Trigonometry & Radians
Angles, waves and the unit circle
Angles, triangles and waves
The language of geometry and everything periodic
Trigonometry links angles to ratios of sides. SOHCAHTOA captures the three core functions, and the unit circle extends them to any angle — including the obtuse and reflex angles that turn up in molecular geometry and diffraction.
Chemistry measures angles in radians because that is what calculus expects: the clean identity holds only in radians. The conversion is . Sine and cosine then describe every wave — light, sound, quantum wavefunctions — with just three parameters: amplitude, frequency and phase.
The most important trig formula in analytical chemistry is Bragg's law, , which gives the spacing between crystal planes from the angle at which X-rays constructively interfere. Knowing at the diffraction peak is enough to deduce an atomic spacing to picometre precision.
Core identities and conversions
Crystallography and wave extras
- Calculator in degrees when radians are needed (or vice versa). Bragg's law uses , which is dimensionless and the same in both systems — but when evaluating integrals or derivatives involving trig, the variable must be in radians. Check your calculator mode before every calculation.
- Using cos instead of sin in Bragg's law. The correct form is where is the glancing angle (angle between the beam and the plane surface). A common mistake is to use the complement or write , which is valid only when is measured from the normal rather than the surface.
- Sign/convention errors with phase. A phase shift of shifts the wave left (earlier in time/space), while shifts it right. Mixing sign conventions when adding two waves can give a phase difference of instead of zero, incorrectly predicting constructive vs destructive interference.
- Forgetting the factor of 2 in the phase-difference formula. A path difference of corresponds to a phase difference of , not . Missing the factor of halves the predicted phase, turning what should be destructive interference into constructive.
The Miller-index spacing formula combines with Bragg's law to give a direct route from peak positions to the lattice parameter. Each observed reflection has a unique combination of integers (hkl); plotting against for a cubic crystal gives a straight line of slope . The systematic absences — certain (hkl) combinations that give no reflection in bcc or fcc — are a direct consequence of destructive interference from atoms at the cell centre or face centres, and they are what allows crystallographers to distinguish the cell type from a powder diffraction pattern.
Unit circle
Sweep the angle and read sine, cosine and tangent directly off the circle. sin²θ + cos²θ = 1 holds at every point.
A tetrahedral molecule has a bond angle of 109.47°. Express this in radians. Also convert the octahedral angle of 90° to radians.
X-rays of wavelength (Cu Kα) diffract from a set of NaCl planes at a first-order () Bragg angle of . Find the plane spacing .
Wave explorer
Adjust amplitude, frequency and phase. Two waves with a phase difference of π cancel completely — the maths of destructive interference.
An NMR free-induction decay (FID) is modelled as where is in seconds. Identify the amplitude, frequency (in Hz), and phase shift (in degrees).
Two atomic orbitals are described by and . Their sum is the bonding combination and their difference the antibonding. What value of gives maximum constructive interference, and what value gives complete cancellation?
Worked examples
Pull Bragg's law, SOHCAHTOA and wave interference together — try each before revealing the solution.
In a tetrahedral CH₄ molecule the C–H bond length is 109 pm and the bond angle is 109.47°. Using the bisector of the H–C–H angle, find the perpendicular distance from C to the line joining two H atoms.
Silicon (111) planes have spacing . At what angle does second-order () Bragg diffraction occur for Cu Kα radiation ()?
Two coherent light beams travel paths of and before recombining. The wavelength is . Calculate the phase difference and state whether the interference is constructive or destructive.
Platinum (fcc, ) gives a Bragg reflection at with Cu Kα radiation (). Find the d-spacing and hence the Miller indices (hkl) of the reflecting planes.
In small-angle X-ray scattering (SAXS) a polymer forms a lamellar repeat with spacing . The first-order Bragg peak occurs at scattering angle for . Verify Bragg's law exactly, then show the small-angle approximation ( in radians) gives the same answer to three significant figures.
A powder diffraction pattern of a cubic metal recorded with Mo Kα radiation () shows first-order peaks at and . Index these two peaks (assign Miller indices), deduce the lattice parameter , and identify the cell type (sc, bcc, or fcc) from the systematic absences.
Check yourself
Four quick questions on angles, waves and Bragg's law.
How many radians are in 180°?