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Further Pure Mathematics 2

Board Coverage

BoardPaperNotes
AQAPaper 2Groups, further complex, Maclaurin series, further DEs
EdexcelFP2Series, further complex, 1st/2nd order DEs, conics
OCR (A)Pure Core 2Groups, Maclaurin, polar area, vectors, conics
CIE (9709)Paper 3Complex, vectors, further calculus, conics

:::info This is advanced content in most cases appearing in the second year of Further Mathematics. Ensure full mastery of Further Pure 1 before proceeding.


1. Further Complex Numbers

1.1 Euler’s Relation

Euler’s relation connects the exponential and trigonometric functions:

eiθ=cosθ+isinθe^{i\theta} = \cos\theta + i\sin\theta

From which:

cosθ=eiθ+eiθ2sinθ=eiθeiθ2i\cos\theta = \frac{e^{i\theta} + e^{-i\theta}}{2} \qquad \sin\theta = \frac{e^{i\theta} - e^{-i\theta}}{2i}

Euler’s identity: eiπ+1=0e^{i\pi} + 1 = 0 (connects ee, ii, π\pi, 11, and 00).

1.2 Exponential Form

Any non-zero complex number can be written as:

z=reiθz = re^{i\theta}

where r=zr = |z| and θ=arg(z)\theta = \arg(z).

This form is particularly convenient for:

  • Raising to powers: zn=rneinθz^n = r^n e^{in\theta}
  • Taking roots: z1/n=r1/nei(θ+2kπ)/nz^{1/n} = r^{1/n} e^{i(\theta + 2k\pi)/n}
  • Multiplication and division (rules are the same as in modulus-argument form)

1.3 Solving Equations with Complex Numbers

Linear equations: straightforward algebraic manipulation.

Quadratic with complex coefficients: the quadratic formula still applies.

az2+bz+c=0    z=b±b24ac2aaz^2 + bz + c = 0 \implies z = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}

Even when a,b,ca, b, c are complex, the formula gives both roots.

Example. Solve z2=iz^2 = i. In exponential form: z=ei(π/2+2kπ)/2=eiπ/4z = e^{i(\pi/2 + 2k\pi)/2} = e^{i\pi/4} or ei5π/4e^{i5\pi/4}, so z=12(1+i)z = \frac{1}{\sqrt{2}}(1 + i) or 12(1i)\frac{1}{\sqrt{2}}(-1 - i).

1.4 Geometry in the Complex Plane

Rotation about a point z0z_0 by angle α\alpha: multiply by eiαe^{i\alpha} and add z0z_0.

wz0=eiα(zz0)w - z_0 = e^{i\alpha}(z - z_0)

Reflection in a line: express the line as arg(za)=θ\arg(z - a) = \theta and use the formula:

w=a+e2iθ(zˉaˉ)w = a + e^{2i\theta}(\bar{z} - \bar{a})

Distance between two points: z1z2|z_1 - z_2|.


2. Groups

2.1 Axioms

A group (G,)(G, *) is a set GG with a binary operation * satisfying:

  1. Closure: for all a,bGa, b \in G, abGa * b \in G
  2. Associativity: for all a,b,cGa, b, c \in G, (ab)c=a(bc)(a * b) * c = a * (b * c)
  3. Identity: there exists eGe \in G such that ae=ea=aa * e = e * a = a for all aa
  4. Inverse: for each aGa \in G, there exists a1Ga^{-1} \in G such that aa1=a1a=ea * a^{-1} = a^{-1} * a = e

An abelian group also satisfies commutativity: ab=baa * b = b * a for all a,ba, b.

2.2 Subgroups

(H,)(H, *) is a subgroup of (G,)(G, *) if HGH \subseteq G and (H,)(H, *) is itself a group.

Subgroup test: HH is a subgroup of GG if and only if for all a,bHa, b \in H: ab1Ha * b^{-1} \in H.

Lagrange’s theorem: For a finite group, the order of any subgroup divides the order of the group. H|H| divides G|G|.

2.3 Cyclic Groups

A group is cyclic if every element is a power of a single element (the generator).

If G=gG = \langle g \rangle, then G={e,g,g2,g3,}G = \{e, g, g^2, g^3, \ldots\}.

Example. (Z6,+)(\mathbb{Z}_6, +) is cyclic: 1={0,1,2,3,4,5}\langle 1 \rangle = \{0, 1, 2, 3, 4, 5\}.

Subgroups of a cyclic group: If G=gG = \langle g \rangle with G=n|G| = n, then for each divisor dd of nn, there is exactly one subgroup of order dd, generated by gn/dg^{n/d}.

2.4 Isomorphism

An isomorphism ϕ:GH\phi: G \to H is a bijection that preserves the group operation:

ϕ(ab)=ϕ(a)ϕ(b)\phi(a * b) = \phi(a) \circ \phi(b)

If an isomorphism exists between GG and HH, they are isomorphic (GHG \cong H) and have the same group structure (same Cayley table up to relabelling).

Isomorphic groups share: order, number of elements of each order, abelian or non-abelian, subgroup structure, number of subgroups of each order.

2.5 Group Homomorphisms

A homomorphism ϕ:GH\phi: G \to H is a function preserving the operation (but not necessarily bijective):

ϕ(ab)=ϕ(a)ϕ(b)\phi(a * b) = \phi(a) \circ \phi(b)

Kernel: ker(ϕ)={gG:ϕ(g)=eH}\ker(\phi) = \{g \in G : \phi(g) = e_H\}. The kernel is always a subgroup of GG.

Image: im(ϕ)={ϕ(g):gG}\text{im}(\phi) = \{\phi(g) : g \in G\}. The image is always a subgroup of HH.


3. Further Calculus

3.1 Maclaurin Series

The Maclaurin series of f(x)f(x) is its Taylor expansion about x=0x = 0:

f(x)=f(0)+f(0)x+f(0)2!x2+f(0)3!x3+=n=0f(n)(0)n!xnf(x) = f(0) + f'(0)x + \frac{f''(0)}{2!}x^2 + \frac{f'''(0)}{3!}x^3 + \cdots = \sum_{n=0}^{\infty} \frac{f^{(n)}(0)}{n!}x^n

Standard Maclaurin series:

ex=1+x+x22!+x33!+e^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \cdots

ln(1+x)=xx22+x33x44+for x<1\ln(1 + x) = x - \frac{x^2}{2} + \frac{x^3}{3} - \frac{x^4}{4} + \cdots \quad \text{for } |x| < 1

sinx=xx33!+x55!\sin x = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \cdots

cosx=1x22!+x44!\cos x = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \cdots

(1+x)n=1+nx+n(n1)2!x2+(general binomial)(1 + x)^n = 1 + nx + \frac{n(n-1)}{2!}x^2 + \cdots \quad \text{(general binomial)}

3.2 Taylor Series

Expanding about a general point x=ax = a:

f(x)=f(a)+f(a)(xa)+f(a)2!(xa)2+f(x) = f(a) + f'(a)(x-a) + \frac{f''(a)}{2!}(x-a)^2 + \cdots

Useful technique: let u=xau = x - a, then expand in powers of uu.

3.3 Differential Equations: Series Solutions

For equations that cannot be solved by standard methods, assume a power series solution:

y=n=0anxny = \sum_{n=0}^{\infty} a_n x^n

Substitute into the differential equation, equate coefficients of each power of xx, and solve the resulting recurrence relation for ana_n.

Example. For y=yy' = y with y(0)=1y(0) = 1: substituting y=a0+a1x+a2x2+y = a_0 + a_1 x + a_2 x^2 + \cdots gives a1=a0a_1 = a_0, 2a2=a12a_2 = a_1, 3a3=a23a_3 = a_2, and so an=a0/n!a_n = a_0/n!, yielding y=xn/n!=exy = \sum x^n/n! = e^x.

3.4 Reduction Formulae

A reduction formula expresses an integral InI_n (depending on nn) in terms of In1I_{n-1} or In2I_{n-2}.

Method: Use integration by parts, choosing uu and dvdv so that the resulting integral involves n1n - 1 or n2n - 2.

Example. For In=0π/2sinnxdxI_n = \int_0^{\pi/2} \sin^n x\,dx:

In=n1nIn2I_n = \frac{n-1}{n}I_{n-2}

with I0=π/2I_0 = \pi/2 and I1=1I_1 = 1.

Another common example: In=xneaxdxI_n = \int x^n e^{ax}\,dx:

In=1axneaxnaIn1I_n = \frac{1}{a}x^n e^{ax} - \frac{n}{a}I_{n-1}


4. Vectors and 3D Geometry

4.1 Scalar Product

The scalar (dot) product of vectors a\mathbf{a} and b\mathbf{b}:

ab=abcosθ=a1b1+a2b2+a3b3\mathbf{a} \cdot \mathbf{b} = |\mathbf{a}|\,|\mathbf{b}|\cos\theta = a_1 b_1 + a_2 b_2 + a_3 b_3

where θ\theta is the angle between them.

Perpendicular vectors: ab=0\mathbf{a} \cdot \mathbf{b} = 0.

Angle between vectors: cosθ=abab\cos\theta = \dfrac{\mathbf{a} \cdot \mathbf{b}}{|\mathbf{a}|\,|\mathbf{b}|}.

4.2 Vector Product

The vector (cross) product in 3D:

a×b=ijka1a2a3b1b2b3\mathbf{a} \times \mathbf{b} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \end{vmatrix}

a×b=absinθ|\mathbf{a} \times \mathbf{b}| = |\mathbf{a}|\,|\mathbf{b}|\sin\theta

Properties:

  • a×b\mathbf{a} \times \mathbf{b} is perpendicular to both a\mathbf{a} and b\mathbf{b}
  • a×b=b×a\mathbf{a} \times \mathbf{b} = -\mathbf{b} \times \mathbf{a} (anti-commutative)
  • a×a=0\mathbf{a} \times \mathbf{a} = \mathbf{0}
  • a×b\mathbf{a} \times \mathbf{b} gives the area of the parallelogram formed by a\mathbf{a} and b\mathbf{b}
  • a(b×c)|\mathbf{a} \cdot (\mathbf{b} \times \mathbf{c})| = volume of the parallelepiped

4.3 Lines in 3D

Parametric form through point a\mathbf{a} with direction d\mathbf{d}:

r=a+td(tR)\mathbf{r} = \mathbf{a} + t\mathbf{d} \qquad (t \in \mathbb{R})

Cartesian (symmetric) form:

xa1d1=ya2d2=za3d3=t\frac{x - a_1}{d_1} = \frac{y - a_2}{d_2} = \frac{z - a_3}{d_3} = t

Two lines are parallel if their direction vectors are proportional.

Two lines intersect if there exists a parameter value t1=t2t_1 = t_2 satisfying all three component equations simultaneously.

Angle between two lines: cosθ=d1d2d1d2\cos\theta = \dfrac{|\mathbf{d}_1 \cdot \mathbf{d}_2|}{|\mathbf{d}_1|\,|\mathbf{d}_2|}.

4.4 Planes

Equation of a plane: rn=an\mathbf{r} \cdot \mathbf{n} = \mathbf{a} \cdot \mathbf{n}, or in Cartesian form:

n1x+n2y+n3z=dn_1 x + n_2 y + n_3 z = d

where n=(n1,n2,n3)\mathbf{n} = (n_1, n_2, n_3) is the normal vector and d=and = \mathbf{a} \cdot \mathbf{n} for a known point a\mathbf{a} on the plane.

Plane through three points: Find two direction vectors from the points, take their cross product for the normal, then substitute.

Angle between two planes: angle between their normal vectors.

Line of intersection: find two points satisfying both plane equations, then write the parametric line through them.

4.5 Shortest Distance

Point to line: d=(ap)×ddd = \dfrac{|(\mathbf{a} - \mathbf{p}) \times \mathbf{d}|}{|\mathbf{d}|}

where p\mathbf{p} is a point on the line with direction d\mathbf{d}, and a\mathbf{a} is the external point.

Point to plane: d=nadnd = \dfrac{|\mathbf{n} \cdot \mathbf{a} - d|}{|\mathbf{n}|}

where a\mathbf{a} is the point and the plane is rn=d\mathbf{r} \cdot \mathbf{n} = d.

Skew lines (shortest distance between):

d=(a2a1)(d1×d2)d1×d2d = \frac{|(\mathbf{a}_2 - \mathbf{a}_1) \cdot (\mathbf{d}_1 \times \mathbf{d}_2)|}{|\mathbf{d}_1 \times \mathbf{d}_2|}

where a1,a2\mathbf{a}_1, \mathbf{a}_2 are points on the respective lines and d1,d2\mathbf{d}_1, \mathbf{d}_2 are direction vectors.


5. Conics

5.1 Focus-Directrix Properties

A conic section is the locus of points PP such that:

distance from P to focus Fdistance from P to directrix=e(eccentricity)\frac{\text{distance from } P \text{ to focus } F}{\text{distance from } P \text{ to directrix}} = e \quad (\text{eccentricity})

ConicEccentricity
Circlee=0e = 0
Ellipse0<e<10 < e < 1
Parabolae=1e = 1
Hyperbolae>1e > 1

5.2 Parametric Equations

Ellipse x2a2+y2b2=1\dfrac{x^2}{a^2} + \dfrac{y^2}{b^2} = 1 (a>ba > b):

x=acosθ,y=bsinθx = a\cos\theta, \quad y = b\sin\theta

Focus: (±ae,0)(\pm ae, 0) where e=1b2/a2e = \sqrt{1 - b^2/a^2}.

Hyperbola x2a2y2b2=1\dfrac{x^2}{a^2} - \dfrac{y^2}{b^2} = 1:

x=asecθ,y=btanθx = a\sec\theta, \quad y = b\tan\theta

Focus: (±ae,0)(\pm ae, 0) where e=1+b2/a2e = \sqrt{1 + b^2/a^2}. Asymptotes: y=±baxy = \pm \dfrac{b}{a}x.

Parabola y2=4axy^2 = 4ax:

x=at2,y=2atx = at^2, \quad y = 2at

Focus: (a,0)(a, 0). Directrix: x=ax = -a.

5.3 Cartesian Equations

Rectangular hyperbola: xy=c2xy = c^2. Parametric form: x=ctx = ct, y=c/ty = c/t. Asymptotes are the coordinate axes. Eccentricity e=2e = \sqrt{2}.

Tangent to a parabola y2=4axy^2 = 4ax at (at2,2at)(at^2, 2at):

ty=x+at2ty = x + at^2

Normal to a parabola y2=4axy^2 = 4ax at (at2,2at)(at^2, 2at):

y=tx+2at+at3y = -tx + 2at + at^3

Tangent to ellipse x2a2+y2b2=1\dfrac{x^2}{a^2} + \dfrac{y^2}{b^2} = 1 at (acosθ,bsinθ)(a\cos\theta, b\sin\theta):

xcosθa+ysinθb=1\frac{x\cos\theta}{a} + \frac{y\sin\theta}{b} = 1


6. Common Mistakes

  1. Incorrect branch of cosh1\cosh^{-1}. cosh1x\cosh^{-1} x is defined only for x1x \geq 1 and returns non-negative values. Do not forget the domain restriction.
  2. Wrong sign in the hyperbolic identity. It is cosh2xsinh2x=1\cosh^2 x - \sinh^2 x = 1 (minus, not plus). A sign error here propagates through to derivatives and integrals.
  3. Forgetting closure or identity when checking group axioms. All four axioms (closure, associativity, identity, inverses) must be verified; omission of any one is a common error.
  4. Confusing scalar and vector products. ab\mathbf{a} \cdot \mathbf{b} is a scalar; a×b\mathbf{a} \times \mathbf{b} is a vector. Know which to use: scalar for angles and projections, vector for areas and perpendicular directions.
  5. Incorrect shortest distance formula. The formula for point-to-line distance uses the cross product (3D); the formula for point-to-plane distance uses the dot product with the normal. Do not mix them up.
  6. Wrong parametric form for hyperbola. For x2a2y2b2=1\frac{x^2}{a^2} - \frac{y^2}{b^2} = 1, use x=asecθx = a\sec\theta, y=btanθy = b\tan\theta. Do not use cosh\cosh and sinh\sinh unless the question specifies the rectangular hyperbola xy=c2xy = c^2.
  7. Series solution recurrence with wrong initial terms. When equating coefficients in series solutions, carefully determine a0a_0 and a1a_1 from initial conditions before deriving the recurrence for ana_n.

Worked Examples

Example 1: Finding a Reduction Formula

Problem: Find a reduction formula for In=0π/2cosnxdxI_n = \int_0^{\pi/2} \cos^n x\,dx where n0n \geq 0. Solution: Use integration by parts with u=cosn1xu = \cos^{n-1}x and dv=cosxdxdv = \cos x\,dx: u=cosn1x    du=(n1)cosn2xsinxdx,v=sinxu = \cos^{n-1}x \implies du = -(n-1)\cos^{n-2}x\sin x\,dx, \quad v = \sin x In=[cosn1xsinx]0π/2+(n1)0π/2cosn2xsin2xdxI_n = \left[\cos^{n-1}x\sin x\right]_0^{\pi/2} + (n-1)\int_0^{\pi/2}\cos^{n-2}x\sin^2 x\,dx The boundary term vanishes. Replace sin2x=1cos2x\sin^2 x = 1 - \cos^2 x: In=(n1)0π/2cosn2xdx(n1)0π/2cosnxdx=(n1)In2(n1)InI_n = (n-1)\int_0^{\pi/2}\cos^{n-2}x\,dx - (n-1)\int_0^{\pi/2}\cos^n x\,dx = (n-1)I_{n-2} - (n-1)I_n nIn=(n1)In2    In=n1nIn2nI_n = (n-1)I_{n-2} \implies I_n = \frac{n-1}{n}I_{n-2} With I0=π/2I_0 = \pi/2 and I1=1I_1 = 1.

Example 2: Proving a Group Isomorphism

Problem: Show that the group ({1,1,i,i},×)(\{1, -1, i, -i\}, \times) is isomorphic to the cyclic group (Z4,+)(\mathbb{Z}_4, +). Solution: Define ϕ:Z4{1,1,i,i}\phi: \mathbb{Z}_4 \to \{1, -1, i, -i\} by ϕ(k)=ik\phi(k) = i^k. Check: ϕ\phi is bijective and ϕ(a+b)=ia+b=iaib=ϕ(a)ϕ(b)\phi(a + b) = i^{a+b} = i^a \cdot i^b = \phi(a)\phi(b). The multiplication table of {1,1,i,i}\{1, -1, i, -i\} matches the addition table of Z4\mathbb{Z}_4 under this mapping, confirming the isomorphism.

Common Pitfalls

  • Omitting axioms when checking groups: All four axioms (closure, associativity, identity, inverses) must be verified. Associativity is often assumed but should be checked or stated.
  • Wrong reduction formula boundary terms: Always evaluate [uv][uv] at the limits. If the boundary term is non-zero, it must be included in the formula.
  • Confusing cosh1\cosh^{-1} domain: cosh1x\cosh^{-1} x is defined only for x1x \geq 1. Applying it to values outside this domain produces an error.

Summary

Further Pure 2 extends FP1 material through further complex numbers (Euler’s relation, geometry in the complex plane), group theory (axioms, subgroups, cyclic groups, isomorphism, homomorphisms), further calculus (Maclaurin and Taylor series, series solutions, reduction formulae), vectors in 3D (scalar and vector products, lines, planes, shortest distances), and conics (focus-directrix properties, parametric and Cartesian equations, tangents and normals).

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