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Part IA Michaelmas, Lent, Easter Term

Methods I Tripos Questions

This section contains worked examples from past Tripos papers relevant to Methods I topics.


Limits and Continuity

Tripos 2016, Paper 2, Question 19Y

Calculate for real xx and constant aa:

(i) lim⁡x→0tan⁡xsin⁡xsin⁡3x\displaystyle\lim_{x \to 0} \frac{\tan x \sin x}{\sin^3 x}

(ii) lim⁡x→asin⁡x−sin⁡ax−a\displaystyle\lim_{x \to a} \frac{\sin x - \sin a}{x - a}

(iii) lim⁡x→∞(x+ax−a)x+a\displaystyle\lim_{x \to \infty} \left(\frac{x + a}{x - a}\right)^{x+a}

Solutions:

(i) Using tan⁡x=sin⁡xcos⁡x\tan x = \frac{\sin x}{\cos x}:

lim⁡x→0sin⁡2xcos⁡xsin⁡3x=lim⁡x→01cos⁡xsin⁡x\lim_{x \to 0} \frac{\sin^2 x}{\cos x \sin^3 x} = \lim_{x \to 0} \frac{1}{\cos x \sin x}

This doesn’t exist (goes to ∞\infty). Actually, let’s reconsider:

tan⁡xsin⁡xsin⁡3x=1cos⁡xsin⁡2x\frac{\tan x \sin x}{\sin^3 x} = \frac{1}{\cos x \sin^2 x}

Using sin⁡x∼x\sin x \sim x near 0: this behaves like 1x2\frac{1}{x^2}, so the limit is ∞\infty.

(ii) This is the derivative of sin⁡x\sin x at x=ax = a:

lim⁡x→asin⁡x−sin⁡ax−a=cos⁡a\lim_{x \to a} \frac{\sin x - \sin a}{x - a} = \cos a

Alternatively, use the identity sin⁡x−sin⁡a=2cos⁡x+a2sin⁡x−a2\sin x - \sin a = 2\cos\frac{x+a}{2}\sin\frac{x-a}{2}.

(iii) Let y=(x+ax−a)x+ay = \left(\frac{x+a}{x-a}\right)^{x+a}. Then:

ln⁡y=(x+a)ln⁡(1+2ax−a)\ln y = (x+a)\ln\left(1 + \frac{2a}{x-a}\right)

For large xx: ln⁡(1+2ax−a)∼2ax−a\ln\left(1 + \frac{2a}{x-a}\right) \sim \frac{2a}{x-a}

So ln⁡y∼(x+a)⋅2ax−a→2a\ln y \sim (x+a) \cdot \frac{2a}{x-a} \to 2a as x→∞x \to \infty.

Therefore: y→e2ay \to e^{2a}


Tripos 2008, Paper 1, Question 19X

A function is defined for integer n∈{0,1,2,3,4}n \in \{0, 1, 2, 3, 4\}:

ϕ(x,n)={xnsin⁡(1/x)x≠00x=0,n≠41x=0,n=4\phi(x, n) = \begin{cases} x^n \sin(1/x) & x \neq 0 \\ 0 & x = 0, n \neq 4 \\ 1 & x = 0, n = 4 \end{cases}

(i) Determine values of nn for which ϕ(x,n)\phi(x,n) tends to a limit as x→0x \to 0.

(ii) Determine values of nn for which ϕ(x,n)\phi(x,n) is continuous at x=0x = 0.

(iii) Determine values of nn for which ϕ(x,n)\phi(x,n) is differentiable at x=0x = 0.

Solutions:

(i) Limit exists if n>0n > 0. For n=0n = 0: sin⁡(1/x)\sin(1/x) oscillates. For n≥1n \geq 1: ∣xnsin⁡(1/x)∣≤∣x∣n→0|x^n \sin(1/x)| \leq |x|^n \to 0.

(ii) For continuity, need lim⁡x→0ϕ=ϕ(0)\lim_{x \to 0} \phi = \phi(0). The limit is 0 for n≥1n \geq 1, so we need ϕ(0)=0\phi(0) = 0. This holds for n∈{1,2,3}n \in \{1, 2, 3\}.

(iii) For differentiability:

ϕ′(0)=lim⁡h→0ϕ(h)−ϕ(0)h=lim⁡h→0hnsin⁡(1/h)h=lim⁡h→0hn−1sin⁡(1/h)\phi'(0) = \lim_{h \to 0} \frac{\phi(h) - \phi(0)}{h} = \lim_{h \to 0} \frac{h^n \sin(1/h)}{h} = \lim_{h \to 0} h^{n-1}\sin(1/h)

This exists (equals 0) if n−1>0n - 1 > 0, i.e., n∈{2,3}n \in \{2, 3\}.

For n=1n = 1: oscillates. For n=0n = 0: unbounded.


Vectors

Tripos 2005, Paper 1, Question 5C

Consider tetrahedron with vertices at O(0,0,0)O(0,0,0), A(1,0,0)A(1,0,0), B(0,1,0)B(0,1,0), C(0,0,1)C(0,0,1).

(a) Find the cosines of angles between faces.

(b) Find the areas of the four faces.

(c) Find the distance from OO to face ABCABC.

Solution outline:

(a) Normal to face OABOAB is in zz-direction. Normal to OBCOBC is in xx-direction. These are perpendicular. Angle between faces OABOAB and OACOAC: normals are (0,0,1)(0,0,1) and (0,1,0)(0,1,0), angle is 90°90°.

Face ABCABC has normal (1,1,1)(1,1,1) (from cross product). Angle with other faces uses dot product.

(b) Face OABOAB is right triangle with area 1/21/2. Similarly for OBCOBC, OACOAC. Face ABCABC has area 32\frac{\sqrt{3}}{2}.

(c) Equation of face ABCABC: r⋅(1,1,1)=1\mathbf{r} \cdot (1,1,1) = 1, or x+y+z=1x + y + z = 1.

Distance from OO: d=13d = \frac{1}{\sqrt{3}}.


Tripos 2004, Paper 1, Question 1A

Given vectors a\mathbf{a}, b\mathbf{b}, c\mathbf{c} with a⋅(b×c)≠0\mathbf{a} \cdot (\mathbf{b} \times \mathbf{c}) \neq 0, define reciprocal basis (a∗,b∗,c∗)(\mathbf{a}^*, \mathbf{b}^*, \mathbf{c}^*) by:

a∗=b×ca⋅(b×c)\mathbf{a}^* = \frac{\mathbf{b} \times \mathbf{c}}{\mathbf{a} \cdot (\mathbf{b} \times \mathbf{c})}

with analogous definitions for b∗\mathbf{b}^*, c∗\mathbf{c}^*.

Show that a∗⋅a=1\mathbf{a}^* \cdot \mathbf{a} = 1 and a∗⋅b=0\mathbf{a}^* \cdot \mathbf{b} = 0.

Solution:

a∗⋅a=a⋅(b×c)a⋅(b×c)=1\mathbf{a}^* \cdot \mathbf{a} = \frac{\mathbf{a} \cdot (\mathbf{b} \times \mathbf{c})}{\mathbf{a} \cdot (\mathbf{b} \times \mathbf{c})} = 1

a∗⋅b=(b×c)⋅ba⋅(b×c)\mathbf{a}^* \cdot \mathbf{b} = \frac{(\mathbf{b} \times \mathbf{c}) \cdot \mathbf{b}}{\mathbf{a} \cdot (\mathbf{b} \times \mathbf{c})}

But (b×c)⋅b=[b,c,b]=0(\mathbf{b} \times \mathbf{c}) \cdot \mathbf{b} = [\mathbf{b}, \mathbf{c}, \mathbf{b}] = 0 (repeated vector in scalar triple product).


Series

Tripos 2014, Paper 1

Find the expansion of ln⁡(1+x+x2)\ln(1 + x + x^2) for:

(i) small xx

(ii) large xx

Solution:

(i) 1+x+x2=1+x+x21 + x + x^2 = 1 + x + x^2. Let u=x+x2u = x + x^2, then for small uu:

ln⁡(1+u)=u−u22+u33−⋯\ln(1+u) = u - \frac{u^2}{2} + \frac{u^3}{3} - \cdots

Substitute back: ln⁡(1+x+x2)=x+x2−(x+x2)22+⋯\ln(1+x+x^2) = x + x^2 - \frac{(x+x^2)^2}{2} + \cdots

(ii) For large xx: ln⁡(1+x+x2)=ln⁡(x2)+ln⁡(1x2+1x+1)\ln(1+x+x^2) = \ln(x^2) + \ln\left(\frac{1}{x^2} + \frac{1}{x} + 1\right)

Let w=1x+1x2w = \frac{1}{x} + \frac{1}{x^2}. Then:

=2ln⁡x+w−w22+⋯= 2\ln x + w - \frac{w^2}{2} + \cdots