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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:

∬Dex2 dA\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 0≤x≤10 \leq x \leq 1 and 0≤y≤x0 \leq y \leq x. Since ex2e^{x^2} has no elementary antiderivative with respect to xx, we must integrate with respect to yy first:

∫01∫0xex2 dy dx=∫01x ex2 dx\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=2x dxdu = 2x \, dx:

=12∫01eu du=12(e−1)= \frac{1}{2} \int_0^1 e^u \, du = \frac{1}{2}(e - 1)

medium1 mark


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=2i−j+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, 1−1, 3⋅2⋅1)=(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=∇f⋅v^=13(8+0+12)=203D_{\hat{\mathbf{v}}} f = \nabla f \cdot \hat{\mathbf{v}} = \frac{1}{3}(8 + 0 + 12) = \frac{20}{3}

medium1 mark


Compute the line integral ∫CF⋅dr\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)=(cos⁡t,sin⁡t,t)\mathbf{r}(t) = (\cos t, \sin t, t) for 0≤t≤2π0 \leq t \leq 2\pi.

Solution:

r′(t)=(−sin⁡t,cos⁡t,1)\mathbf{r}'(t) = (-\sin t, \cos t, 1).

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

F⋅r′=−sin⁡2t+cos⁡2t+t=cos⁡2t+t\mathbf{F} \cdot \mathbf{r}' = -\sin^2 t + \cos^2 t + t = \cos 2t + t ∫02π(cos⁡2t+t) dt=[sin⁡2t2+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

medium1 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+y2≤3x^2 + y^2 \leq 3 at z=1z = 1:

∭V(∇⋅F) dV=∭V3 dV=3 Vol(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(3R−h)=π3(6−1)=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=−∬disk1 dA=−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=3⋅5π3−(−3π)=5π+3π=8π\Phi_{\text{cap}} = 3 \cdot \frac{5\pi}{3} - (-3\pi) = 5\pi + 3\pi = 8\pi

hard1 mark


Use Green’s Theorem to evaluate ∮C(xy dx+x2 dy)\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:

∮CP dx+Q dy=∬D(∂Q∂x−∂P∂y)dA=∬D(2x−x) dA=∬Dx dA\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 0≤x≤10 \leq x \leq 1:

∫01∫x2xx dy dx=∫01x(x−x2) dx=∫01(x2−x3) dx=13−14=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}

medium1 mark


Verify Stokes’ Theorem for F=(z,x,y)\mathbf{F} = (z, x, y) on the hemisphere z=1−x2−y2z = \sqrt{1 - x^2 - y^2} with boundary CC the unit circle in the xyxy-plane.

Solution:

On CC: r(t)=(cos⁡t,sin⁡t,0)\mathbf{r}(t) = (\cos t, \sin t, 0), r′(t)=(−sin⁡t,cos⁡t,0)\mathbf{r}'(t) = (-\sin t, \cos t, 0).

∮CF⋅dr=∫02π(0⋅(−sin⁡t)+cos⁡t⋅cos⁡t+sin⁡t⋅0) dt=∫02πcos⁡2t dt=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+z1−x2−y2⋅11−x2−y2 dA\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, ∬x dA=∬y dA=0\iint x \, dA = \iint y \, dA = 0, leaving:

∬Dzz2⋅z2 dA=∬D1 dA=π\iint_D \frac{z}{z^2} \cdot z^2 \, dA = \iint_D 1 \, dA = \pi

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

hard1 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=excos⁡yf_x = e^x \cos y, fy=−exsin⁡yf_y = -e^x \sin y. At (0,0)(0,0): fx=1f_x = 1, fy=0f_y = 0.

Second partials: fxx=excos⁡yf_{xx} = e^x \cos y, fxy=−exsin⁡yf_{xy} = -e^x \sin y, fyy=−excos⁡yf_{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(x2−y2)+⋯T_2(x,y) = 1 + x + \frac{1}{2}(x^2 - y^2) + \cdots

easy1 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+z2−1g = x^2 + y^2 + z^2 - 1.

∇f=λ∇g\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).

medium1 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⁡(A−λI)=(3−λ)(2−λ)(5−λ)=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: (A−2I)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: (A−3I)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: (A−5I)v=0(A - 5I)\mathbf{v} = 0 gives v3=(0,0,1)T\mathbf{v}_3 = (0, 0, 1)^T.

easy1 mark


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

Solution:

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

(A−I)=(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.

easy1 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=x−⟨x,1⟩⟨1,1⟩⋅1=x−1/21=x−12e_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,x−1/2⟩=∫01x2(x−1/2) dx=14−16=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}.

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

e3=x2−1/31⋅1−1/121/12(x−12)=x2−x+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, x−12, x2−x+16}\left\{1, \, x - \frac{1}{2}, \, x^2 - x + \frac{1}{6}\right\}.

medium1 mark


Let T:R3→R3T: \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:

(1100110−11)→(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)=2≠0\det(A) = 2 \neq 0). TT is invertible.

easy1 mark


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

Solution:

The associated symmetric matrix is:

A=(11−1140−101)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=4−1=3>0\Delta_2 = 4 - 1 = 3 > 0, Δ3=det⁡(A)=1(4)−1(1)+(−1)(4)=4−1−4=−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.

medium1 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={A∈M2×2:AT=A}W = \{A \in M_{2 \times 2} : A^T = A\}.

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

  3. Closure under scalar multiplication: (cA)T=cAT=cA(cA)^T = cA^T = cA, so cA∈WcA \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.

medium1 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 λ1≠λ2\lambda_1 \neq \lambda_2, then v1⋅v2=0\mathbf{v}_1 \cdot \mathbf{v}_2 = 0. This follows from λ1v1⋅v2=(Av1)⋅v2=v1⋅(Av2)=λ2v1⋅v2\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.

hard1 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)210−kNk=210I+10⋅29N+45⋅28N2A^{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}

hard1 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=⟨a⟩≅Z4G = \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 g∈Gg \in G, so g=g−1g = g^{-1}. For any a,b∈Ga, b \in G:

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

Therefore GG is abelian. In fact, G≅Z2×Z2G \cong \mathbb{Z}_2 \times \mathbb{Z}_2 (the Klein four-group).

medium1 mark


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

Solution:

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

Then ab−ac=0ab - ac = 0, so a(b−c)=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 a≠0a \neq 0, we must have b−c=0b - c = 0, i.e., b=cb = c.

easy1 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 G∖H=aHG \setminus H = aH for any a∉Ha \notin H. Similarly, the right cosets are HH and Ha=G∖HHa = G \setminus H.

For any g∈Gg \in G:

  • If g∈Hg \in H, then gH=H=HggH = H = Hg.
  • If g∉Hg \notin H, then gH=G∖H=HggH = G \setminus H = Hg.

In both cases, gH=HggH = Hg for all g∈Gg \in G, so H⊴GH \trianglelefteq G.

medium1 mark


Let ϕ:G→H\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 eG∈ker⁡(ϕ)e_G \in \ker(\phi). If a,b∈ker⁡(ϕ)a, b \in \ker(\phi), then ϕ(ab−1)=ϕ(a)ϕ(b)−1=eH⋅eH=eH\phi(ab^{-1}) = \phi(a)\phi(b)^{-1} = e_H \cdot e_H = e_H, so ab−1∈ker⁡(ϕ)ab^{-1} \in \ker(\phi).

  2. Normal: For any g∈Gg \in G and k∈ker⁡(ϕ)k \in \ker(\phi):

ϕ(gkg−1)=ϕ(g)ϕ(k)ϕ(g)−1=ϕ(g)⋅eH⋅ϕ(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 gkg−1∈ker⁡(ϕ)gkg^{-1} \in \ker(\phi), proving ker⁡(ϕ)⊴G\ker(\phi) \trianglelefteq G.

medium1 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+1−x(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=x⋅x+1x^2 + 1 = x \cdot x + 1

Dividing xx by 11:

x=x⋅1+0x = x \cdot 1 + 0

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

hard1 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 x2−2x^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 3∉Q(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]=2⋅2=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}\}.

medium1 mark


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

Solution:

∣G∣=15=3⋅5|G| = 15 = 3 \cdot 5.

By Sylow’s theorems:

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

Since both Sylow subgroups are unique, they are normal. Let P≅Z5P \cong \mathbb{Z}_5 and Q≅Z3Q \cong \mathbb{Z}_3. Since P∩Q={e}P \cap Q = \{e\} and PQ=GPQ = G, we have G≅P×Q≅Z5×Z3≅Z15G \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.

medium1 mark


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

Solution:

Claim: an→1a_n \to 1 as n→∞n \to \infty.

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

∣an−1∣=∣nn+1−1∣=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 lim⁡n→∞an=1\lim_{n \to \infty} a_n = 1.

easy1 mark


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

Solution:

Apply the ratio test:

an+1an=(n+1)22n+1⋅2nn2=12(n+1n)2→12<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.

easy1 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 ∣x−3∣<δ  ⟹  ∣x2−9∣<ϵ|x - 3| < \delta \implies |x^2 - 9| < \epsilon.

∣x2−9∣=∣x−3∣⋅∣x+3∣|x^2 - 9| = |x - 3| \cdot |x + 3|.

If ∣x−3∣<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:

∣x2−9∣=∣x−3∣⋅∣x+3∣<δ⋅7≤ϵ|x^2 - 9| = |x - 3| \cdot |x + 3| < \delta \cdot 7 \leq \epsilon

medium1 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 x∈Rx \in \mathbb{R}:

lim⁡n→∞fn(x)=lim⁡n→∞xn=0\lim_{n \to \infty} f_n(x) = \lim_{n \to \infty} \frac{x}{n} = 0

So fn→ff_n \to f where f(x)=0f(x) = 0.

Not uniform: For uniform convergence, we need sup⁡x∈R∣fn(x)−f(x)∣→0\sup_{x \in \mathbb{R}} |f_n(x) - f(x)| \to 0. But:

sup⁡x∈R∣x∣n=∞\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 sup⁡∣x∣n=Mn→0\sup \frac{|x|}{n} = \frac{M}{n} \to 0.)

medium1 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)b−af'(c) = \frac{f(b) - f(a)}{b - a}

Proof: Define g(x)=f(x)−f(a)−f(b)−f(a)b−a(x−a)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)b−a=0g'(c) = f'(c) - \frac{f(b)-f(a)}{b-a} = 0, giving f′(c)=f(b)−f(a)b−af'(c) = \frac{f(b)-f(a)}{b-a}.

hard1 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) dx≥0\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=inf⁡x∈[xi−1,xi]f(x)m_i = \inf_{x \in [x_{i-1}, x_i]} f(x). Since f(x)≥0f(x) \geq 0 everywhere, mi≥0m_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=sup⁡PL(f,P)≥0\int_a^b f = \sup_P L(f, P) \geq 0.

medium1 mark


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

Solution:

Theorem: A subset K⊆RK \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):n∈N}\{(-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 x∉Kx \notin K. For each k∈Nk \in \mathbb{N}, the set Uk=R∖[x−1/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 x∉Kx \notin K, each point of KK is at positive distance from xx). By compactness, K⊆Uk1∪⋯∪Ukm=R∖[x−1/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∩(x−1/N,x+1/N)≠∅K \cap (x - 1/N, x + 1/N) \neq \emptyset, contradiction.

hard1 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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