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Complex numbers and complex exponentials

Calculate with complex numbers, interpret their plane and unit-circle representation, and use Euler's formula to encode a supplied scalar displacement model without inventing an extra physical direction.

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After reading, you can

  • Identify the real and imaginary coefficients of a complex number.
  • Add, subtract, multiply and divide complex numbers with the stated restrictions.
  • Calculate a conjugate and a nonnegative modulus.
  • Introduce general oriented angles and their numerical radian values before using sine and cosine.
  • Use Euler's formula at exact cardinal phases and state its mathematical scope.
  • Recover a stated scalar physical quantity from a chosen complex representation.
01

Introduce the imaginary unit

The square of a real number is nonnegative, so no real number solves x² = −1. Complex numbers extend real-number arithmetic. Introduce the imaginary unit i by i² = −1, and write a complex number as z = a + ib, where a and b are real numbers. The symbol i is a number, not a unit such as metre.

The real part is Re z = a; the imaginary part is Im z = b. Both parts are real coefficients. For z = −4 + 7i, Re z = −4 and Im z = 7, rather than 7i. A real number a is also a complex number a + 0i. The term imaginary does not assign a physical direction to its coefficient.

A square means multiplication by itself. From i² = −1, i³ = i² i = −i and i⁴ = i² i² = 1. This locally supplies the rule needed in later products. Our bare-number arithmetic cases are exact mathematical choices with no physical unit or measurement claim.

02

Locate and combine complex numbers

Represent z = a + ib by the ordered pair (a, b) in the complex plane. The horizontal real axis gives a and the perpendicular imaginary axis gives b. Thus −4 + 7i is represented by (−4, 7). Use matching coordinate scales when interpreting distances and angles in this number plane.

Add or subtract corresponding coefficients: (a + ib) + (c + id) = (a + c) + i(b + d) and (a + ib) − (c + id) = (a − c) + i(b − d). For our choices z1 = 2 + 3i and z2 = 1 − 2i, their sum is 3 + i and their difference z1 − z2 is 1 + 5i.

Equal complex numbers have equal real coefficients and equal imaginary coefficients. The coordinate picture organizes this arithmetic. Its two axes alone do not establish two physical spatial directions; that would require a separately declared physical interpretation.

03

Multiply with the rule for i

Use distribution, multiplying each term in the first factor by each term in the second. Then replace i² by −1 and collect coefficients. This gives (a + ib)(c + id) = (ac − bd) + i(ad + bc). The negative bd term is essential.

For the same chosen pair, (2 + 3i)(1 − 2i) = 2 − 4i + 3i − 6i² = 8 − i. Treating i² as +1 would give an incorrect real part. The product generally differs from multiplying real parts and imaginary parts separately.

Multiplication by i sends a + ib to −b + ia, so its complex-plane coordinates become (−b, a). For instance, i(2 + 3i) = −3 + 2i. In an equally scaled complex-plane drawing this is a counterclockwise quarter-turn about the origin. This statement concerns the number representation, not a claim that an object turned.

04

Conjugate, measure and divide

The conjugate of z = a + ib is z* = a − ib; the star denotes conjugation here. Its imaginary coefficient changes sign, reflecting the represented point across the real axis. The modulus is |z| = √(a² + b²), the nonnegative distance from the origin in the equally scaled complex plane. The square-root symbol selects the nonnegative root. In particular, |0| = 0.

Multiplying a number by its conjugate gives z z* = (a + ib)(a − ib) = a² + b² = |z|². For our original choice z = −8 + 15i, z* = −8 − 15i and |z| = √(64 + 225) = 17. The modulus 17 is a magnitude; Re z = −8 is a signed coefficient. These answer different questions.

To divide by a nonzero complex number, multiply numerator and denominator by the denominator's conjugate. If the denominator is c + id, its resulting denominator is c² + d², which is positive whenever c and d are not both zero. This also works for a nonzero purely real or purely imaginary denominator. Division by zero remains undefined.

05

Introduce general unit-circle angles

Acute right-triangle ratios alone do not define the cardinal phases we need. Use an oriented angle from the positive real axis, with counterclockwise positive and clockwise negative. If the supplied angle is θ = φ rad, φ is its numerical radian value. The radian is an angle unit; angle remains a different quantity kind from an ordinary length ratio. A full turn is 2π rad, equivalent to 360°.

In a dimensionless coordinate plane, the unit circle has centre (0, 0) and radius 1. For any real numerical radian value φ, the point specified by the oriented angle has coordinates (cos φ, sin φ). This defines cosine and sine for negative angles and angles beyond an acute triangle or a full turn. Each coordinate lies between −1 and +1, and cos² φ + sin² φ = 1.

Here cos φ means cosine of the angle whose radian value is φ; sin φ has the corresponding meaning. The inputs φ and the outputs are dimensionless numbers in these formulas. A quarter-turn angle (π/2) rad therefore uses φ = π/2, rather than φ = 90. Adding 2π to φ leaves the unit-circle point unchanged. This is a mathematical angle convention, not a specified time evolution.

Exact unit-circle coordinates at selected supplied angles; φ is the numerical radian value in θ = φ rad
Angle θNumerical value φcos φsin φ
0 rad010
(π/2) radπ/201
π radπ−10
(3π/2) rad3π/20−1
2π rad2π10
06

Use Euler's formula with its scope

In exponent notation, the base is the number being raised and the exponent is the superscript. For a positive integer n, eⁿ is a product of n factors e; e⁰ = 1. The real exponential also extends to real exponents. Its standard base e is approximately 2.718282. A complex exponent requires a mathematical extension beyond the repeated-multiplication picture.

For every real φ, Euler's established mathematical relation is e^(iφ) = cos φ + i sin φ, with φ the dimensionless numerical radian value just introduced. This lesson uses the complex exponential at purely imaginary exponents iφ. The relation is compatible with the usual exponential extension; it is not a guessed physical law or something proved by plotting a few points. Its mathematical proof is outside the prerequisites of this lesson.

The table gives e^0 = 1, e^(iπ/2) = i, e^(iπ) = −1, e^(i3π/2) = −i and e^(i2π) = 1. Setting φ = π gives Euler's identity e^(iπ) + 1 = 0. The modulus is always |e^(iφ)| = √(cos² φ + sin² φ) = 1. These are exact identities; the circle illustrates their representation without proving the exponential relation.

07

Recover a stated physical quantity

Cosine displacement and a positive amplitude appear in elementary models of oscillation. Our original hypothetical case supplies only the scalar relation q(φ) = A cos φ, with A = 0.025 m and any supplied real φ. The displacement q is measured from a fixed reference position along one line, with right positive. The positive amplitude A is the maximum value of |q|. These stipulated values are not measurements.

Define an auxiliary complex representation W(φ) = A e^(iφ) = A cos φ + i A sin φ. Recover the model's physical scalar using q = Re W. Both Re W and Im W have metre units, and W/A = e^(iφ) is dimensionless because the positive reference amplitude has matching length units. Here Im W is a second coefficient used in the representation; it does not describe a second physical displacement axis.

For θ = (π/2) rad, φ = π/2, W = 0 + i(0.025 m) and q = 0 m, although |W| = A = 0.025 m. At θ = π rad, q = −0.025 m. The auxiliary circle therefore has fixed modulus while the scalar's absolute value can vary. No relation between φ and time, frequency or force is supplied. The representation cannot by itself specify an object's trajectory, speed or physical cause.

Exact original stipulated displacement representations; φ is the numerical radian value, A = 0.025 m and q = Re W
Supplied φAuxiliary WScalar q (m)
0+0.025 m + i(0 m)+0.025
π/20 m + i(+0.025 m)0
π−0.025 m + i(0 m)−0.025
3π/20 m + i(−0.025 m)0
2π+0.025 m + i(0 m)+0.025

An auxiliary circle for one scalar displacement

An auxiliary circle for one scalar displacementAn auxiliary complex plane with perpendicular real and imaginary coefficient axes, both in metres and drawn with equal scales. A circle centred at zero has radius 0.025 m. Its selected exact points are (Re W, Im W) = (+0.025 m, 0 m) for φ = 0 or 2π; (0 m, +0.025 m) for φ = π/2; (−0.025 m, 0 m) for φ = π; and (0 m, −0.025 m) for φ = 3π/2. Read the horizontal coefficient as the declared physical scalar q. At the top and bottom, q is zero while |W| remains 0.025 m. The vertical coefficient is auxiliary bookkeeping here, not another physical displacement axis. The circle illustrates the stipulated representation and Euler relation; it neither proves that relation nor assigns times, speeds or an object's circular motion.
  • φ = 0 or 2π; q = +0.025 m
  • φ = π/2; q = 0 m
  • φ = π; q = −0.025 m
  • φ = 3π/2; q = 0 m
  • Zero coefficients
  • |W| = A = 0.025 m
  1. 1. Supply the angle convention

    Write θ = φ rad and use the numerical value φ in e^(iφ). Positive φ is counterclockwise from the positive real axis. A full turn adds 2π and returns to the same representation.

  2. 2. Recover the named scalar

    In this declared model, q = Re W. At φ = π/2, W = i(0.025 m), so q = 0 m even though the auxiliary modulus is 0.025 m.

  3. 3. Keep the representation's limits

    Both coefficient axes use metre units, but Im W is not a second physical displacement. Supplied phases and the auxiliary circle give no time evolution, speed or measurement precision.

Original exact hypothetical representation: A = 0.025 m > 0, W(φ) = A e^(iφ), and the scalar displacement is q = Re W. The supplied angle is θ = φ rad; φ is its dimensionless numerical radian value. The displacement reference is fixed, with right positive along one physical line. The equally scaled complex-plane circle shows possible auxiliary coefficients for supplied phases. It is not an observed trajectory, and no phase–time rule is provided.

Worked examples

Divide an original complex pair

Calculate (2 + 3i)/(1 − i) in the form a + ib. These are exact dimensionless numbers.

  1. The denominator 1 − i is nonzero. Its conjugate is 1 + i.
  2. Multiply both numerator and denominator by 1 + i: [(2 + 3i)(1 + i)]/[(1 − i)(1 + i)].
  3. The numerator is 2 + 2i + 3i + 3i² = −1 + 5i. The denominator is 1 − i² = 2.
  4. Divide both coefficients by 2: −1/2 + (5/2)i. Multiplying this result by 1 − i recovers 2 + 3i.

−1/2 + (5/2)i. The nonzero denominator and the negative sign of i² are essential.

Check a conjugate and modulus

For the exact dimensionless number z = −8 + 15i, calculate z*, |z| and z z*.

  1. Reverse the imaginary coefficient's sign: z* = −8 − 15i.
  2. Square and add the real coefficients: (−8)² + 15² = 64 + 225 = 289.
  3. The nonnegative square root of 289 is 17, so |z| = 17.
  4. In the product (−8 + 15i)(−8 − 15i), the imaginary cross terms cancel and −225i² becomes +225. Thus z z* = 289 = |z|².

z* = −8 − 15i, |z| = 17 and z z* = 289. The negative real coefficient is compatible with a nonnegative modulus.

Extract the scalar at a cardinal phase

In the supplied model A = 0.025 m, W = A e^(iφ) and q = Re W, the angle is θ = (3π/2) rad. Find W, q and |W|, and state what the imaginary coefficient means here.

  1. Use φ = 3π/2, the numerical radian value. The unit-circle values are cos φ = 0 and sin φ = −1.
  2. Euler's formula gives e^(iφ) = −i, so W = 0 m + i(−0.025 m).
  3. Take the real coefficient: q = 0 m. The modulus is √[(0 m)² + (−0.025 m)²] = 0.025 m.
  4. Im W = −0.025 m is the representation's imaginary coefficient. The model supplies one scalar displacement and no second spatial motion or phase–time rule.

W = −i(0.025 m), q = 0 m and |W| = 0.025 m. The imaginary coefficient is auxiliary bookkeeping in this declared representation.

Try it yourself

  1. For the exact dimensionless number z = 6 − 11i, give Re z, Im z and z*. Does Im z include i?

    Show the answer and reasoning

    Re z = 6, Im z = −11 and z* = 6 + 11i. Im z does not include i.

    In a + ib, a and b are real coefficients. Here b = −11; conjugation changes b to +11.

  2. For exact dimensionless choices u = −3 + 2i and v = 5 − 7i, calculate u + v and u − v.

    Show the answer and reasoning

    u + v = 2 − 5i; u − v = −8 + 9i.

    Addition gives (−3 + 5) + i(2 − 7). Subtraction gives (−3 − 5) + i[2 − (−7)]. Subtracting a negative coefficient increases the imaginary coefficient.

  3. Calculate i(−2 + 7i). Give its complex-plane coordinates before and after multiplication, without assigning a physical motion.

    Show the answer and reasoning

    i(−2 + 7i) = −7 − 2i. The coordinates change from (−2, 7) to (−7, −2).

    Distribution gives −2i + 7i² = −7 − 2i. The coordinate rule (a, b) → (−b, a) describes the mathematical quarter-turn when both axes use the same scale.

  4. In exact dimensionless arithmetic, calculate 1/i using a conjugate. Is 1/0 defined, and what is |0|?

    Show the answer and reasoning

    1/i = −i; 1/0 is undefined; |0| = 0.

    The nonzero denominator i has conjugate −i. Multiplying numerator and denominator by −i gives (−i)/(−i²) = −i. A nonzero purely imaginary denominator is allowed; zero is not. The modulus is nonnegative and need not be strictly positive.

  5. A supplied angle is θ = −90°. Use 1° = (π/180) rad to find its numerical radian value φ, then calculate e^(iφ). What happens if 2π is added to φ?

    Show the answer and reasoning

    θ = (−π/2) rad, φ = −π/2 and e^(iφ) = −i. Adding 2π gives φ = 3π/2 and the same complex number −i.

    A clockwise quarter-turn from the positive real axis reaches (0, −1) on the unit circle. Thus cos φ = 0 and sin φ = −1. The exponent uses the numerical radian value, and a full turn returns to the same point.

  6. In the supplied model A = 0.025 m, W = A e^(iφ) and q = Re W, compare φ = 0 and φ = π/2. Give q and |W| at each. Do these two supplied phases determine how fast an object moves?

    Show the answer and reasoning

    At φ = 0, q = +0.025 m and |W| = 0.025 m. At φ = π/2, q = 0 m and |W| = 0.025 m. They do not determine a speed.

    The real coefficient changes from A to zero while the auxiliary modulus remains A. There are no times or phase–time rule in the stipulated model, so the phase comparison is not a speed calculation or evidence for circular object motion.

What to carry forward

  • For z = a + ib, Re z = a and Im z = b are real coefficients; i² = −1.
  • Complex arithmetic combines coefficients and uses i² = −1; division requires a nonzero denominator.
  • Conjugation reverses the imaginary coefficient, and the modulus √(a² + b²) is nonnegative.
  • For θ = φ rad, φ is the numerical radian input; unit-circle coordinates define cosine and sine for any real φ.
  • Euler's formula e^(iφ) = cos φ + i sin φ is an established mathematical relation; a diagram illustrates it without proving it.
  • A physical interpretation must be declared: in the selected scalar model q = Re W, the imaginary coefficient and auxiliary circle supply no second physical axis or time evolution.

References

Sources for the concepts and teaching approaches in this article.

  1. National Council of Educational Research and Training (NCERT)2 sources
    1. Mathematics, Chapter 4: Complex Numbers and Quadratic EquationsNational Council of Educational Research and Training (NCERT), IndiaTextbook chapter · PDFncert.nic.inRead source
    2. Physics Part II, Chapter 13: OscillationsNational Council of Educational Research and Training (NCERT), IndiaTextbook chapter · PDFncert.nic.inRead source
  2. Jay Abramson — OpenStax / Rice University2 sources
    1. Precalculus 2eJay Abramson — OpenStax / Rice UniversityTextbook chapterPrecalculus 2e, 5.1 AnglesPrecalculus 2e, 5.2 Unit Circle: Sine and Cosine Functionsopenstax.org
    2. College Algebra 2e, 6.1 Exponential FunctionsJay Abramson — OpenStax / Rice UniversityTextbook chapteropenstax.orgRead source
  3. The International System of Units (SI), 9th edition, version 4.01Bureau International des Poids et Mesures (BIPM)Reference guidebipm.orgRead source
  4. Bridging Course in Mathematics, Chapter 1: Complex NumbersRichard Earl — University of Oxford Mathematical InstituteCourse notes · PDFmaths.ox.ac.ukRead source