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Section A: Long Answer Questions

Attempt all questions.

5 questions
1long10 marks

Solve the following system of linear equations by the matrix-inverse method (find A1A^{-1} using the adjoint and then compute X=A1BX = A^{-1}B):

x+2y+3z=62x+4y+5z=133x+5y+6z=18\begin{aligned} x + 2y + 3z &= 6 \\ 2x + 4y + 5z &= 13 \\ 3x + 5y + 6z &= 18 \end{aligned}

State clearly the condition under which this method is applicable and verify your solution.

Step 1 — Write in matrix form AX=BAX=B.

A=(123245356),X=(xyz),B=(61318).A=\begin{pmatrix}1&2&3\\2&4&5\\3&5&6\end{pmatrix},\quad X=\begin{pmatrix}x\\y\\z\end{pmatrix},\quad B=\begin{pmatrix}6\\13\\18\end{pmatrix}.

Step 2 — Condition for applicability. The inverse method requires detA0\det A \ne 0 (i.e. AA is non-singular), so that a unique solution exists.

Step 3 — Compute detA\det A. Expand along the first row:

detA=1(4655)2(2653)+3(2543)\det A = 1(4\cdot 6-5\cdot5) - 2(2\cdot6-5\cdot3) + 3(2\cdot5-4\cdot3) =1(2425)2(1215)+3(1012)=1(1)2(3)+3(2)=1+66=1.= 1(24-25) - 2(12-15) + 3(10-12) = 1(-1) - 2(-3) + 3(-2) = -1+6-6 = -1.

Since detA=10\det A = -1 \ne 0, the method applies.

Step 4 — Cofactor matrix.

C11=+(2425)=1,C12=(1215)=3,C13=+(1012)=2,C21=(1215)=3,C22=+(69)=3,C23=(56)=1,C31=+(1012)=2,C32=(56)=1,C33=+(44)=0.\begin{aligned} C_{11}&=+(24-25)=-1, & C_{12}&=-(12-15)=3, & C_{13}&=+(10-12)=-2,\\ C_{21}&=-(12-15)=3, & C_{22}&=+(6-9)=-3, & C_{23}&=-(5-6)=1,\\ C_{31}&=+(10-12)=-2, & C_{32}&=-(5-6)=1, & C_{33}&=+(4-4)=0. \end{aligned}

Step 5 — Adjoint (transpose of cofactor matrix).

adjA=(132331210).\operatorname{adj}A=\begin{pmatrix}-1&3&-2\\3&-3&1\\-2&1&0\end{pmatrix}.

Step 6 — Inverse.

A1=1detAadjA=11(132331210)=(132331210).A^{-1}=\frac{1}{\det A}\operatorname{adj}A=\frac{1}{-1}\begin{pmatrix}-1&3&-2\\3&-3&1\\-2&1&0\end{pmatrix}=\begin{pmatrix}1&-3&2\\-3&3&-1\\2&-1&0\end{pmatrix}.

Step 7 — Solve X=A1BX=A^{-1}B.

x=1(6)+(3)(13)+2(18)=639+36=3,y=(3)(6)+3(13)+(1)(18)=18+3918=3,z=2(6)+(1)(13)+0(18)=1213+0=1.\begin{aligned} x&=1(6)+(-3)(13)+2(18)=6-39+36=3,\\ y&=(-3)(6)+3(13)+(-1)(18)=-18+39-18=3,\\ z&=2(6)+(-1)(13)+0(18)=12-13+0=-1. \end{aligned}

Step 8 — Verify in the original equations.

  • Eq.1: 3+2(3)+3(1)=3+63=63+2(3)+3(-1)=3+6-3=6
  • Eq.2: 2(3)+4(3)+5(1)=6+125=132(3)+4(3)+5(-1)=6+12-5=13
  • Eq.3: 3(3)+5(3)+6(1)=9+156=183(3)+5(3)+6(-1)=9+15-6=18

Final answer: x=3,  y=3,  z=1\boxed{x=3,\; y=3,\; z=-1}.

determinantsmatriceslinear-systems
2long8 marks

Find the equation of the plane passing through the line of intersection of the planes

2xy+3z1=0andx+2yz+2=0,2x - y + 3z - 1 = 0 \quad\text{and}\quad x + 2y - z + 2 = 0,

and which is perpendicular to the plane 3x4yz+6=03x - 4y - z + 6 = 0.

Step 1 — Family of planes through the line of intersection. Any plane through the intersection of the two given planes is

(2xy+3z1)+λ(x+2yz+2)=0.(2x - y + 3z - 1) + \lambda (x + 2y - z + 2) = 0.

Group terms:

(2+λ)x+(1+2λ)y+(3λ)z+(1+2λ)=0.(2+\lambda)x + (-1+2\lambda)y + (3-\lambda)z + (-1+2\lambda) = 0.

Its normal vector is n=(2+λ,  1+2λ,  3λ).\vec{n}=\big(2+\lambda,\; -1+2\lambda,\; 3-\lambda\big).

Step 2 — Perpendicularity condition. Two planes are perpendicular when their normals are orthogonal. The normal of 3x4yz+6=03x-4y-z+6=0 is m=(3,4,1)\vec{m}=(3,-4,-1). Require nm=0\vec{n}\cdot\vec{m}=0:

3(2+λ)4(1+2λ)1(3λ)=0.3(2+\lambda) - 4(-1+2\lambda) - 1(3-\lambda) = 0. 6+3λ+48λ3+λ=0    (6+43)+(38+1)λ=0    74λ=0.6+3\lambda + 4 - 8\lambda - 3 + \lambda = 0 \;\Rightarrow\; (6+4-3) + (3-8+1)\lambda = 0 \;\Rightarrow\; 7 - 4\lambda = 0.

Hence λ=74.\lambda = \dfrac{7}{4}.

Step 3 — Substitute λ=7/4\lambda=7/4. Multiply the family equation through by 44 for convenience, with 4λ=74\lambda = 7:

(8+7)x+(4+14)y+(127)z+(4+14)=0(8+7)x + (-4+14)y + (12-7)z + (-4+14) = 0 15x+10y+5z+10=0.15x + 10y + 5z + 10 = 0.

Divide by 55:

3x+2y+z+2=0.\boxed{3x + 2y + z + 2 = 0.}

Step 4 — Verification of perpendicularity. Normal of the answer is (3,2,1)(3,2,1); dot with (3,4,1)(3,-4,-1) gives 981=09-8-1=0 ✓. The plane also belongs to the family, so it contains the line of intersection.

3d-geometryplaneline
3long8 marks

Solve the differential equation

d2ydx23dydx+2y=e3x+sinx.\frac{d^2y}{dx^2} - 3\frac{dy}{dx} + 2y = e^{3x} + \sin x.

Step 1 — Complementary function (CF). Auxiliary equation: m23m+2=0(m1)(m2)=0m=1,2.m^2 - 3m + 2 = 0 \Rightarrow (m-1)(m-2)=0 \Rightarrow m=1,2.

yc=C1ex+C2e2x.y_c = C_1 e^{x} + C_2 e^{2x}.

Step 2 — Particular integral for e3xe^{3x}. Using 1f(D)eax=1f(a)eax\dfrac{1}{f(D)}e^{ax}=\dfrac{1}{f(a)}e^{ax} with f(D)=D23D+2f(D)=D^2-3D+2 and a=3a=3:

f(3)=99+2=20yp1=12e3x.f(3)=9-9+2=2 \ne 0 \Rightarrow y_{p1}=\frac{1}{2}e^{3x}.

Step 3 — Particular integral for sinx\sin x. Replace D21D^2\to -1 in f(D)f(D):

yp2=1D23D+2sinx=1(1)3D+2sinx=113Dsinx.y_{p2}=\frac{1}{D^2-3D+2}\sin x = \frac{1}{(-1)-3D+2}\sin x = \frac{1}{1-3D}\sin x.

Rationalise by multiplying numerator and denominator by (1+3D)(1+3D):

yp2=1+3D19D2sinx=1+3D19(1)sinx=1+3D10sinx.y_{p2}=\frac{1+3D}{1-9D^2}\sin x = \frac{1+3D}{1-9(-1)}\sin x = \frac{1+3D}{10}\sin x.

Now Dsinx=cosxD\sin x=\cos x, so

yp2=sinx+3cosx10.y_{p2}=\frac{\sin x + 3\cos x}{10}.

Step 4 — General solution.

y=C1ex+C2e2x+12e3x+110(sinx+3cosx).\boxed{y = C_1 e^{x} + C_2 e^{2x} + \tfrac{1}{2}e^{3x} + \tfrac{1}{10}\big(\sin x + 3\cos x\big).}

Check (PI for e3xe^{3x}): if y=12e3xy=\tfrac12 e^{3x} then y3y+2y=12(99+2)e3x=e3xy''-3y'+2y=\tfrac12(9-9+2)e^{3x}=e^{3x} ✓.

second-order-odeundetermined-coefficients
4long8 marks

Obtain the Fourier series expansion of the function

f(x)=x2,π<x<π,f(x) = x^2, \qquad -\pi < x < \pi,

of period 2π2\pi. Hence deduce that n=11n2=π26.\displaystyle\sum_{n=1}^{\infty}\frac{1}{n^2} = \frac{\pi^2}{6}.

Step 1 — Note symmetry. f(x)=x2f(x)=x^2 is even on (π,π)(-\pi,\pi), so all sine coefficients bn=0b_n=0.

Step 2 — Constant term a0a_0.

a0=1πππx2dx=2π0πx2dx=2ππ33=2π23.a_0=\frac{1}{\pi}\int_{-\pi}^{\pi}x^2\,dx=\frac{2}{\pi}\int_{0}^{\pi}x^2\,dx=\frac{2}{\pi}\cdot\frac{\pi^3}{3}=\frac{2\pi^2}{3}.

Step 3 — Cosine coefficients ana_n.

an=1πππx2cosnxdx=2π0πx2cosnxdx.a_n=\frac{1}{\pi}\int_{-\pi}^{\pi}x^2\cos nx\,dx=\frac{2}{\pi}\int_{0}^{\pi}x^2\cos nx\,dx.

Integrate by parts twice:

x2cosnxdx=x2sinnxn+2xcosnxn22sinnxn3.\int x^2\cos nx\,dx = \frac{x^2\sin nx}{n} + \frac{2x\cos nx}{n^2} - \frac{2\sin nx}{n^3}.

Evaluate from 00 to π\pi. At x=πx=\pi: sinnπ=0\sin n\pi=0, cosnπ=(1)n\cos n\pi=(-1)^n. At x=0x=0 all terms vanish.

0πx2cosnxdx=0+2π(1)nn20=2π(1)nn2.\int_{0}^{\pi}x^2\cos nx\,dx = 0 + \frac{2\pi(-1)^n}{n^2} - 0 = \frac{2\pi(-1)^n}{n^2}.

Therefore

an=2π2π(1)nn2=4(1)nn2.a_n=\frac{2}{\pi}\cdot\frac{2\pi(-1)^n}{n^2}=\frac{4(-1)^n}{n^2}.

Step 4 — Fourier series. With f(x)=a02+ancosnxf(x)=\dfrac{a_0}{2}+\sum a_n\cos nx:

x2=π23+4n=1(1)nn2cosnx,π<x<π.\boxed{x^2 = \frac{\pi^2}{3} + 4\sum_{n=1}^{\infty}\frac{(-1)^n}{n^2}\cos nx,\qquad -\pi<x<\pi.}

Step 5 — Deduction. Put x=πx=\pi (a point where the periodic extension is continuous, value π2\pi^2; here cosnπ=(1)n\cos n\pi=(-1)^n so (1)ncosnπ=1(-1)^n\cos n\pi=1):

π2=π23+4n=1(1)n(1)nn2=π23+4n=11n2.\pi^2 = \frac{\pi^2}{3} + 4\sum_{n=1}^{\infty}\frac{(-1)^n(-1)^n}{n^2} = \frac{\pi^2}{3} + 4\sum_{n=1}^{\infty}\frac{1}{n^2}.

So 41n2=π2π23=2π234\sum \frac{1}{n^2} = \pi^2 - \frac{\pi^2}{3} = \frac{2\pi^2}{3}, giving

n=11n2=2π2314=π26.\sum_{n=1}^{\infty}\frac{1}{n^2} = \frac{2\pi^2}{3}\cdot\frac{1}{4} = \boxed{\frac{\pi^2}{6}.}
fourier-seriesperiodic-functions
5long8 marks

Test the convergence of the following series:

(a) n=1n!nn\displaystyle\sum_{n=1}^{\infty}\frac{n!}{n^n}

(b) n=1n22n\displaystyle\sum_{n=1}^{\infty}\frac{n^2}{2^n}

(c) n=11n2+1\displaystyle\sum_{n=1}^{\infty}\frac{1}{n^2+1}

(a) n!nn\sum \dfrac{n!}{n^n} — Ratio test. Let un=n!nnu_n=\dfrac{n!}{n^n}. Then

un+1un=(n+1)!(n+1)n+1nnn!=(n+1)nn(n+1)n+1=nn(n+1)n=(nn+1)n=1(1+1n)n.\frac{u_{n+1}}{u_n}=\frac{(n+1)!}{(n+1)^{n+1}}\cdot\frac{n^n}{n!}=\frac{(n+1)\,n^n}{(n+1)^{n+1}}=\frac{n^n}{(n+1)^n}=\left(\frac{n}{n+1}\right)^n=\frac{1}{\left(1+\frac1n\right)^n}. limnun+1un=1e0.368<1.\lim_{n\to\infty}\frac{u_{n+1}}{u_n}=\frac{1}{e}\approx 0.368 < 1.

By the ratio test the series converges.

(b) n22n\sum \dfrac{n^2}{2^n} — Ratio test.

un+1un=(n+1)22n+12nn2=12(n+1n)2.\frac{u_{n+1}}{u_n}=\frac{(n+1)^2}{2^{n+1}}\cdot\frac{2^n}{n^2}=\frac{1}{2}\left(\frac{n+1}{n}\right)^2. limnun+1un=121=12<1.\lim_{n\to\infty}\frac{u_{n+1}}{u_n}=\frac12 \cdot 1 = \frac12 < 1.

Hence the series converges.

(c) 1n2+1\sum \dfrac{1}{n^2+1} — Comparison test. For all n1n\ge 1,   n2+1>n2\;n^2+1 > n^2, so 1n2+1<1n2\dfrac{1}{n^2+1} < \dfrac{1}{n^2}. The pp-series 1n2\sum \dfrac{1}{n^2} converges (p=2>1p=2>1). By the comparison test, the smaller-term series 1n2+1\sum \dfrac{1}{n^2+1} also converges.

Summary: all three series converge.

infinite-seriesconvergence-tests
B

Section B: Short Answer Questions

Attempt all questions.

6 questions
6short6 marks

Find the rank of the matrix by reducing it to echelon form:

A=(1230243232136875).A=\begin{pmatrix}1 & 2 & 3 & 0 \\ 2 & 4 & 3 & 2 \\ 3 & 2 & 1 & 3 \\ 6 & 8 & 7 & 5\end{pmatrix}.

Step 1 — Row operations. R2R22R1,  R3R33R1,  R4R46R1R_2\to R_2-2R_1,\; R_3\to R_3-3R_1,\; R_4\to R_4-6R_1:

(12300032048304115).\begin{pmatrix}1&2&3&0\\0&0&-3&2\\0&-4&-8&3\\0&-4&-11&5\end{pmatrix}.

Step 2 — Swap R2R3R_2\leftrightarrow R_3 to bring a pivot into column 2:

(12300483003204115).\begin{pmatrix}1&2&3&0\\0&-4&-8&3\\0&0&-3&2\\0&-4&-11&5\end{pmatrix}.

Step 3 — R4R4R2R_4\to R_4-R_2:

(1230048300320032).\begin{pmatrix}1&2&3&0\\0&-4&-8&3\\0&0&-3&2\\0&0&-3&2\end{pmatrix}.

Step 4 — R4R4R3R_4\to R_4-R_3:

(1230048300320000).\begin{pmatrix}1&2&3&0\\0&-4&-8&3\\0&0&-3&2\\0&0&0&0\end{pmatrix}.

Step 5 — Count non-zero rows. There are 3 non-zero rows.

rank(A)=3.\boxed{\operatorname{rank}(A)=3.}
matricesrankechelon-form
7short6 marks

Find the shortest distance between the two skew lines

x12=y23=z34andx23=y44=z55.\frac{x-1}{2}=\frac{y-2}{3}=\frac{z-3}{4} \quad\text{and}\quad \frac{x-2}{3}=\frac{y-4}{4}=\frac{z-5}{5}.

Step 1 — Identify points and direction vectors. Line 1: point A=(1,2,3)A=(1,2,3), direction b1=(2,3,4)\vec{b_1}=(2,3,4). Line 2: point C=(2,4,5)C=(2,4,5), direction b2=(3,4,5)\vec{b_2}=(3,4,5).

AC=CA=(1,2,2).\vec{AC}=C-A=(1,2,2).

Step 2 — Cross product b1×b2\vec{b_1}\times\vec{b_2}.

b1×b2=ijk234345=i(3544)j(2543)+k(2433).\vec{b_1}\times\vec{b_2}=\begin{vmatrix}\mathbf{i}&\mathbf{j}&\mathbf{k}\\2&3&4\\3&4&5\end{vmatrix}=\mathbf{i}(3\cdot5-4\cdot4)-\mathbf{j}(2\cdot5-4\cdot3)+\mathbf{k}(2\cdot4-3\cdot3). =i(1516)j(1012)+k(89)=(1,2,1).=\mathbf{i}(15-16)-\mathbf{j}(10-12)+\mathbf{k}(8-9)=(-1,\,2,\,-1).

Magnitude: b1×b2=(1)2+22+(1)2=1+4+1=6.|\vec{b_1}\times\vec{b_2}|=\sqrt{(-1)^2+2^2+(-1)^2}=\sqrt{1+4+1}=\sqrt6.

Step 3 — Scalar triple product AC(b1×b2)\vec{AC}\cdot(\vec{b_1}\times\vec{b_2}).

(1,2,2)(1,2,1)=1(1)+2(2)+2(1)=1+42=1.(1,2,2)\cdot(-1,2,-1)=1(-1)+2(2)+2(-1)=-1+4-2=1.

Step 4 — Shortest distance.

d=AC(b1×b2)b1×b2=16=16.d=\frac{|\vec{AC}\cdot(\vec{b_1}\times\vec{b_2})|}{|\vec{b_1}\times\vec{b_2}|}=\frac{|1|}{\sqrt6}=\frac{1}{\sqrt6}. d=160.408 units.\boxed{d=\dfrac{1}{\sqrt6}\approx 0.408\text{ units}.}
3d-geometryshortest-distanceskew-lines
8short6 marks

Solve the Cauchy-Euler equation

x2d2ydx22xdydx4y=x4.x^2\frac{d^2y}{dx^2} - 2x\frac{dy}{dx} - 4y = x^4.

Step 1 — Substitute x=etx=e^t (so t=lnxt=\ln x). With θ=ddt\theta=\dfrac{d}{dt}: xdydx=θyx\dfrac{dy}{dx}=\theta y and x2d2ydx2=θ(θ1)yx^2\dfrac{d^2y}{dx^2}=\theta(\theta-1)y. The equation becomes

θ(θ1)y2θy4y=e4t,\theta(\theta-1)y - 2\theta y - 4y = e^{4t}, [θ2θ2θ4]y=e4t    (θ23θ4)y=e4t.\big[\theta^2 - \theta - 2\theta - 4\big]y = e^{4t} \;\Rightarrow\; (\theta^2 - 3\theta - 4)y = e^{4t}.

Step 2 — Complementary function. Auxiliary: m23m4=0(m4)(m+1)=0m=4,1.m^2-3m-4=0 \Rightarrow (m-4)(m+1)=0 \Rightarrow m=4,-1.

yc=C1e4t+C2et=C1x4+C2x1.y_c = C_1 e^{4t} + C_2 e^{-t} = C_1 x^4 + C_2 x^{-1}.

Step 3 — Particular integral.

yp=1θ23θ4e4t.y_p=\frac{1}{\theta^2-3\theta-4}e^{4t}.

Since θ=4\theta=4 makes the denominator zero (it is a root), use the standard rule 1f(θ)eat=tf(a)eat\dfrac{1}{f(\theta)}e^{at}=\dfrac{t}{f'(a)}e^{at} when f(a)=0f(a)=0. Here f(θ)=2θ3f'(\theta)=2\theta-3, so f(4)=83=5f'(4)=8-3=5:

yp=t5e4t=lnx5x4.y_p=\frac{t}{5}e^{4t}=\frac{\ln x}{5}x^4.

Step 4 — General solution.

y=C1x4+C2x+x4lnx5.\boxed{y = C_1 x^4 + \frac{C_2}{x} + \frac{x^4\ln x}{5}.}
higher-order-odecauchy-euler
9short6 marks

Find the interval of convergence of the power series

n=1(x2)nn3n.\sum_{n=1}^{\infty}\frac{(x-2)^n}{n\,3^n}.

Step 1 — Apply the ratio test. Let un=(x2)nn3nu_n=\dfrac{(x-2)^n}{n\,3^n}. Then

un+1un=(x2)n+1(n+1)3n+1n3n(x2)n=nn+1x23.\left|\frac{u_{n+1}}{u_n}\right|=\left|\frac{(x-2)^{n+1}}{(n+1)3^{n+1}}\cdot\frac{n\,3^n}{(x-2)^n}\right|=\frac{n}{n+1}\cdot\frac{|x-2|}{3}. limnun+1un=x23.\lim_{n\to\infty}\left|\frac{u_{n+1}}{u_n}\right|=\frac{|x-2|}{3}.

For convergence this limit must be <1<1:

x23<1    x2<3    1<x<5.\frac{|x-2|}{3}<1 \;\Rightarrow\; |x-2|<3 \;\Rightarrow\; -1 < x < 5.

Radius of convergence R=3R=3, centred at x=2x=2.

Step 2 — Test endpoints.

At x=5x=5: series becomes 3nn3n=1n\displaystyle\sum \frac{3^n}{n\,3^n}=\sum\frac{1}{n}, the harmonic series, which diverges.

At x=1x=-1: series becomes (3)nn3n=(1)nn\displaystyle\sum \frac{(-3)^n}{n\,3^n}=\sum\frac{(-1)^n}{n}, the alternating harmonic series, which converges (by the Leibniz test).

Step 3 — Interval of convergence.

1x<5,i.e. [1,5).\boxed{-1 \le x < 5,\quad\text{i.e. } [-1,\,5).}
infinite-seriespower-seriesradius-of-convergence
10short6 marks

Find the half-range sine series of f(x)=xf(x)=x in the interval 0<x<π0 < x < \pi.

Step 1 — Form of half-range sine series. On (0,π)(0,\pi) the half-range sine series is

f(x)=n=1bnsinnx,bn=2π0πf(x)sinnxdx.f(x)=\sum_{n=1}^{\infty}b_n\sin nx,\qquad b_n=\frac{2}{\pi}\int_{0}^{\pi}f(x)\sin nx\,dx.

Step 2 — Compute bnb_n for f(x)=xf(x)=x.

bn=2π0πxsinnxdx.b_n=\frac{2}{\pi}\int_{0}^{\pi}x\sin nx\,dx.

Integration by parts (u=x,  dv=sinnxdxu=x,\;dv=\sin nx\,dx):

xsinnxdx=xcosnxn+sinnxn2.\int x\sin nx\,dx = -\frac{x\cos nx}{n} + \frac{\sin nx}{n^2}.

Evaluate from 00 to π\pi. At x=πx=\pi: cosnπ=(1)n\cos n\pi=(-1)^n, sinnπ=0\sin n\pi=0. At x=0x=0: both terms vanish.

0πxsinnxdx=π(1)nn+0=π(1)n+1n.\int_{0}^{\pi}x\sin nx\,dx = -\frac{\pi(-1)^n}{n} + 0 = \frac{\pi(-1)^{n+1}}{n}.

Therefore

bn=2ππ(1)n+1n=2(1)n+1n.b_n=\frac{2}{\pi}\cdot\frac{\pi(-1)^{n+1}}{n}=\frac{2(-1)^{n+1}}{n}.

Step 3 — Series.

x=2n=1(1)n+1nsinnx=2(sinxsin2x2+sin3x3),0<x<π.\boxed{x = 2\sum_{n=1}^{\infty}\frac{(-1)^{n+1}}{n}\sin nx = 2\left(\sin x - \frac{\sin 2x}{2} + \frac{\sin 3x}{3} - \cdots\right),\quad 0<x<\pi.}
fourier-serieshalf-rangesine-series
11short8 marks

Find the eigenvalues and the corresponding eigenvectors of the matrix

A=(4123).A=\begin{pmatrix}4 & 1 \\ 2 & 3\end{pmatrix}.

Step 1 — Characteristic equation det(AλI)=0\det(A-\lambda I)=0.

det(4λ123λ)=(4λ)(3λ)(1)(2)=0.\det\begin{pmatrix}4-\lambda & 1\\ 2 & 3-\lambda\end{pmatrix}=(4-\lambda)(3-\lambda)-(1)(2)=0. λ27λ+122=0    λ27λ+10=0.\lambda^2 - 7\lambda + 12 - 2 = 0 \;\Rightarrow\; \lambda^2 - 7\lambda + 10 = 0. (λ5)(λ2)=0    λ1=5,  λ2=2.(\lambda-5)(\lambda-2)=0 \;\Rightarrow\; \lambda_1=5,\;\lambda_2=2.

Step 2 — Eigenvector for λ1=5\lambda_1=5. Solve (A5I)v=0(A-5I)v=0:

(1122)(xy)=0    x+y=0    y=x.\begin{pmatrix}-1 & 1\\ 2 & -2\end{pmatrix}\begin{pmatrix}x\\y\end{pmatrix}=0 \;\Rightarrow\; -x+y=0 \;\Rightarrow\; y=x.

Taking x=1x=1: v1=(11).v_1=\begin{pmatrix}1\\1\end{pmatrix}.

Step 3 — Eigenvector for λ2=2\lambda_2=2. Solve (A2I)v=0(A-2I)v=0:

(2121)(xy)=0    2x+y=0    y=2x.\begin{pmatrix}2 & 1\\ 2 & 1\end{pmatrix}\begin{pmatrix}x\\y\end{pmatrix}=0 \;\Rightarrow\; 2x+y=0 \;\Rightarrow\; y=-2x.

Taking x=1x=1: v2=(12).v_2=\begin{pmatrix}1\\-2\end{pmatrix}.

Step 4 — Result.

λ1=5,  v1=(11);λ2=2,  v2=(12).\boxed{\lambda_1=5,\;v_1=\begin{pmatrix}1\\1\end{pmatrix};\qquad \lambda_2=2,\;v_2=\begin{pmatrix}1\\-2\end{pmatrix}.}

Check (λ=5\lambda=5): Av1=(4+12+3)=(55)=5v1Av_1=\begin{pmatrix}4+1\\2+3\end{pmatrix}=\begin{pmatrix}5\\5\end{pmatrix}=5v_1 ✓.

determinantseigenvalueseigenvectors

Frequently asked questions

Where can I find the BE Civil Engineering (IOE, TU) Engineering Mathematics II (IOE, SH 451) question paper 2078?
The full BE Civil Engineering (IOE, TU) Engineering Mathematics II (IOE, SH 451) 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 Engineering Mathematics II (IOE, SH 451) 2078 paper come with solutions?
Yes. Every question on this Engineering Mathematics II (IOE, SH 451) past paper includes a step-by-step solution, plus instant AI feedback when you attempt it on Kekkei.
How many marks is the BE Civil Engineering (IOE, TU) Engineering Mathematics II (IOE, SH 451) 2078 paper?
The BE Civil Engineering (IOE, TU) Engineering Mathematics II (IOE, SH 451) 2078 paper carries 80 full marks and is meant to be completed in 180 minutes, across 11 questions.
Is practising this Engineering Mathematics II (IOE, SH 451) past paper free?
Yes — reading and attempting this Engineering Mathematics II (IOE, SH 451) past paper on Kekkei is completely free.