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Section A: Long Answer Questions

Attempt any TWO questions.

3 questions·10 marks each
1long10 marks

State the conditions for a system of linear equations to have (i) a unique solution (ii) infinitely many solutions (iii) no solution. Illustrate each with an example using the rank method.

Consistency of a Linear System by the Rank Method

Consider AX=BAX = B, where AA is the m×nm \times n coefficient matrix, XX the column of nn unknowns, BB the column of constants, and [AB][A\,|\,B] the augmented matrix. Let r=rank(A)r = \operatorname{rank}(A), r=rank([AB])r' = \operatorname{rank}([A\,|\,B]), and nn the number of unknowns.

(i) Unique solution

Condition: rank(A)=rank([AB])=n\operatorname{rank}(A) = \operatorname{rank}([A\,|\,B]) = n (the system is consistent and the rank equals the number of unknowns).

Example: x+y=3, xy=1x + y = 3,\ x - y = 1.

[AB]=[113111]R2R2R1[113022].[A\,|\,B] = \begin{bmatrix} 1 & 1 & 3 \\ 1 & -1 & 1 \end{bmatrix} \xrightarrow{R_2 \to R_2 - R_1} \begin{bmatrix} 1 & 1 & 3 \\ 0 & -2 & -2 \end{bmatrix}.

Here r=r=2=nr = r' = 2 = n, so there is a unique solution x=2, y=1x = 2,\ y = 1.

(ii) Infinitely many solutions

Condition: rank(A)=rank([AB])=r<n\operatorname{rank}(A) = \operatorname{rank}([A\,|\,B]) = r < n (consistent, but rank less than the number of unknowns; nrn - r free parameters).

Example: x+y+z=2, 2x+2y+2z=4x + y + z = 2,\ 2x + 2y + 2z = 4.

[AB]=[11122224]R2R22R1[11120000].[A\,|\,B] = \begin{bmatrix} 1 & 1 & 1 & 2 \\ 2 & 2 & 2 & 4 \end{bmatrix} \xrightarrow{R_2 \to R_2 - 2R_1} \begin{bmatrix} 1 & 1 & 1 & 2 \\ 0 & 0 & 0 & 0 \end{bmatrix}.

Here r=r=1<n=3r = r' = 1 < n = 3, so there are infinitely many solutions (two free parameters).

(iii) No solution

Condition: rank(A)rank([AB])\operatorname{rank}(A) \neq \operatorname{rank}([A\,|\,B]), i.e. rank(A)<rank([AB])\operatorname{rank}(A) < \operatorname{rank}([A\,|\,B]) (the system is inconsistent).

Example: x+y=1, x+y=3x + y = 1,\ x + y = 3.

[AB]=[111113]R2R2R1[111002].[A\,|\,B] = \begin{bmatrix} 1 & 1 & 1 \\ 1 & 1 & 3 \end{bmatrix} \xrightarrow{R_2 \to R_2 - R_1} \begin{bmatrix} 1 & 1 & 1 \\ 0 & 0 & 2 \end{bmatrix}.

Here rank(A)=1\operatorname{rank}(A) = 1 but rank([AB])=2\operatorname{rank}([A\,|\,B]) = 2, so the system has no solution.

Summary: Consistency requires r=rr = r'; then r=nr = n gives a unique solution and r<nr < n gives infinitely many, while rrr \neq r' gives no solution.

linear-systemsrank
2long10 marks

Define a symmetric and a skew-symmetric matrix. Show that every square matrix can be expressed uniquely as the sum of a symmetric and a skew-symmetric matrix.

Symmetric and Skew-Symmetric Matrices

Symmetric matrix: A square matrix AA is symmetric if AT=AA^T = A, i.e. aij=ajia_{ij} = a_{ji} for all i,ji, j.

Skew-symmetric matrix: A square matrix AA is skew-symmetric if AT=AA^T = -A, i.e. aij=ajia_{ij} = -a_{ji} for all i,ji, j. In particular every diagonal entry satisfies aii=aiia_{ii} = -a_{ii}, so aii=0a_{ii} = 0.

Every Square Matrix = Symmetric + Skew-Symmetric (uniquely)

Let AA be any n×nn \times n matrix. Define

P=12(A+AT),Q=12(AAT).P = \tfrac{1}{2}\left(A + A^T\right), \qquad Q = \tfrac{1}{2}\left(A - A^T\right).

Existence. Clearly

P+Q=12(A+AT)+12(AAT)=A.P + Q = \tfrac{1}{2}(A + A^T) + \tfrac{1}{2}(A - A^T) = A.

PP is symmetric because

PT=12(A+AT)T=12(AT+A)=P.P^T = \tfrac{1}{2}(A + A^T)^T = \tfrac{1}{2}(A^T + A) = P.

QQ is skew-symmetric because

QT=12(AAT)T=12(ATA)=Q.Q^T = \tfrac{1}{2}(A - A^T)^T = \tfrac{1}{2}(A^T - A) = -Q.

Thus A=P+QA = P + Q is a sum of a symmetric and a skew-symmetric matrix.

Uniqueness. Suppose A=S+KA = S + K with ST=SS^T = S (symmetric) and KT=KK^T = -K (skew-symmetric). Then

AT=ST+KT=SK.A^T = S^T + K^T = S - K.

Adding and subtracting,

A+AT=2S    S=12(A+AT)=P,A + A^T = 2S \implies S = \tfrac{1}{2}(A + A^T) = P, AAT=2K    K=12(AAT)=Q.A - A^T = 2K \implies K = \tfrac{1}{2}(A - A^T) = Q.

Hence the decomposition is unique, S=PS = P and K=QK = Q. \blacksquare

Example: For A=[1243]A = \begin{bmatrix} 1 & 2 \\ 4 & 3 \end{bmatrix}, P=[1333]P = \begin{bmatrix} 1 & 3 \\ 3 & 3 \end{bmatrix} (symmetric) and Q=[0110]Q = \begin{bmatrix} 0 & -1 \\ 1 & 0 \end{bmatrix} (skew-symmetric), and P+Q=AP + Q = A.

matrixsymmetric
3long10 marks

Find the eigenvalues and eigenvectors of the given matrix and hence diagonalize it. Use the diagonal form to compute (A^4).

Eigenvalues, Eigenvectors, Diagonalization and A4A^4

Since the paper does not print a specific matrix, take the standard representative

A=[2112].A = \begin{bmatrix} 2 & 1 \\ 1 & 2 \end{bmatrix}.

The method below applies to any diagonalizable matrix.

Step 1: Characteristic equation

det(AλI)=2λ112λ=(2λ)21=λ24λ+3=0.\det(A - \lambda I) = \begin{vmatrix} 2-\lambda & 1 \\ 1 & 2-\lambda \end{vmatrix} = (2-\lambda)^2 - 1 = \lambda^2 - 4\lambda + 3 = 0.

So (λ1)(λ3)=0(\lambda - 1)(\lambda - 3) = 0, giving eigenvalues λ1=1, λ2=3\lambda_1 = 1,\ \lambda_2 = 3.

Step 2: Eigenvectors

For λ1=1\lambda_1 = 1: (AI)X=0[1111]X=0x1+x2=0(A - I)X = 0 \Rightarrow \begin{bmatrix} 1 & 1 \\ 1 & 1 \end{bmatrix}X = 0 \Rightarrow x_1 + x_2 = 0, eigenvector v1=[11]v_1 = \begin{bmatrix} 1 \\ -1 \end{bmatrix}.

For λ2=3\lambda_2 = 3: (A3I)X=0[1111]X=0x1=x2(A - 3I)X = 0 \Rightarrow \begin{bmatrix} -1 & 1 \\ 1 & -1 \end{bmatrix}X = 0 \Rightarrow x_1 = x_2, eigenvector v2=[11]v_2 = \begin{bmatrix} 1 \\ 1 \end{bmatrix}.

Step 3: Diagonalization

Let

P=[1111],D=[1003],P1=12[1111].P = \begin{bmatrix} 1 & 1 \\ -1 & 1 \end{bmatrix}, \qquad D = \begin{bmatrix} 1 & 0 \\ 0 & 3 \end{bmatrix}, \qquad P^{-1} = \tfrac{1}{2}\begin{bmatrix} 1 & -1 \\ 1 & 1 \end{bmatrix}.

Then A=PDP1A = PDP^{-1} (equivalently P1AP=DP^{-1}AP = D).

Step 4: Compute A4A^4

Because A4=PD4P1A^4 = P D^4 P^{-1} and D4=diag(14,34)=diag(1,81)D^4 = \operatorname{diag}(1^4, 3^4) = \operatorname{diag}(1, 81),

A4=[1111][10081]12[1111]=12[181181][1111].A^4 = \begin{bmatrix} 1 & 1 \\ -1 & 1 \end{bmatrix} \begin{bmatrix} 1 & 0 \\ 0 & 81 \end{bmatrix} \cdot \tfrac{1}{2}\begin{bmatrix} 1 & -1 \\ 1 & 1 \end{bmatrix} = \tfrac{1}{2}\begin{bmatrix} 1 & 81 \\ -1 & 81 \end{bmatrix}\begin{bmatrix} 1 & -1 \\ 1 & 1 \end{bmatrix}. A4=12[82808082]=[41404041].A^4 = \tfrac{1}{2}\begin{bmatrix} 82 & 80 \\ 80 & 82 \end{bmatrix} = \begin{bmatrix} 41 & 40 \\ 40 & 41 \end{bmatrix}.

Result: eigenvalues 1,31, 3; eigenvectors (1,1)T, (1,1)T(1,-1)^T,\ (1,1)^T; A=PDP1A = PDP^{-1}; and A4=[41404041]A^4 = \begin{bmatrix} 41 & 40 \\ 40 & 41 \end{bmatrix}.

eigenvaluesdiagonalization
B

Section B: Short Answer Questions

Attempt any EIGHT questions.

9 questions·5 marks each
4short5 marks

Define a skew-symmetric matrix with an example.

A square matrix AA is skew-symmetric if AT=AA^T = -A, equivalently aij=ajia_{ij} = -a_{ji} for all i,ji, j. This forces every diagonal entry to be zero (aii=0a_{ii} = 0).

Example:

A=[023205350],AT=A.A = \begin{bmatrix} 0 & 2 & -3 \\ -2 & 0 & 5 \\ 3 & -5 & 0 \end{bmatrix}, \qquad A^T = -A.
matrix
5short5 marks

Find the determinant of [[2,1,0],[1,3,1],[0,1,2]].

Expanding along the first row,

det=2311211102+0.\det = 2\begin{vmatrix} 3 & 1 \\ 1 & 2 \end{vmatrix} - 1\begin{vmatrix} 1 & 1 \\ 0 & 2 \end{vmatrix} + 0. =2(3211)1(1210)=2(5)1(2)=102=8.= 2(3\cdot 2 - 1\cdot 1) - 1(1\cdot 2 - 1\cdot 0) = 2(5) - 1(2) = 10 - 2 = 8.

Determinant =8= 8.

determinant
6short5 marks

Define the image and kernel of a linear map.

Let T:VWT : V \to W be a linear map between vector spaces.

Image (range): the set of all output vectors,

Im(T)={T(v):vV}W.\operatorname{Im}(T) = \{\, T(v) : v \in V \,\} \subseteq W.

It is a subspace of WW; its dimension is the rank of TT.

Kernel (null space): the set of all inputs mapped to the zero vector,

ker(T)={vV:T(v)=0}V.\ker(T) = \{\, v \in V : T(v) = 0 \,\} \subseteq V.

It is a subspace of VV; its dimension is the nullity of TT.

They are linked by the rank–nullity theorem: dimV=dimker(T)+dimIm(T)\dim V = \dim \ker(T) + \dim \operatorname{Im}(T).

linear-transformation
7short5 marks

What is the algebraic multiplicity of an eigenvalue?

The algebraic multiplicity of an eigenvalue λ\lambda of a matrix AA is the number of times λ\lambda occurs as a root of the characteristic polynomial det(AλI)=0\det(A - \lambda I) = 0, i.e. the multiplicity of the factor (λλ0)(\lambda - \lambda_0) in that polynomial.

For example, if det(AλI)=(λ2)3(λ5)\det(A - \lambda I) = (\lambda - 2)^3(\lambda - 5), then the eigenvalue λ=2\lambda = 2 has algebraic multiplicity 33. It is always greater than or equal to the geometric multiplicity (the dimension of the corresponding eigenspace).

eigenvalues
8short5 marks

Define an inner product on (R^n).

An inner product on Rn\mathbb{R}^n is a function ,:Rn×RnR\langle \cdot, \cdot \rangle : \mathbb{R}^n \times \mathbb{R}^n \to \mathbb{R} that assigns a real number to each pair of vectors and satisfies, for all u,v,wRnu, v, w \in \mathbb{R}^n and scalar cc:

  1. Symmetry: u,v=v,u\langle u, v \rangle = \langle v, u \rangle.
  2. Linearity: cu+w,v=cu,v+w,v\langle cu + w, v \rangle = c\langle u, v \rangle + \langle w, v \rangle.
  3. Positive-definiteness: u,u0\langle u, u \rangle \geq 0, with equality iff u=0u = 0.

The standard (dot) inner product is

u,v=uTv=i=1nuivi.\langle u, v \rangle = u^T v = \sum_{i=1}^{n} u_i v_i.
inner-product
9short5 marks

State whether the vectors (1,2), (2,4) are linearly independent.

The vectors are linearly dependent.

Note that (2,4)=2(1,2)(2,4) = 2\,(1,2), so one is a scalar multiple of the other. Equivalently, the equation c1(1,2)+c2(2,4)=(0,0)c_1(1,2) + c_2(2,4) = (0,0) has the non-trivial solution c1=2, c2=1c_1 = 2,\ c_2 = -1. The determinant test also confirms this:

1224=1422=0.\begin{vmatrix} 1 & 2 \\ 2 & 4 \end{vmatrix} = 1\cdot 4 - 2\cdot 2 = 0.

Since the determinant is 00, the vectors are not linearly independent.

linear-independence
10short5 marks

Define a finite-dimensional vector space.

A vector space VV is said to be finite-dimensional if it has a finite spanning set, i.e. there exist finitely many vectors v1,v2,,vnVv_1, v_2, \dots, v_n \in V such that every vector in VV can be written as a linear combination a1v1+a2v2++anvna_1 v_1 + a_2 v_2 + \cdots + a_n v_n.

Equivalently, VV is finite-dimensional if it possesses a basis with a finite number of elements; that number is the dimension dimV\dim V. For example, Rn\mathbb{R}^n is finite-dimensional with dimRn=n\dim \mathbb{R}^n = n. A space with no finite basis (e.g. the space of all polynomials) is infinite-dimensional.

dimension
11short5 marks

What is the canonical form of a quadratic form?

The canonical form of a quadratic form Q(x)=xTAxQ(x) = x^T A x is the expression obtained, after a suitable change of variables, in which only squared terms appear and all cross-product terms are eliminated:

Q=λ1y12+λ2y22++λnyn2.Q = \lambda_1 y_1^2 + \lambda_2 y_2^2 + \cdots + \lambda_n y_n^2.

This is achieved by an orthogonal transformation x=Pyx = Py (with PP the matrix of orthonormal eigenvectors of the symmetric matrix AA), where the coefficients λi\lambda_i are the eigenvalues of AA. The number of positive, negative and zero coefficients gives the signature and rank of the form (which are invariant by Sylvester's law of inertia).

quadratic-form
12short5 marks

Find the sum and product of eigenvalues of [[1,2],[3,4]] using trace and determinant.

For A=[1234]A = \begin{bmatrix} 1 & 2 \\ 3 & 4 \end{bmatrix}:

Sum of eigenvalues == trace(A)=1+4=5(A) = 1 + 4 = 5.

Product of eigenvalues == det(A)=(1)(4)(2)(3)=46=2\det(A) = (1)(4) - (2)(3) = 4 - 6 = -2.

Thus λ1+λ2=5\lambda_1 + \lambda_2 = 5 and λ1λ2=2\lambda_1 \lambda_2 = -2 (the eigenvalues themselves are 5±332\tfrac{5 \pm \sqrt{33}}{2}).

eigenvalues

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