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Mathematics · Ch 2 — Complex Numbers

Polar Form of a Complex Number

2.7.1

Polar Form of a Complex Number

Polar coordinates form another set of parameters characterising the vector from the origin to a point z=x+iyz=x+iy, using magnitude and direction instead of horizontal/vertical components. The polar coordinate system has a fixed point OO (the pole) and a horizontal half-line from OO (the initial line or polar axis). For a point PP, if rr is the distance from OO to PP and θ\theta is the angle (measured counter-clockwise from the initial line) to the line OPOP, then (r,θ)(r,\theta) are the polar coordinates of PP.

Superimposing this on the ordinary rectangular system gives

x=rcos⁡θ...(1)y=rsin⁡θ...(2)x=r\cos\theta \qquad\text{...(1)} \qquad\qquad y=r\sin\theta \qquad\text{...(2)}

so any nonzero complex number z=x+iyz=x+iy can be expressed as z=rcos⁡θ+irsin⁡θz=r\cos\theta+ir\sin\theta.

Definition. Let r,θr,\theta be polar coordinates of the point P(x,y)P(x,y) corresponding to z=x+iy≠0z=x+iy\ne0. The polar (trigonometric) form of zz is

z=r(cos⁡θ+isin⁡θ),written for short as z=rcis⁡θ.z=r(\cos\theta+i\sin\theta),\qquad\text{written for short as } z=r\operatorname{cis}\theta.

Here rr is the modulus of zz (the absolute value, as before), and θ\theta is called the argument (or amplitude) of zz, written arg⁡z\arg z.

  • If z=0z=0, θ\theta is undefined — polar coordinates always assume z≠0z\ne0.
  • If z=x+iyz=x+iy has polar coordinates (r,θ)(r,\theta), its conjugate z‾=x−iy\overline z=x-iy has polar coordinates (r,−θ)(r,-\theta).

Squaring and adding (1) and (2) gives r=∣z∣=x2+y2r=|z|=\sqrt{x^2+y^2}; dividing (2) by (1) gives tan⁡θ=y/x\tan\theta=y/x.

General argument vs. principal argument. θ\theta can take infinitely many values, all differing by an integer multiple of 2π2\pi — every value of θ\theta satisfying tan⁡θ=y/x\tan\theta=y/x in the correct quadrant for zz is an argument of zz, and the full set of such values is denoted arg⁡z\arg z. There is a unique value of θ\theta satisfying −π<θ≤π-\pi<\theta\le\pi; this is called the principal argument, Arg⁡z\operatorname{Arg}z. In general, arg⁡z=Arg⁡z+2nπ, n∈Z\arg z=\operatorname{Arg}z+2n\pi,\ n\in\mathbb Z.

To find Arg⁡z\operatorname{Arg}z in practice: compute α=tan⁡−1∣yx∣\alpha=\tan^{-1}\left|\dfrac yx\right| (the reference angle, always taken as the acute angle from the calculator) and then adjust for the quadrant containing z=x+iyz=x+iy:

Quadrantsign of (x,y)(x,y)Arg⁡z\operatorname{Arg}z
I(+,+)(+,+)α\alpha
II(−,+)(-,+)π−α\pi-\alpha
III(−,−)(-,-)−(π−α)-(\pi-\alpha)
IV(+,−)(+,-)−α-\alpha

For instance, the principal argument and (general) argument of 1,i,−1,−i1,i,-1,-i are 0, π2, π (but arg⁡=2nπ+π using the branch just past −π too), −π20,\ \dfrac\pi2,\ \pi\ (\text{but}\ \arg=2n\pi+\pi\text{ using the branch just past }-\pi\text{ too}),\ -\dfrac\pi2 respectively, matching the point's position on the axes.

Properties of arguments (parallel to the modulus properties):

arg⁡(z1z2)=arg⁡z1+arg⁡z2,arg⁡ ⁣(z1z2)=arg⁡z1−arg⁡z2,arg⁡(zn)=narg⁡z,\arg(z_1z_2)=\arg z_1+\arg z_2,\qquad \arg\!\left(\frac{z_1}{z_2}\right)=\arg z_1-\arg z_2,\qquad \arg(z^n)=n\arg z,

and cos⁡θ+isin⁡θ\cos\theta+i\sin\theta has the equivalent alternate forms cos⁡(2kπ+θ)+isin⁡(2kπ+θ), k∈Z\cos(2k\pi+\theta)+i\sin(2k\pi+\theta),\ k\in\mathbb Z (adding any whole number of full turns changes nothing). …