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University Mathematics Practice Test — 30 Challenging Problems

University Mathematics Practice Test — 30 Challenging Problems

Section titled “University Mathematics Practice Test — 30 Challenging Problems”

This practice test covers 30 problems across four major domains of university mathematics: Multivariable Calculus, Linear Algebra, Abstract Algebra, and Real Analysis. Each problem requires rigorous reasoning, proof construction, and the application of fundamental theorems. Work through the problems with pen and paper before checking the solutions.

  • Time limit: 120 minutes (4 minutes per problem)
  • Format: Problem-solving — show all working and proofs
  • Marking: 1 mark per problem, 30 marks total
  • Conditions: Attempt without notes. Write complete, rigorous proofs.
  • After the test: Check the solutions at the bottom. Study the proof techniques for any problems you got wrong.
DomainProblemsMarks
Multivariable CalculusP1–P88
Linear AlgebraP9–P168
Abstract AlgebraP17–P237
Real AnalysisP24–P307
Total3030

Evaluate the double integral:

Dex2dA\iint_D e^{x^2} \, dA

where DD is the region bounded by y=0y = 0, y=xy = x, and x=1x = 1.

Solution:

The region DD is described by 0x10 \leq x \leq 1 and 0yx0 \leq y \leq x. Since ex2e^{x^2} has no elementary antiderivative with respect to xx, we must integrate with respect to yy first:

010xex2dydx=01xex2dx\int_0^1 \int_0^x e^{x^2} \, dy \, dx = \int_0^1 x \, e^{x^2} \, dx

Substituting u=x2u = x^2, du=2xdxdu = 2x \, dx:

=1201eudu=12(e1)= \frac{1}{2} \int_0^1 e^u \, du = \frac{1}{2}(e - 1)

medium — 1 mark


P2 — Gradient and Directional Derivatives

Section titled “P2 — Gradient and Directional Derivatives”

Find the directional derivative of f(x,y,z)=x2y+yz3f(x,y,z) = x^2 y + yz^3 at the point (1,2,1)(1,2,-1) in the direction of the vector v=2ij+2k\mathbf{v} = 2\mathbf{i} - \mathbf{j} + 2\mathbf{k}.

Solution:

The gradient is:

f=(2xy,x2+z3,3yz2)\nabla f = (2xy, \, x^2 + z^3, \, 3yz^2)

At (1,2,1)(1,2,-1):

f(1,2,1)=(4,11,321)=(4,0,6)\nabla f(1,2,-1) = (4, \, 1 - 1, \, 3 \cdot 2 \cdot 1) = (4, 0, 6)

The unit vector in the direction of v\mathbf{v} is:

v^=13(2,1,2)\hat{\mathbf{v}} = \frac{1}{3}(2, -1, 2)

The directional derivative is:

Dv^f=fv^=13(8+0+12)=203D_{\hat{\mathbf{v}}} f = \nabla f \cdot \hat{\mathbf{v}} = \frac{1}{3}(8 + 0 + 12) = \frac{20}{3}

medium — 1 mark


Compute the line integral CFdr\int_C \mathbf{F} \cdot d\mathbf{r} where F=(y,x,z)\mathbf{F} = (y, x, z) and CC is the helix r(t)=(cost,sint,t)\mathbf{r}(t) = (\cos t, \sin t, t) for 0t2π0 \leq t \leq 2\pi.

Solution:

r(t)=(sint,cost,1)\mathbf{r}'(t) = (-\sin t, \cos t, 1).

F(r(t))=(sint,cost,t)\mathbf{F}(\mathbf{r}(t)) = (\sin t, \cos t, t).

Fr=sin2t+cos2t+t=cos2t+t\mathbf{F} \cdot \mathbf{r}' = -\sin^2 t + \cos^2 t + t = \cos 2t + t

02π(cos2t+t)dt=[sin2t2+t22]02π=2π2\int_0^{2\pi} (\cos 2t + t) \, dt = \left[\frac{\sin 2t}{2} + \frac{t^2}{2}\right]_0^{2\pi} = 2\pi^2

medium — 1 mark


Find the flux of F=(x,y,z)\mathbf{F} = (x, y, z) across the portion of the sphere x2+y2+z2=4x^2 + y^2 + z^2 = 4 lying above the plane z=1z = 1.

Solution:

Using the Divergence Theorem on the closed region bounded by the spherical cap and the disk x2+y23x^2 + y^2 \leq 3 at z=1z = 1:

V(F)dV=V3dV=3Vol(V)\iiint_V (\nabla \cdot \mathbf{F}) \, dV = \iiint_V 3 \, dV = 3 \, \text{Vol}(V)

The volume of the spherical cap of height h=1h = 1 from a sphere of radius R=2R = 2:

Vcap=πh23(3Rh)=π3(61)=5π3V_{\text{cap}} = \frac{\pi h^2}{3}(3R - h) = \frac{\pi}{3}(6 - 1) = \frac{5\pi}{3}

The flux through the disk (normal k-\mathbf{k}, z=1z = 1):

diskF(k)dA=disk1dA=3π\iint_{\text{disk}} \mathbf{F} \cdot (-\mathbf{k}) \, dA = -\iint_{\text{disk}} 1 \, dA = -3\pi

Therefore the flux through the spherical cap:

Φcap=35π3(3π)=5π+3π=8π\Phi_{\text{cap}} = 3 \cdot \frac{5\pi}{3} - (-3\pi) = 5\pi + 3\pi = 8\pi

hard — 1 mark


Use Green’s Theorem to evaluate C(xydx+x2dy)\oint_C (xy \, dx + x^2 \, dy) where CC is the boundary of the region enclosed by y=xy = x and y=x2y = x^2.

Solution:

By Green’s Theorem with P=xyP = xy, Q=x2Q = x^2:

CPdx+Qdy=D(QxPy)dA=D(2xx)dA=DxdA\oint_C P \, dx + Q \, dy = \iint_D \left(\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}\right) dA = \iint_D (2x - x) \, dA = \iint_D x \, dA

The region is bounded by y=x2y = x^2 (below) and y=xy = x (above), with 0x10 \leq x \leq 1:

01x2xxdydx=01x(xx2)dx=01(x2x3)dx=1314=112\int_0^1 \int_{x^2}^x x \, dy \, dx = \int_0^1 x(x - x^2) \, dx = \int_0^1 (x^2 - x^3) \, dx = \frac{1}{3} - \frac{1}{4} = \frac{1}{12}

medium — 1 mark


Verify Stokes’ Theorem for F=(z,x,y)\mathbf{F} = (z, x, y) on the hemisphere z=1x2y2z = \sqrt{1 - x^2 - y^2} with boundary CC the unit circle in the xyxy-plane.

Solution:

On CC: r(t)=(cost,sint,0)\mathbf{r}(t) = (\cos t, \sin t, 0), r(t)=(sint,cost,0)\mathbf{r}'(t) = (-\sin t, \cos t, 0).

CFdr=02π(0(sint)+costcost+sint0)dt=02πcos2tdt=π\oint_C \mathbf{F} \cdot d\mathbf{r} = \int_0^{2\pi} (0 \cdot (-\sin t) + \cos t \cdot \cos t + \sin t \cdot 0) \, dt = \int_0^{2\pi} \cos^2 t \, dt = \pi

For the surface integral, ×F=(1,1,1)\nabla \times \mathbf{F} = (1, 1, 1). On the hemisphere with outward normal:

S(×F)dS=Sx+y+z1x2y211x2y2dA\iint_S (\nabla \times \mathbf{F}) \cdot d\mathbf{S} = \iint_S \frac{x + y + z}{\sqrt{1-x^2-y^2}} \cdot \frac{1}{\sqrt{1-x^2-y^2}} \, dA

By symmetry, xdA=ydA=0\iint x \, dA = \iint y \, dA = 0, leaving:

Dzz2z2dA=D1dA=π\iint_D \frac{z}{z^2} \cdot z^2 \, dA = \iint_D 1 \, dA = \pi

Both integrals equal π\pi, confirming Stokes’ Theorem.

hard — 1 mark


Find the second-order Taylor expansion of f(x,y)=excos(y)f(x,y) = e^{x}\cos(y) about the origin.

Solution:

At the origin: f(0,0)=1f(0,0) = 1.

First partials: fx=excosyf_x = e^x \cos y, fy=exsinyf_y = -e^x \sin y. At (0,0)(0,0): fx=1f_x = 1, fy=0f_y = 0.

Second partials: fxx=excosyf_{xx} = e^x \cos y, fxy=exsinyf_{xy} = -e^x \sin y, fyy=excosyf_{yy} = -e^x \cos y. At (0,0)(0,0): fxx=1f_{xx} = 1, fxy=0f_{xy} = 0, fyy=1f_{yy} = -1.

T2(x,y)=1+x+12(x2y2)+T_2(x,y) = 1 + x + \frac{1}{2}(x^2 - y^2) + \cdots

easy — 1 mark


Find the maximum and minimum values of f(x,y,z)=x+2y+3zf(x,y,z) = x + 2y + 3z subject to x2+y2+z2=1x^2 + y^2 + z^2 = 1.

Solution:

f=(1,2,3)\nabla f = (1, 2, 3), g=(2x,2y,2z)\nabla g = (2x, 2y, 2z) where g=x2+y2+z21g = x^2 + y^2 + z^2 - 1.

f=λg\nabla f = \lambda \nabla g gives 1=2λx1 = 2\lambda x, 2=2λy2 = 2\lambda y, 3=2λz3 = 2\lambda z, so x=1/(2λ)x = 1/(2\lambda), y=2/(2λ)y = 2/(2\lambda), z=3/(2λ)z = 3/(2\lambda).

Substituting into the constraint:

1+4+94λ2=1    λ=±142\frac{1 + 4 + 9}{4\lambda^2} = 1 \implies \lambda = \pm\frac{\sqrt{14}}{2}

Maximum: f=12λ(1+4+9)=142λ=14f = \frac{1}{2\lambda}(1 + 4 + 9) = \frac{14}{2\lambda} = \sqrt{14} at (x,y,z)=114(1,2,3)(x,y,z) = \frac{1}{\sqrt{14}}(1,2,3).

Minimum: f=14f = -\sqrt{14} at (x,y,z)=114(1,2,3)(x,y,z) = -\frac{1}{\sqrt{14}}(1,2,3).

medium — 1 mark


Find the eigenvalues and eigenvectors of the matrix:

A=(310020005)A = \begin{pmatrix} 3 & 1 & 0 \\ 0 & 2 & 0 \\ 0 & 0 & 5 \end{pmatrix}

Solution:

The characteristic polynomial is:

det(AλI)=(3λ)(2λ)(5λ)=0\det(A - \lambda I) = (3-\lambda)(2-\lambda)(5-\lambda) = 0

Eigenvalues: λ1=2\lambda_1 = 2, λ2=3\lambda_2 = 3, λ3=5\lambda_3 = 5.

For λ1=2\lambda_1 = 2: (A2I)v=0(A - 2I)\mathbf{v} = 0 gives v1=(1,1,0)T\mathbf{v}_1 = (1, -1, 0)^T.

For λ2=3\lambda_2 = 3: (A3I)v=0(A - 3I)\mathbf{v} = 0 gives v2=(1,0,0)T\mathbf{v}_2 = (1, 0, 0)^T.

For λ3=5\lambda_3 = 5: (A5I)v=0(A - 5I)\mathbf{v} = 0 gives v3=(0,0,1)T\mathbf{v}_3 = (0, 0, 1)^T.

easy — 1 mark


Determine whether the matrix A=(1201)A = \begin{pmatrix} 1 & 2 \\ 0 & 1 \end{pmatrix} is diagonalisable.

Solution:

The characteristic polynomial is (1λ)2=0(1-\lambda)^2 = 0, giving a repeated eigenvalue λ=1\lambda = 1 with algebraic multiplicity 2.

(AI)=(0200)(A - I) = \begin{pmatrix} 0 & 2 \\ 0 & 0 \end{pmatrix}. The null space is spanned by (1,0)T(1, 0)^T, so the geometric multiplicity is 1.

Since the geometric multiplicity (1) is less than the algebraic multiplicity (2), AA is not diagonalisable.

easy — 1 mark


Let V=P2(R)V = P_2(\mathbb{R}) with inner product f,g=01f(x)g(x)dx\langle f, g \rangle = \int_0^1 f(x)g(x) \, dx. Apply the Gram-Schmidt process to the basis {1,x,x2}\{1, x, x^2\}.

Solution:

e1=1e_1 = 1.

e2=xx,11,11=x1/21=x12e_2 = x - \frac{\langle x, 1 \rangle}{\langle 1, 1 \rangle} \cdot 1 = x - \frac{1/2}{1} = x - \frac{1}{2}.

x2,1=13\langle x^2, 1 \rangle = \frac{1}{3}, x2,x1/2=01x2(x1/2)dx=1416=112\langle x^2, x - 1/2 \rangle = \int_0^1 x^2(x - 1/2) \, dx = \frac{1}{4} - \frac{1}{6} = \frac{1}{12}.

x1/2,x1/2=01(x1/2)2dx=112\langle x - 1/2, x - 1/2 \rangle = \int_0^1 (x - 1/2)^2 \, dx = \frac{1}{12}.

e3=x21/3111/121/12(x12)=x2x+16e_3 = x^2 - \frac{1/3}{1} \cdot 1 - \frac{1/12}{1/12}\left(x - \frac{1}{2}\right) = x^2 - x + \frac{1}{6}

The orthogonal basis is {1,x12,x2x+16}\left\{1, \, x - \frac{1}{2}, \, x^2 - x + \frac{1}{6}\right\}.

medium — 1 mark


Let T:R3R3T: \mathbb{R}^3 \to \mathbb{R}^3 be defined by T(x,y,z)=(x+y,y+z,z+x)T(x,y,z) = (x + y, y + z, z + x). Find the rank and nullity of TT.

Solution:

The matrix of TT relative to the standard basis is:

A=(110011101)A = \begin{pmatrix} 1 & 1 & 0 \\ 0 & 1 & 1 \\ 1 & 0 & 1 \end{pmatrix}

Row reducing:

(110011011)(110011002)\begin{pmatrix} 1 & 1 & 0 \\ 0 & 1 & 1 \\ 0 & -1 & 1 \end{pmatrix} \to \begin{pmatrix} 1 & 1 & 0 \\ 0 & 1 & 1 \\ 0 & 0 & 2 \end{pmatrix}

The rank is 3 and the nullity is 0 (since det(A)=20\det(A) = 2 \neq 0). TT is invertible.

easy — 1 mark


Classify the quadratic form Q(x,y,z)=x2+4y2+z2+2xy2xzQ(x,y,z) = x^2 + 4y^2 + z^2 + 2xy - 2xz.

Solution:

The associated symmetric matrix is:

A=(111140101)A = \begin{pmatrix} 1 & 1 & -1 \\ 1 & 4 & 0 \\ -1 & 0 & 1 \end{pmatrix}

Leading principal minors: Δ1=1>0\Delta_1 = 1 > 0, Δ2=41=3>0\Delta_2 = 4 - 1 = 3 > 0, Δ3=det(A)=1(4)1(1)+(1)(4)=414=1<0\Delta_3 = \det(A) = 1(4) - 1(1) + (-1)(4) = 4 - 1 - 4 = -1 < 0.

By Sylvester’s criterion, AA has signature (2,1)(2, 1): two positive eigenvalues and one negative eigenvalue. The quadratic form is indefinite.

medium — 1 mark


Prove that the set of all 2×22 \times 2 symmetric matrices forms a subspace of M2×2(R)M_{2 \times 2}(\mathbb{R}), and find its dimension.

Solution:

Let W={AM2×2:AT=A}W = \{A \in M_{2 \times 2} : A^T = A\}.

  1. Zero matrix: 0T=00^T = 0, so 0W0 \in W.

  2. Closure under addition: If AT=AA^T = A and BT=BB^T = B, then (A+B)T=AT+BT=A+B(A+B)^T = A^T + B^T = A + B, so A+BWA + B \in W.

  3. Closure under scalar multiplication: (cA)T=cAT=cA(cA)^T = cA^T = cA, so cAWcA \in W.

A general symmetric 2×22 \times 2 matrix has the form (abbd)\begin{pmatrix} a & b \\ b & d \end{pmatrix}, parameterised by (a,b,d)(a, b, d). The basis is:

{(1000),(0110),(0001)}\left\{\begin{pmatrix} 1 & 0 \\ 0 & 0 \end{pmatrix}, \begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix}, \begin{pmatrix} 0 & 0 \\ 0 & 1 \end{pmatrix}\right\}

The dimension is 3.

medium — 1 mark


State the Spectral Theorem for real symmetric matrices and sketch a proof outline.

Solution:

Theorem: If AA is a real symmetric matrix (A=ATA = A^T), then AA is orthogonally diagonalisable: there exists an orthogonal matrix QQ (QTQ=IQ^T Q = I) and a diagonal matrix DD such that A=QDQTA = QDQ^T.

Proof outline:

  1. Real eigenvalues: The characteristic polynomial of AA has real coefficients, and since AA is symmetric, all eigenvalues are real (if λ\lambda is complex with eigenvector v\mathbf{v}, then λˉ=λ\bar{\lambda} = \lambda follows from A=ATA = A^T).

  2. Orthogonal eigenvectors: If v1\mathbf{v}_1 and v2\mathbf{v}_2 are eigenvectors of AA with distinct eigenvalues λ1λ2\lambda_1 \neq \lambda_2, then v1v2=0\mathbf{v}_1 \cdot \mathbf{v}_2 = 0. This follows from λ1v1v2=(Av1)v2=v1(Av2)=λ2v1v2\lambda_1 \mathbf{v}_1 \cdot \mathbf{v}_2 = (A\mathbf{v}_1) \cdot \mathbf{v}_2 = \mathbf{v}_1 \cdot (A\mathbf{v}_2) = \lambda_2 \mathbf{v}_1 \cdot \mathbf{v}_2.

  3. Orthonormal basis: By induction on dimension, we can construct an orthonormal basis of eigenvectors, giving A=QDQTA = QDQ^T.

hard — 1 mark


Find the Jordan normal form of A=(210021002)A = \begin{pmatrix} 2 & 1 & 0 \\ 0 & 2 & 1 \\ 0 & 0 & 2 \end{pmatrix} and compute A10A^{10}.

Solution:

AA already has the Jordan normal form J=(210021002)J = \begin{pmatrix} 2 & 1 & 0 \\ 0 & 2 & 1 \\ 0 & 0 & 2 \end{pmatrix} with eigenvalue λ=2\lambda = 2 of algebraic multiplicity 3 and geometric multiplicity 1.

We write A=2I+NA = 2I + N where N=(010001000)N = \begin{pmatrix} 0 & 1 & 0 \\ 0 & 0 & 1 \\ 0 & 0 & 0 \end{pmatrix} is nilpotent (N3=0N^3 = 0).

Using the binomial theorem (valid since 2I2I and NN commute):

A10=k=02(10k)210kNk=210I+1029N+4528N2A^{10} = \sum_{k=0}^{2} \binom{10}{k} 2^{10-k} N^k = 2^{10}I + 10 \cdot 2^9 N + 45 \cdot 2^8 N^2

=(102400010240001024)+(051200005120000)+(0011520000000)= \begin{pmatrix} 1024 & 0 & 0 \\ 0 & 1024 & 0 \\ 0 & 0 & 1024 \end{pmatrix} + \begin{pmatrix} 0 & 5120 & 0 \\ 0 & 0 & 5120 \\ 0 & 0 & 0 \end{pmatrix} + \begin{pmatrix} 0 & 0 & 11520 \\ 0 & 0 & 0 \\ 0 & 0 & 0 \end{pmatrix}

A10=(1024512011520010245120001024)A^{10} = \begin{pmatrix} 1024 & 5120 & 11520 \\ 0 & 1024 & 5120 \\ 0 & 0 & 1024 \end{pmatrix}

hard — 1 mark


Prove that every group of order 4 is abelian.

Solution:

Let G=4|G| = 4. By Lagrange’s theorem, every non-identity element has order 2 or 4.

Case 1: GG contains an element of order 4. Then G=aZ4G = \langle a \rangle \cong \mathbb{Z}_4, which is abelian.

Case 2: Every non-identity element has order 2. Then g2=eg^2 = e for all gGg \in G, so g=g1g = g^{-1}. For any a,bGa, b \in G:

ab=(ab)1=b1a1=baab = (ab)^{-1} = b^{-1}a^{-1} = ba

Therefore GG is abelian. In fact, GZ2×Z2G \cong \mathbb{Z}_2 \times \mathbb{Z}_2 (the Klein four-group).

medium — 1 mark


Prove that in an integral domain, the cancellation law holds: if ab=acab = ac and a0a \neq 0, then b=cb = c.

Solution:

Let DD be an integral domain and suppose ab=acab = ac with a0a \neq 0.

Then abac=0ab - ac = 0, so a(bc)=0a(b - c) = 0.

Since DD is an integral domain, it has no zero divisors: if xy=0xy = 0 then x=0x = 0 or y=0y = 0.

Since a0a \neq 0, we must have bc=0b - c = 0, i.e., b=cb = c.

easy — 1 mark


Let HH be a subgroup of index 2 in a group GG. Prove that HH is normal in GG.

Solution:

Since [G:H]=2[G:H] = 2, there are exactly two left cosets of HH in GG: HH itself and GH=aHG \setminus H = aH for any aHa \notin H. Similarly, the right cosets are HH and Ha=GHHa = G \setminus H.

For any gGg \in G:

  • If gHg \in H, then gH=H=HggH = H = Hg.
  • If gHg \notin H, then gH=GH=HggH = G \setminus H = Hg.

In both cases, gH=HggH = Hg for all gGg \in G, so HGH \trianglelefteq G.

medium — 1 mark


Let ϕ:GH\phi: G \to H be a group homomorphism. Prove that ker(ϕ)\ker(\phi) is a normal subgroup of GG.

Solution:

  1. Subgroup: ϕ(eG)=eH\phi(e_G) = e_H, so eGker(ϕ)e_G \in \ker(\phi). If a,bker(ϕ)a, b \in \ker(\phi), then ϕ(ab1)=ϕ(a)ϕ(b)1=eHeH=eH\phi(ab^{-1}) = \phi(a)\phi(b)^{-1} = e_H \cdot e_H = e_H, so ab1ker(ϕ)ab^{-1} \in \ker(\phi).

  2. Normal: For any gGg \in G and kker(ϕ)k \in \ker(\phi):

ϕ(gkg1)=ϕ(g)ϕ(k)ϕ(g)1=ϕ(g)eHϕ(g)1=eH\phi(gkg^{-1}) = \phi(g)\phi(k)\phi(g)^{-1} = \phi(g) \cdot e_H \cdot \phi(g)^{-1} = e_H

So gkg1ker(ϕ)gkg^{-1} \in \ker(\phi), proving ker(ϕ)G\ker(\phi) \trianglelefteq G.

medium — 1 mark


Find the gcd of f(x)=x4+1f(x) = x^4 + 1 and g(x)=x3+x+1g(x) = x^3 + x + 1 in F2[x]\mathbb{F}_2[x] using the Euclidean algorithm.

Solution:

Working in F2\mathbb{F}_2 (where 1=1-1 = 1):

x4+1=(x+1)(x3+x+1)+(x2+x+1)x^4 + 1 = (x + 1)(x^3 + x + 1) + (x^2 + x + 1)

x3+x+1=x(x2+x+1)+(x2+x+1)+(x2+1)=(x+1)(x2+x+1)+xx^3 + x + 1 = x(x^2 + x + 1) + (x^2 + x + 1) + (x^2 + 1) = (x+1)(x^2+x+1) + x

Wait, let me redo this more carefully:

Dividing x3+x+1x^3 + x + 1 by x2+x+1x^2 + x + 1:

x3+x+1=x(x2+x+1)+(x2+x+1)+x3+x+1x(x2+x+1)x^3 + x + 1 = x \cdot (x^2 + x + 1) + (x^2 + x + 1) + x^3 + x + 1 - x(x^2+x+1)

x(x2+x+1)=x3+x2+xx(x^2+x+1) = x^3 + x^2 + x

x3+x+1(x3+x2+x)=x2+1x^3 + x + 1 - (x^3 + x^2 + x) = x^2 + 1

So x3+x+1=x(x2+x+1)+(x2+1)x^3 + x + 1 = x(x^2 + x + 1) + (x^2 + 1).

Now dividing x2+x+1x^2 + x + 1 by x2+1x^2 + 1:

x2+x+1=1(x2+1)+xx^2 + x + 1 = 1 \cdot (x^2 + 1) + x

Dividing x2+1x^2 + 1 by xx:

x2+1=xx+1x^2 + 1 = x \cdot x + 1

Dividing xx by 11:

x=x1+0x = x \cdot 1 + 0

The last nonzero remainder is 11, so gcd(f,g)=1\gcd(f, g) = 1 — they are coprime.

hard — 1 mark


Find the degree [Q(2,3):Q][\mathbb{Q}(\sqrt{2}, \sqrt{3}) : \mathbb{Q}] and construct a basis.

Solution:

We build the extension in stages:

[Q(2):Q]=2[\mathbb{Q}(\sqrt{2}) : \mathbb{Q}] = 2 with basis {1,2}\{1, \sqrt{2}\}, since x22x^2 - 2 is irreducible over Q\mathbb{Q}.

[Q(2,3):Q(2)]=2[\mathbb{Q}(\sqrt{2}, \sqrt{3}) : \mathbb{Q}(\sqrt{2})] = 2 with basis {1,3}\{1, \sqrt{3}\} over Q(2)\mathbb{Q}(\sqrt{2}), since 3Q(2)\sqrt{3} \notin \mathbb{Q}(\sqrt{2}) (if 3=a+b2\sqrt{3} = a + b\sqrt{2} then 3=a2+2b2+2ab23 = a^2 + 2b^2 + 2ab\sqrt{2}, forcing ab=0ab = 0, which gives a contradiction).

By the tower law:

[Q(2,3):Q]=[Q(2,3):Q(2)][Q(2):Q]=22=4[\mathbb{Q}(\sqrt{2}, \sqrt{3}) : \mathbb{Q}] = [\mathbb{Q}(\sqrt{2}, \sqrt{3}) : \mathbb{Q}(\sqrt{2})] \cdot [\mathbb{Q}(\sqrt{2}) : \mathbb{Q}] = 2 \cdot 2 = 4

A basis is {1,2,3,6}\{1, \sqrt{2}, \sqrt{3}, \sqrt{6}\}.

medium — 1 mark


Use the Sylow theorems to show that every group of order 15 is cyclic.

Solution:

G=15=35|G| = 15 = 3 \cdot 5.

By Sylow’s theorems:

  • The number n5n_5 of Sylow 5-subgroups satisfies n51(mod5)n_5 \equiv 1 \pmod{5} and n53n_5 \mid 3. So n5=1n_5 = 1.
  • The number n3n_3 of Sylow 3-subgroups satisfies n31(mod3)n_3 \equiv 1 \pmod{3} and n35n_3 \mid 5. So n3=1n_3 = 1.

Since both Sylow subgroups are unique, they are normal. Let PZ5P \cong \mathbb{Z}_5 and QZ3Q \cong \mathbb{Z}_3. Since PQ={e}P \cap Q = \{e\} and PQ=GPQ = G, we have GP×QZ5×Z3Z15G \cong P \times Q \cong \mathbb{Z}_5 \times \mathbb{Z}_3 \cong \mathbb{Z}_{15} (since gcd(3,5)=1\gcd(3,5) = 1). Therefore GG is cyclic.

medium — 1 mark


Prove that the sequence an=nn+1a_n = \frac{n}{n+1} converges, and find its limit.

Solution:

Claim: an1a_n \to 1 as nn \to \infty.

Proof: For any ϵ>0\epsilon > 0, choose N>1ϵN > \frac{1}{\epsilon}. For all n>Nn > N:

an1=nn+11=1n+1<1n<1N<ϵ|a_n - 1| = \left|\frac{n}{n+1} - 1\right| = \frac{1}{n+1} < \frac{1}{n} < \frac{1}{N} < \epsilon

Therefore limnan=1\lim_{n \to \infty} a_n = 1.

easy — 1 mark


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

Solution:

Apply the ratio test:

an+1an=(n+1)22n+12nn2=12(n+1n)212<1\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 \to \frac{1}{2} < 1

Since the limit is less than 1, the series converges by the ratio test.

easy — 1 mark


Prove that f(x)=x2f(x) = x^2 is continuous at x=3x = 3 using the ϵ\epsilon-δ\delta definition.

Solution:

We need: for every ϵ>0\epsilon > 0, there exists δ>0\delta > 0 such that x3<δ    x29<ϵ|x - 3| < \delta \implies |x^2 - 9| < \epsilon.

x29=x3x+3|x^2 - 9| = |x - 3| \cdot |x + 3|.

If x3<1|x - 3| < 1, then 2<x<42 < x < 4, so x+3<7|x + 3| < 7.

Choose δ=min(1,ϵ7)\delta = \min\left(1, \frac{\epsilon}{7}\right). Then:

x29=x3x+3<δ7ϵ|x^2 - 9| = |x - 3| \cdot |x + 3| < \delta \cdot 7 \leq \epsilon

medium — 1 mark


Show that fn(x)=xnf_n(x) = \frac{x}{n} converges pointwise but not uniformly on R\mathbb{R}.

Solution:

Pointwise convergence: For each fixed xRx \in \mathbb{R}:

limnfn(x)=limnxn=0\lim_{n \to \infty} f_n(x) = \lim_{n \to \infty} \frac{x}{n} = 0

So fnff_n \to f where f(x)=0f(x) = 0.

Not uniform: For uniform convergence, we need supxRfn(x)f(x)0\sup_{x \in \mathbb{R}} |f_n(x) - f(x)| \to 0. But:

supxRxn=\sup_{x \in \mathbb{R}} \frac{|x|}{n} = \infty

for every nn, so the convergence is not uniform on R\mathbb{R}.

(Note: convergence is uniform on any bounded subset [M,M][-M, M] since supxn=Mn0\sup \frac{|x|}{n} = \frac{M}{n} \to 0.)

medium — 1 mark


State and prove the Mean Value Theorem.

Solution:

Theorem: If ff is continuous on [a,b][a,b] and differentiable on (a,b)(a,b), then there exists c(a,b)c \in (a,b) such that:

f(c)=f(b)f(a)baf'(c) = \frac{f(b) - f(a)}{b - a}

Proof: Define g(x)=f(x)f(a)f(b)f(a)ba(xa)g(x) = f(x) - f(a) - \frac{f(b)-f(a)}{b-a}(x-a). Then g(a)=g(b)=0g(a) = g(b) = 0.

By Rolle’s theorem (since gg is continuous on [a,b][a,b], differentiable on (a,b)(a,b), and g(a)=g(b)g(a) = g(b)), there exists c(a,b)c \in (a,b) with g(c)=0g'(c) = 0.

g(c)=f(c)f(b)f(a)ba=0g'(c) = f'(c) - \frac{f(b)-f(a)}{b-a} = 0, giving f(c)=f(b)f(a)baf'(c) = \frac{f(b)-f(a)}{b-a}.

hard — 1 mark


Prove that if ff is Riemann integrable on [a,b][a,b] and f(x)0f(x) \geq 0 for all xx, then abf(x)dx0\int_a^b f(x) \, dx \geq 0.

Solution:

For any partition P={x0,x1,,xn}P = \{x_0, x_1, \ldots, x_n\} of [a,b][a,b], the lower Darboux sum is:

L(f,P)=i=1nmiΔxiL(f, P) = \sum_{i=1}^n m_i \Delta x_i

where mi=infx[xi1,xi]f(x)m_i = \inf_{x \in [x_{i-1}, x_i]} f(x). Since f(x)0f(x) \geq 0 everywhere, mi0m_i \geq 0 for all ii, and Δxi>0\Delta x_i > 0, so L(f,P)0L(f, P) \geq 0.

The Riemann integral is abf=supPL(f,P)0\int_a^b f = \sup_P L(f, P) \geq 0.

medium — 1 mark


Prove that a closed and bounded subset of R\mathbb{R} is compact (Heine-Borel theorem).

Solution:

Theorem: A subset KRK \subseteq \mathbb{R} is compact if and only if it is closed and bounded.

Proof (\Rightarrow): If KK is compact, consider the open cover {(n,n):nN}\{(-n, n) : n \in \mathbb{N}\}. This has a finite subcover {(n1,n1),,(nk,nk)}\{(-n_1, n_1), \ldots, (-n_k, n_k)\}, so K(N,N)K \subseteq (-N, N) where N=max(ni)N = \max(n_i). Thus KK is bounded.

To show KK is closed, suppose xx is a limit point of KK but xKx \notin K. For each kNk \in \mathbb{N}, the set Uk=R[x1/k,x+1/k]U_k = \mathbb{R} \setminus [x - 1/k, x + 1/k] is open. The family {Uk}\{U_k\} covers KK (since xKx \notin K, each point of KK is at positive distance from xx). By compactness, KUk1Ukm=R[x1/N,x+1/N]K \subseteq U_{k_1} \cup \cdots \cup U_{k_m} = \mathbb{R} \setminus [x - 1/N, x + 1/N] where N=max(ki)N = \max(k_i). But xx is a limit point, so K(x1/N,x+1/N)K \cap (x - 1/N, x + 1/N) \neq \emptyset — contradiction.

hard — 1 mark


Click to reveal the answer key
ProblemKey Result
P1(e - 1)/2
P220/3
P32 pi^2
P48 pi
P51/12
P6Both integrals equal pi
P71 + x + (x^2 - y^2)/2
P8Maximum: sqrt(14); Minimum: -sqrt(14)
ProblemKey Result
P9lambda = 2, 3, 5 with eigenvectors (1,-1,0), (1,0,0), (0,0,1)
P10Not diagonalisable (geometric multiplicity < algebraic)
P11{1, x - 1/2, x^2 - x + 1/6}
P12Rank 3, nullity 0
P13Indefinite (signature (2,1))
P14Dimension 3
P15A = QDQ^T with Q orthogonal
P16J with eigenvalue 2, A^10 = 2^10 I + 102^9 N + 452^8 N^2
ProblemKey Result
P17All groups of order 4 are abelian
P18Cancellation follows from no zero divisors
P19Index 2 subgroups are always normal
P20Kernel is always normal
P21gcd = 1 (coprime)
P22Degree 4, basis {1, sqrt(2), sqrt(3), sqrt(6)}
P23G is cyclic (Z_15)
ProblemKey Result
P24Limit is 1
P25Converges (ratio test)
P26delta = min(1, epsilon/7)
P27Pointwise yes, uniform no
P28MVT: f’(c) = (f(b) - f(a))/(b - a)
P29Integral is non-negative
P30Heine-Borel: closed and bounded iff compact

DifficultyCount
Easy7
Medium17
Hard6


  1. Write complete proofs. University mathematics demands rigour — every claim must be justified.
  2. Check your work. Verify dimensions, signs, and boundary cases. Dimensional analysis catches many errors.
  3. Study the proof techniques. The solutions demonstrate key methods: induction, contradiction, construction, and the ϵ\epsilon-δ\delta argument.
  4. Understand definitions. Many problems test whether you can apply definitions precisely (e.g., uniform convergence, normal subgroups).
  5. Retake after one week. Mathematics requires understanding, not memorisation. Spaced repetition builds lasting knowledge.

Last updated: 24 July 2026

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