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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-inversion method, using the adjoint to find the inverse of the coefficient matrix:

2x+y+z=7x+3y+2z=133x+2y+z=10\begin{aligned} 2x + y + z &= 7 \\ x + 3y + 2z &= 13 \\ 3x + 2y + z &= 10 \end{aligned}

Verify your solution by direct substitution into the third equation.

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

A=(211132321),X=(xyz),B=(71310).A=\begin{pmatrix}2&1&1\\1&3&2\\3&2&1\end{pmatrix},\quad X=\begin{pmatrix}x\\y\\z\end{pmatrix},\quad B=\begin{pmatrix}7\\13\\10\end{pmatrix}.

Step 2 — Determinant of AA.

detA=2(3122)1(1123)+1(1233)\det A = 2(3\cdot1-2\cdot2) - 1(1\cdot1-2\cdot3) + 1(1\cdot2-3\cdot3) =2(34)1(16)+1(29)=2(1)1(5)+1(7)=2+57=4.= 2(3-4) - 1(1-6) + 1(2-9) = 2(-1) -1(-5) + 1(-7) = -2+5-7 = -4.

Since detA=40\det A = -4 \neq 0, A1A^{-1} exists and the solution is unique.

Step 3 — Cofactor matrix.

C11=+(34)=1,  C12=(16)=5,  C13=+(29)=7,C_{11}=+(3-4)=-1,\; C_{12}=-(1-6)=5,\; C_{13}=+(2-9)=-7, C21=(12)=1,  C22=+(23)=1,  C23=(43)=1,C_{21}=-(1-2)=1,\; C_{22}=+(2-3)=-1,\; C_{23}=-(4-3)=-1, C31=+(23)=1,  C32=(41)=3,  C33=+(61)=5.C_{31}=+(2-3)=-1,\; C_{32}=-(4-1)=-3,\; C_{33}=+(6-1)=5.

Step 4 — Adjoint (transpose of cofactor matrix).

adjA=(111513715).\operatorname{adj}A = \begin{pmatrix}-1&1&-1\\5&-1&-3\\-7&-1&5\end{pmatrix}.

Step 5 — Inverse.

A1=1detAadjA=14(111513715).A^{-1}=\frac{1}{\det A}\operatorname{adj}A = -\frac{1}{4}\begin{pmatrix}-1&1&-1\\5&-1&-3\\-7&-1&5\end{pmatrix}.

Step 6 — Solve X=A1BX = A^{-1}B.

Compute adjAB\operatorname{adj}A \cdot B:

(111513715)(71310)=(7+13103513304913+50)=(4812).\begin{pmatrix}-1&1&-1\\5&-1&-3\\-7&-1&5\end{pmatrix}\begin{pmatrix}7\\13\\10\end{pmatrix}=\begin{pmatrix}-7+13-10\\35-13-30\\-49-13+50\end{pmatrix}=\begin{pmatrix}-4\\-8\\-12\end{pmatrix}.

Then

X=14(4812)=(123).X = -\frac{1}{4}\begin{pmatrix}-4\\-8\\-12\end{pmatrix}=\begin{pmatrix}1\\2\\3\end{pmatrix}.

Hence x=1,  y=2,  z=3\boxed{x=1,\; y=2,\; z=3}.

Step 7 — Verification (third equation): 3(1)+2(2)+1(3)=3+4+3=10.3(1)+2(2)+1(3)=3+4+3=10. ✓ (Also: 2(1)+2+3=72(1)+2+3=7 ✓, 1+6+6=131+6+6=13 ✓.)

determinantsmatriceslinear-systems
2long10 marks

Find the equation of the plane passing through the points A(1,1,0)A(1,1,0), B(2,0,1)B(2,0,1) and C(0,2,3)C(0,2,3). Hence find the perpendicular distance from the point P(3,4,5)P(3,4,5) to this plane.

Step 1 — Two direction vectors in the plane.

AB=BA=(1,1,1),AC=CA=(1,1,3).\vec{AB}=B-A=(1,-1,1),\qquad \vec{AC}=C-A=(-1,1,3).

Step 2 — Normal vector n=AB×AC\vec n = \vec{AB}\times\vec{AC}.

n=ijk111113.\vec n = \begin{vmatrix}\mathbf i&\mathbf j&\mathbf k\\1&-1&1\\-1&1&3\end{vmatrix}. nx=(1)(3)(1)(1)=31=4,n_x = (-1)(3)-(1)(1) = -3-1 = -4, ny=[(1)(3)(1)(1)]=(3+1)=4,n_y = -\big[(1)(3)-(1)(-1)\big] = -(3+1) = -4, nz=(1)(1)(1)(1)=11=0.n_z = (1)(1)-(-1)(-1) = 1-1 = 0.

So n=(4,4,0)\vec n = (-4,-4,0), or dividing by 4-4, n(1,1,0)\vec n \parallel (1,1,0).

Step 3 — Equation of the plane. Using point A(1,1,0)A(1,1,0) and normal (1,1,0)(1,1,0):

1(x1)+1(y1)+0(z0)=0    x+y2=0.1(x-1)+1(y-1)+0(z-0)=0 \;\Rightarrow\; x+y-2=0.

Plane: x+y=2\boxed{x+y=2}.

Check the three points: A:1+1=2A:1+1=2 ✓, B:2+0=2B:2+0=2 ✓, C:0+2=2C:0+2=2 ✓.

Step 4 — Perpendicular distance from P(3,4,5)P(3,4,5).

d=x0+y0212+12+02=3+422=52=522.d=\frac{|x_0+y_0-2|}{\sqrt{1^2+1^2+0^2}}=\frac{|3+4-2|}{\sqrt2}=\frac{5}{\sqrt2}=\frac{5\sqrt2}{2}.

Distance =52=5223.54= \dfrac{5}{\sqrt2}=\dfrac{5\sqrt2}{2}\approx 3.54 units.

3d-geometryplaneshortest-distance
3long10 marks

Solve the differential equation

d2ydx25dydx+6y=e4x+sinx.\frac{d^2y}{dx^2} - 5\frac{dy}{dx} + 6y = e^{4x} + \sin x.

Step 1 — Complementary function (CF). Auxiliary equation:

m25m+6=0(m2)(m3)=0m=2,3.m^2 - 5m + 6 = 0 \Rightarrow (m-2)(m-3)=0 \Rightarrow m=2,\,3. yc=C1e2x+C2e3x.y_c = C_1 e^{2x} + C_2 e^{3x}.

Step 2 — Particular integral for e4xe^{4x}. With operator f(D)=D25D+6f(D)=D^2-5D+6, put D=4D=4:

f(4)=1620+6=20.f(4)=16-20+6=2 \neq 0. yp1=1f(4)e4x=12e4x.y_{p1}=\frac{1}{f(4)}e^{4x}=\frac{1}{2}e^{4x}.

Step 3 — Particular integral for sinx\sin x. Replace D21D^2 \to -1:

yp2=1D25D+6sinx=115D+6sinx=155Dsinx=1511Dsinx.y_{p2}=\frac{1}{D^2-5D+6}\sin x = \frac{1}{-1-5D+6}\sin x=\frac{1}{5-5D}\sin x=\frac{1}{5}\cdot\frac{1}{1-D}\sin x.

Multiply numerator and denominator by (1+D)(1+D):

=151+D1D2sinx=151+D1(1)sinx=110(1+D)sinx.=\frac{1}{5}\cdot\frac{1+D}{1-D^2}\sin x = \frac{1}{5}\cdot\frac{1+D}{1-(-1)}\sin x = \frac{1}{10}(1+D)\sin x. =110(sinx+cosx).=\frac{1}{10}(\sin x + \cos x).

Step 4 — General solution.

y=C1e2x+C2e3x+12e4x+110(sinx+cosx).\boxed{y = C_1 e^{2x} + C_2 e^{3x} + \tfrac{1}{2}e^{4x} + \tfrac{1}{10}(\sin x + \cos x).}

Verification of the sinx\sin x part: let yp2=110(sinx+cosx)y_{p2}=\frac{1}{10}(\sin x+\cos x), then y=110(cosxsinx)y'=\frac{1}{10}(\cos x-\sin x), y=110(sinxcosx)y''=\frac{1}{10}(-\sin x-\cos x). Substituting: y5y+6y=110[(sinxcosx)5(cosxsinx)+6(sinx+cosx)]=110[(1+5+6)sinx+(15+6)cosx]=110(10sinx)=sinx.y''-5y'+6y=\frac{1}{10}[(-\sin x-\cos x)-5(\cos x-\sin x)+6(\sin x+\cos x)] = \frac{1}{10}[(-1+5+6)\sin x +(-1-5+6)\cos x] = \frac{1}{10}(10\sin x) = \sin x.

second-order-odeundetermined-coefficientsparticular-integral
4long8 marks

Test the convergence of the series

n=1n22n.\sum_{n=1}^{\infty} \frac{n^2}{2^n}.

Further, for what range of values of x>0x>0 does the series n=1n2xn\displaystyle\sum_{n=1}^{\infty} \frac{n^2}{x^n} converge?

Part (a) — Test n2/2n\sum n^2/2^n by the Ratio Test.

Let an=n22na_n = \dfrac{n^2}{2^n}. Then

an+1an=(n+1)22n+12nn2=12(n+1n)2=12(1+1n)2.\frac{a_{n+1}}{a_n} = \frac{(n+1)^2}{2^{n+1}}\cdot\frac{2^n}{n^2}=\frac{1}{2}\left(\frac{n+1}{n}\right)^2 = \frac{1}{2}\left(1+\frac{1}{n}\right)^2.

Taking the limit:

L=limnan+1an=121=12.L=\lim_{n\to\infty}\frac{a_{n+1}}{a_n} = \frac{1}{2}\cdot 1 = \frac{1}{2}.

Since L=12<1L = \tfrac12 < 1, by the Ratio Test the series converges.

Part (b) — General n2/xn\sum n^2/x^n for x>0x>0.

Let bn=n2xnb_n = \dfrac{n^2}{x^n}. Then

bn+1bn=(n+1)2xn+1xnn2=1x(1+1n)21x.\frac{b_{n+1}}{b_n}=\frac{(n+1)^2}{x^{n+1}}\cdot\frac{x^n}{n^2}=\frac{1}{x}\left(1+\frac1n\right)^2 \to \frac{1}{x}.
  • If 1x<1\dfrac1x < 1, i.e. x>1x>1: series converges.
  • If 1x>1\dfrac1x > 1, i.e. 0<x<10<x<1: series diverges.
  • If x=1x=1: the series becomes n2\sum n^2, whose terms \to\infty, so it diverges (term test fails).

Conclusion: the series n2xn\displaystyle\sum \frac{n^2}{x^n} converges precisely for x>1\boxed{x>1}.

infinite-seriesratio-testconvergence
5long12 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, by choosing a suitable value of xx, deduce that

n=11n2=π26.\sum_{n=1}^{\infty}\frac{1}{n^2} = \frac{\pi^2}{6}.

Step 1 — Symmetry. f(x)=x2f(x)=x^2 is an even function on (π,π)(-\pi,\pi), so all sine coefficients vanish: 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}.

(The series uses a02=π23\tfrac{a_0}{2}=\tfrac{\pi^2}{3} as the mean term.)

Step 3 — Cosine coefficients ana_n.

an=2π0πx2cos(nx)dx.a_n=\frac{2}{\pi}\int_0^{\pi}x^2\cos(nx)\,dx.

Integrate by parts twice. The standard result is

x2cos(nx)dx=x2sin(nx)n+2xcos(nx)n22sin(nx)n3.\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: sin(nπ)=0\sin(n\pi)=0, cos(nπ)=(1)n\cos(n\pi)=(-1)^n; at x=0x=0 all terms vanish. Thus

0πx2cos(nx)dx=2π(1)nn2.\int_0^{\pi}x^2\cos(nx)\,dx = \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.

x2=π23+n=14(1)nn2cos(nx)=π234(cosxcos2x4+cos3x9).\boxed{x^2 = \frac{\pi^2}{3} + \sum_{n=1}^{\infty}\frac{4(-1)^n}{n^2}\cos(nx) = \frac{\pi^2}{3} - 4\left(\cos x - \frac{\cos 2x}{4} + \frac{\cos 3x}{9} - \cdots\right).}

Step 5 — Deduce 1/n2\sum 1/n^2. Put x=πx=\pi (where ff is continuous in the periodic extension and equals π2\pi^2):

π2=π23+n=14(1)nn2cos(nπ).\pi^2 = \frac{\pi^2}{3} + \sum_{n=1}^{\infty}\frac{4(-1)^n}{n^2}\cos(n\pi).

Since cos(nπ)=(1)n\cos(n\pi)=(-1)^n, we have (1)n(1)n=1(-1)^n(-1)^n=1, so

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

Rearrange:

4n=11n2=π2π23=2π23    n=11n2=π26.4\sum_{n=1}^{\infty}\frac{1}{n^2}=\pi^2-\frac{\pi^2}{3}=\frac{2\pi^2}{3}\;\Rightarrow\; \sum_{n=1}^{\infty}\frac{1}{n^2}=\frac{\pi^2}{6}. \qquad\blacksquare
fourier-seriesperiodic-functionhalf-range
B

Section B: Short Answer Questions

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6 questions
6short5 marks

Find the rank of the matrix

A=(1232473610)A=\begin{pmatrix}1&2&3\\2&4&7\\3&6&10\end{pmatrix}

by reducing it to row-echelon form.

Step 1 — Eliminate below the first pivot.

R2R22R1R_2 \to R_2 - 2R_1: (22,  44,  76)=(0,0,1)(2-2,\;4-4,\;7-6)=(0,0,1). R3R33R1R_3 \to R_3 - 3R_1: (33,  66,  109)=(0,0,1)(3-3,\;6-6,\;10-9)=(0,0,1).

A(123001001).A \sim \begin{pmatrix}1&2&3\\0&0&1\\0&0&1\end{pmatrix}.

Step 2 — Eliminate the third row.

R3R3R2R_3 \to R_3 - R_2: (0,0,0)(0,0,0).

A(123001000).A \sim \begin{pmatrix}1&2&3\\0&0&1\\0&0&0\end{pmatrix}.

Step 3 — Count non-zero rows. There are 2 non-zero rows.

Rank(A)=2(A) = \boxed{2}.

matricesrankechelon-form
7short5 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).

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

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

So b1×b2=(1,2,1)\vec b_1\times\vec b_2=(-1,2,-1), with b1×b2=1+4+1=6.|\vec b_1\times\vec b_2|=\sqrt{1+4+1}=\sqrt6.

Step 3 — Vector joining the points. AC=CA=(1,2,2).\vec{AC}=C-A=(1,2,2).

Step 4 — Scalar triple product.

AC(b1×b2)=(1)(1)+(2)(2)+(2)(1)=1+42=1.\vec{AC}\cdot(\vec b_1\times\vec b_2)=(1)(-1)+(2)(2)+(2)(-1)=-1+4-2=1.

Step 5 — 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}.

Shortest distance =16=660.408=\dfrac{1}{\sqrt6}=\dfrac{\sqrt6}{6}\approx 0.408 units.

3d-geometrylineskew-lines
8short5 marks

Solve the Cauchy–Euler (homogeneous) differential equation

x2d2ydx23xdydx+4y=0.x^2\frac{d^2y}{dx^2} - 3x\frac{dy}{dx} + 4y = 0.

Step 1 — Trial solution. For a Cauchy–Euler equation try y=xmy=x^m. Then y=mxm1y'=mx^{m-1} and y=m(m1)xm2y''=m(m-1)x^{m-2}.

Step 2 — Substitute.

x2m(m1)xm23xmxm1+4xm=0x^2\,m(m-1)x^{m-2} - 3x\,mx^{m-1} + 4x^m = 0 [m(m1)3m+4]xm=0.\Rightarrow \big[m(m-1) - 3m + 4\big]x^m = 0.

Step 3 — Indicial (auxiliary) equation.

m2m3m+4=0    m24m+4=0    (m2)2=0.m^2 - m - 3m + 4 = 0 \;\Rightarrow\; m^2 - 4m + 4 = 0 \;\Rightarrow\; (m-2)^2 = 0.

This gives a repeated root m=2m=2.

Step 4 — General solution. For a repeated root mm, the solution is y=(C1+C2lnx)xmy=(C_1 + C_2\ln x)x^m:

y=(C1+C2lnx)x2.\boxed{y = (C_1 + C_2\ln x)\,x^2.}

Check: y2=x2lnxy_2=x^2\ln x gives y2=2xlnx+xy_2'=2x\ln x + x, y2=2lnx+3y_2''=2\ln x+3. Then x2(2lnx+3)3x(2xlnx+x)+4x2lnx=2x2lnx+3x26x2lnx3x2+4x2lnx=0.x^2(2\ln x+3)-3x(2x\ln x+x)+4x^2\ln x = 2x^2\ln x+3x^2-6x^2\ln x-3x^2+4x^2\ln x = 0.

second-order-odecauchy-eulergeneral-solution
9short5 marks

Test the convergence of the series

n=11n(n+1)\sum_{n=1}^{\infty}\frac{1}{\sqrt{n(n+1)}}

using the comparison test.

Step 1 — Choose a comparison series. For large nn, n(n+1)n\sqrt{n(n+1)}\approx n, so compare with the pp-series 1/n\sum 1/n (the harmonic series, p=1p=1), which diverges.

Step 2 — Limit comparison test. Let an=1n(n+1)a_n=\dfrac{1}{\sqrt{n(n+1)}} and bn=1nb_n=\dfrac{1}{n}. Then

anbn=1/n(n+1)1/n=nn(n+1)=nn2+n=11+1n.\frac{a_n}{b_n}=\frac{1/\sqrt{n(n+1)}}{1/n}=\frac{n}{\sqrt{n(n+1)}}=\frac{n}{\sqrt{n^2+n}}=\frac{1}{\sqrt{1+\frac1n}}.

Step 3 — Take the limit.

L=limnanbn=11+0=1.L=\lim_{n\to\infty}\frac{a_n}{b_n}=\frac{1}{\sqrt{1+0}}=1.

Since 0<L=1<0<L=1<\infty (finite and non-zero), an\sum a_n and bn\sum b_n behave alike.

Step 4 — Conclusion. Because 1n\sum \dfrac1n diverges, the given series

n=11n(n+1)  diverges.\sum_{n=1}^{\infty}\frac{1}{\sqrt{n(n+1)}}\;\textbf{diverges}.
infinite-seriescomparison-testp-series
10short5 marks

Find the eigenvalues and the 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:

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

Eigenvector: 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)=02x+y=0y=2x.\begin{pmatrix}2&1\\2&1\end{pmatrix}\begin{pmatrix}x\\y\end{pmatrix}=0 \Rightarrow 2x+y=0 \Rightarrow y=-2x.

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

Result: λ1=5\lambda_1=5 with v1=(1,1)Tv_1=(1,1)^T; λ2=2\lambda_2=2 with v2=(1,2)Tv_2=(1,-2)^T.

Check: Av1=(4+12+3)=(55)=5v1Av_1=\binom{4+1}{2+3}=\binom{5}{5}=5v_1 ✓; Av2=(4226)=(24)=2v2Av_2=\binom{4-2}{2-6}=\binom{2}{-4}=2v_2 ✓.

matriceseigenvaluescharacteristic-equation
11short5 marks

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

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

f(x)=n=1bnsin(nx),bn=2π0πf(x)sin(nx)dx.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=2π0πxsin(nx)dx.b_n=\frac{2}{\pi}\int_0^{\pi} x\sin(nx)\,dx.

Integrate by parts (u=xu=x, dv=sin(nx)dxdv=\sin(nx)\,dx):

0πxsin(nx)dx=[xcos(nx)n]0π+1n0πcos(nx)dx.\int_0^{\pi} x\sin(nx)\,dx = \left[-\frac{x\cos(nx)}{n}\right]_0^{\pi} + \frac{1}{n}\int_0^{\pi}\cos(nx)\,dx.

First term: πcos(nπ)n=π(1)nn-\dfrac{\pi\cos(n\pi)}{n} = -\dfrac{\pi(-1)^n}{n}. Second term: 1n[sin(nx)n]0π=0\dfrac{1}{n}\left[\dfrac{\sin(nx)}{n}\right]_0^{\pi}=0 (since sin(nπ)=0\sin(n\pi)=0).

So

0πxsin(nx)dx=π(1)nn=π(1)n+1n.\int_0^{\pi} x\sin(nx)\,dx = -\frac{\pi(-1)^n}{n}=\frac{\pi(-1)^{n+1}}{n}.

Step 3 — Coefficient.

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 4 — Series.

x=n=12(1)n+1nsin(nx)=2(sinxsin2x2+sin3x3),0<x<π.\boxed{x = \sum_{n=1}^{\infty}\frac{2(-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

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