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 x x x and constant a a a :
(i) lim x → 0 tan x sin x sin 3 x \displaystyle\lim_{x \to 0} \frac{\tan x \sin x}{\sin^3 x} x → 0 lim sin 3 x tan x sin x
(ii) lim x → a sin x − sin a x − a \displaystyle\lim_{x \to a} \frac{\sin x - \sin a}{x - a} x → a lim x − a sin x − sin a
(iii) lim x → ∞ ( x + a x − a ) x + a \displaystyle\lim_{x \to \infty} \left(\frac{x + a}{x - a}\right)^{x+a} x → ∞ lim ( x − a x + a ) x + a
Solutions:
(i) Using tan x = sin x cos x \tan x = \frac{\sin x}{\cos x} tan x = c o s x s i n x :
lim x → 0 sin 2 x cos x sin 3 x = lim x → 0 1 cos x sin x \lim_{x \to 0} \frac{\sin^2 x}{\cos x \sin^3 x} = \lim_{x \to 0} \frac{1}{\cos x \sin x} lim x → 0 c o s x s i n 3 x s i n 2 x = lim x → 0 c o s x s i n x 1
This doesn’t exist (goes to ∞ \infty ∞ ). Actually, let’s reconsider:
tan x sin x sin 3 x = 1 cos x sin 2 x \frac{\tan x \sin x}{\sin^3 x} = \frac{1}{\cos x \sin^2 x} s i n 3 x t a n x s i n x = c o s x s i n 2 x 1
Using sin x ∼ x \sin x \sim x sin x ∼ x near 0: this behaves like 1 x 2 \frac{1}{x^2} x 2 1 , so the limit is ∞ \infty ∞ .
(ii) This is the derivative of sin x \sin x sin x at x = a x = a x = a :
lim x → a sin x − sin a x − a = cos a \lim_{x \to a} \frac{\sin x - \sin a}{x - a} = \cos a lim x → a x − a s i n x − s i n a = cos a
Alternatively, use the identity sin x − sin a = 2 cos x + a 2 sin x − a 2 \sin x - \sin a = 2\cos\frac{x+a}{2}\sin\frac{x-a}{2} sin x − sin a = 2 cos 2 x + a sin 2 x − a .
(iii) Let y = ( x + a x − a ) x + a y = \left(\frac{x+a}{x-a}\right)^{x+a} y = ( x − a x + a ) x + a . Then:
ln y = ( x + a ) ln ( 1 + 2 a x − a ) \ln y = (x+a)\ln\left(1 + \frac{2a}{x-a}\right) ln y = ( x + a ) ln ( 1 + x − a 2 a )
For large x x x : ln ( 1 + 2 a x − a ) ∼ 2 a x − a \ln\left(1 + \frac{2a}{x-a}\right) \sim \frac{2a}{x-a} ln ( 1 + x − a 2 a ) ∼ x − a 2 a
So ln y ∼ ( x + a ) ⋅ 2 a x − a → 2 a \ln y \sim (x+a) \cdot \frac{2a}{x-a} \to 2a ln y ∼ ( x + a ) ⋅ x − a 2 a → 2 a as x → ∞ x \to \infty x → ∞ .
Therefore: y → e 2 a y \to e^{2a} y → e 2 a
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\} n ∈ { 0 , 1 , 2 , 3 , 4 } :
ϕ ( x , n ) = { x n sin ( 1 / x ) x ≠ 0 0 x = 0 , n ≠ 4 1 x = 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} ϕ ( x , n ) = ⎩ ⎨ ⎧ x n sin ( 1/ x ) 0 1 x = 0 x = 0 , n = 4 x = 0 , n = 4
(i) Determine values of n n n for which ϕ ( x , n ) \phi(x,n) ϕ ( x , n ) tends to a limit as x → 0 x \to 0 x → 0 .
(ii) Determine values of n n n for which ϕ ( x , n ) \phi(x,n) ϕ ( x , n ) is continuous at x = 0 x = 0 x = 0 .
(iii) Determine values of n n n for which ϕ ( x , n ) \phi(x,n) ϕ ( x , n ) is differentiable at x = 0 x = 0 x = 0 .
Solutions:
(i) Limit exists if n > 0 n > 0 n > 0 . For n = 0 n = 0 n = 0 : sin ( 1 / x ) \sin(1/x) sin ( 1/ x ) oscillates. For n ≥ 1 n \geq 1 n ≥ 1 : ∣ x n sin ( 1 / x ) ∣ ≤ ∣ x ∣ n → 0 |x^n \sin(1/x)| \leq |x|^n \to 0 ∣ x n sin ( 1/ x ) ∣ ≤ ∣ x ∣ n → 0 .
(ii) For continuity, need lim x → 0 ϕ = ϕ ( 0 ) \lim_{x \to 0} \phi = \phi(0) lim x → 0 ϕ = ϕ ( 0 ) . The limit is 0 for n ≥ 1 n \geq 1 n ≥ 1 , so we need ϕ ( 0 ) = 0 \phi(0) = 0 ϕ ( 0 ) = 0 . This holds for n ∈ { 1 , 2 , 3 } n \in \{1, 2, 3\} n ∈ { 1 , 2 , 3 } .
(iii) For differentiability:
ϕ ′ ( 0 ) = lim h → 0 ϕ ( h ) − ϕ ( 0 ) h = lim h → 0 h n sin ( 1 / h ) h = lim h → 0 h n − 1 sin ( 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) ϕ ′ ( 0 ) = lim h → 0 h ϕ ( h ) − ϕ ( 0 ) = lim h → 0 h h n s i n ( 1/ h ) = lim h → 0 h n − 1 sin ( 1/ h )
This exists (equals 0) if n − 1 > 0 n - 1 > 0 n − 1 > 0 , i.e., n ∈ { 2 , 3 } n \in \{2, 3\} n ∈ { 2 , 3 } .
For n = 1 n = 1 n = 1 : oscillates. For n = 0 n = 0 n = 0 : unbounded.
Vectors
Tripos 2005, Paper 1, Question 5C
Consider tetrahedron with vertices at O ( 0 , 0 , 0 ) O(0,0,0) O ( 0 , 0 , 0 ) , A ( 1 , 0 , 0 ) A(1,0,0) A ( 1 , 0 , 0 ) , B ( 0 , 1 , 0 ) B(0,1,0) B ( 0 , 1 , 0 ) , C ( 0 , 0 , 1 ) 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 O O O to face A B C ABC A B C .
Solution outline:
(a) Normal to face O A B OAB O A B is in z z z -direction. Normal to O B C OBC O B C is in x x x -direction. These are perpendicular. Angle between faces O A B OAB O A B and O A C OAC O A C : normals are ( 0 , 0 , 1 ) (0,0,1) ( 0 , 0 , 1 ) and ( 0 , 1 , 0 ) (0,1,0) ( 0 , 1 , 0 ) , angle is 90 ° 90° 90° .
Face A B C ABC A B C has normal ( 1 , 1 , 1 ) (1,1,1) ( 1 , 1 , 1 ) (from cross product). Angle with other faces uses dot product.
(b) Face O A B OAB O A B is right triangle with area 1 / 2 1/2 1/2 . Similarly for O B C OBC O B C , O A C OAC O A C . Face A B C ABC A B C has area 3 2 \frac{\sqrt{3}}{2} 2 3 .
(c) Equation of face A B C ABC A B C : r ⋅ ( 1 , 1 , 1 ) = 1 \mathbf{r} \cdot (1,1,1) = 1 r ⋅ ( 1 , 1 , 1 ) = 1 , or x + y + z = 1 x + y + z = 1 x + y + z = 1 .
Distance from O O O : d = 1 3 d = \frac{1}{\sqrt{3}} d = 3 1 .
Tripos 2004, Paper 1, Question 1A
Given vectors a \mathbf{a} a , b \mathbf{b} b , c \mathbf{c} c with a ⋅ ( b × c ) ≠ 0 \mathbf{a} \cdot (\mathbf{b} \times \mathbf{c}) \neq 0 a ⋅ ( b × c ) = 0 , define reciprocal basis ( a ∗ , b ∗ , c ∗ ) (\mathbf{a}^*, \mathbf{b}^*, \mathbf{c}^*) ( a ∗ , b ∗ , c ∗ ) by:
a ∗ = b × c a ⋅ ( b × c ) \mathbf{a}^* = \frac{\mathbf{b} \times \mathbf{c}}{\mathbf{a} \cdot (\mathbf{b} \times \mathbf{c})} a ∗ = a ⋅ ( b × c ) b × c
with analogous definitions for b ∗ \mathbf{b}^* b ∗ , c ∗ \mathbf{c}^* c ∗ .
Show that a ∗ ⋅ a = 1 \mathbf{a}^* \cdot \mathbf{a} = 1 a ∗ ⋅ a = 1 and a ∗ ⋅ b = 0 \mathbf{a}^* \cdot \mathbf{b} = 0 a ∗ ⋅ 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 ∗ ⋅ a = a ⋅ ( b × c ) a ⋅ ( b × c ) = 1
a ∗ ⋅ b = ( b × c ) ⋅ b a ⋅ ( b × c ) \mathbf{a}^* \cdot \mathbf{b} = \frac{(\mathbf{b} \times \mathbf{c}) \cdot \mathbf{b}}{\mathbf{a} \cdot (\mathbf{b} \times \mathbf{c})} a ∗ ⋅ b = a ⋅ ( b × c ) ( b × c ) ⋅ b
But ( b × c ) ⋅ b = [ b , c , b ] = 0 (\mathbf{b} \times \mathbf{c}) \cdot \mathbf{b} = [\mathbf{b}, \mathbf{c}, \mathbf{b}] = 0 ( b × c ) ⋅ b = [ b , c , b ] = 0 (repeated vector in scalar triple product).
Series
Tripos 2014, Paper 1
Find the expansion of ln ( 1 + x + x 2 ) \ln(1 + x + x^2) ln ( 1 + x + x 2 ) for:
(i) small x x x
(ii) large x x x
Solution:
(i) 1 + x + x 2 = 1 + x + x 2 1 + x + x^2 = 1 + x + x^2 1 + x + x 2 = 1 + x + x 2 . Let u = x + x 2 u = x + x^2 u = x + x 2 , then for small u u u :
ln ( 1 + u ) = u − u 2 2 + u 3 3 − ⋯ \ln(1+u) = u - \frac{u^2}{2} + \frac{u^3}{3} - \cdots ln ( 1 + u ) = u − 2 u 2 + 3 u 3 − ⋯
Substitute back: ln ( 1 + x + x 2 ) = x + x 2 − ( x + x 2 ) 2 2 + ⋯ \ln(1+x+x^2) = x + x^2 - \frac{(x+x^2)^2}{2} + \cdots ln ( 1 + x + x 2 ) = x + x 2 − 2 ( x + x 2 ) 2 + ⋯
(ii) For large x x x : ln ( 1 + x + x 2 ) = ln ( x 2 ) + ln ( 1 x 2 + 1 x + 1 ) \ln(1+x+x^2) = \ln(x^2) + \ln\left(\frac{1}{x^2} + \frac{1}{x} + 1\right) ln ( 1 + x + x 2 ) = ln ( x 2 ) + ln ( x 2 1 + x 1 + 1 )
Let w = 1 x + 1 x 2 w = \frac{1}{x} + \frac{1}{x^2} w = x 1 + x 2 1 . Then:
= 2 ln x + w − w 2 2 + ⋯ = 2\ln x + w - \frac{w^2}{2} + \cdots = 2 ln x + w − 2 w 2 + ⋯