2}\right]_0^b = \frac{b^2 y}{2}.

Outer integral (over yy):

I=0ab2y2dy=b22[y22]0a=b22a22.I = \int_0^a \frac{b^2 y}{2}\,dy = \frac{b^2}{2}\left[\frac{y^2}{2}\right]_0^a = \frac{b^2}{2}\cdot\frac{a^2}{2}. I=a2b24.\boxed{I = \frac{a^2 b^2}{4}.}
multiple-integrals

Frequently asked questions

Where can I find the BSc CSIT (TU) Mathematics I (BSc CSIT, MTH112) question paper 2078?
The full BSc CSIT (TU) Mathematics I (BSc CSIT, MTH112) 2078 (regular) question paper is available free on Kekkei. You can read every question online and attempt the paper under timed exam conditions.
Does the Mathematics I (BSc CSIT, MTH112) 2078 paper come with solutions?
Yes. Every question on this Mathematics I (BSc CSIT, MTH112) past paper includes a step-by-step solution, plus instant AI feedback when you attempt it on Kekkei.
How many marks is the BSc CSIT (TU) Mathematics I (BSc CSIT, MTH112) 2078 paper?
The BSc CSIT (TU) Mathematics I (BSc CSIT, MTH112) 2078 paper carries 60 full marks and is meant to be completed in 180 minutes, across 12 questions.
Is practising this Mathematics I (BSc CSIT, MTH112) past paper free?
Yes — reading and attempting this Mathematics I (BSc CSIT, MTH112) past paper on Kekkei is completely free.