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Differential Equations
The Geometric View of ODEs
01Direction Fields and the Geometric View of ODEs02Integral Curves and the Isocline Method03Perpendicular Isoclines: The Circles of y' = -x/y04Isocline Corridors and a Trap for Solutions05Existence and Uniqueness: One Curve Through a Point06Where Existence and Uniqueness FailProblem set0/10Problem set 20/10MIT problem set0/3
Numerical Methods
01Euler's Method and Its Three Equations02Euler's Method by Hand: Building the Table03Convexity and the Sign of Euler's Error04First Order Error: Halve the Step, Halve the Error05Improved Euler (RK2): Averaging Two Slopes06Runge-Kutta 4 and the Price of Accuracy07Singular Points: Where Every Method FailsProblem set0/10Problem set 20/10MIT problem set0/1
First-Order Linear Equations
01First Order Linear: Standard Form and the Sign of p02The Conduction-Diffusion Model: Newton's Law of Cooling03The Integrating Factor and the Four-Step Method04Integrating Factors: Two Mistakes and a Trick Question05Constant Coefficients: Steady State and TransientProblem set0/10Problem set 20/10MIT problem set0/1
Substitution Methods
01Scaling a First Order ODE: The Fourth-Power Cooling Law02The Bernoulli Equation and the Substitution v = y^(1-n)03A Worked Bernoulli Example: The Substitution v = 1/y04Homogeneous Equations: The Zoom Test and y = zx05Modelling the Lighthouse Chase: A 45-Degree Heading06The Boat's Path: A Logarithmic Spiral in Polar CoordinatesProblem set0/10Problem set 20/10
Autonomous Equations
01Autonomous Equations and Time-Translation Invariance02Critical Points: Constant Solutions as Barriers03The Embezzler Model dy/dt = ry - w: One Unstable Balance04The Logistic Equation: Carrying Capacity Without Solving05Stable, Unstable and Semi-Stable Critical Points06Maximum Sustainable Harvest: Why h = a^2/4bProblem set0/10Problem set 20/10MIT problem set0/3
Complex Numbers
01Complex Division, Polar Form and the Definition of e^(iθ)02Why e^(iθ) Earns Its Name: Multiply Moduli, Add Angles03Integrating e^(-x) cos x by Complexifying04The nth Roots of Unity: Zeta on the Unit CircleProblem set0/10Problem set 20/10MIT problem set0/4
Input and Response
01Steady-State and Transient Solutions of y' + ky = q(t)02Input, Response and the Superposition Principle03Solving y' + ky = k cos ωt by Complexification04Amplitude and Phase Lag of a Sinusoidal ResponseProblem set0/10Problem set 20/10MIT problem set0/2
01Cartesian Method: Rationalise, Then Take the Real Part02The Sinusoidal Identity and Its Right Triangle03Three Proofs of the Sinusoidal Identity04The Mixing Tank: Salt Balance and k = r/V05RC Circuits, Decay Chains and Negative kProblem set0/10Problem set 20/10MIT problem set0/2
Second-Order Linear Equations
01Second-Order Linear ODEs and the Spring–Mass–Dashpot02The Characteristic Equation and Overdamped Motion03Complex Roots a ± bi and Underdamped Oscillation04Critical Damping and Reduction of Order: t e^(−at)Problem set0/10Problem set 20/10MIT problem set0/2

Three Proofs of the Sinusoidal Identity

How can one identity be proved by a trig expansion, a dot product and a complex product, and why does the familiar proof run backwards?


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Your summary note

    1. 1

      The angle-difference proof and its direction

      Expand Acos⁡(θ−ϕ)A\cos(\theta-\phi)Acos(θ−ϕ) with the cosine-of-a-difference formula, match coefficients to get a=Acos⁡ϕa = A\cos\phia=Acosϕ and b=Asin⁡ϕb = A\sin\phib=Asinϕ, and record that this proof runs backwards.

    2. 2

      The dot-product proof with uθ=⟨cos⁡θ,sin⁡θ⟩\mathbf{u}_\theta = \langle\cos\theta, \sin\theta\rangleuθ​=⟨cosθ,sinθ⟩

      Compute ⟨a,b⟩⋅uθ\langle a, b\rangle \cdot \mathbf{u}_\theta⟨a,b⟩⋅uθ​ once from components and once as magnitudes times the cosine of the included angle θ−ϕ\theta - \phiθ−ϕ, and equate the two.

    3. 3

      The complex proof via (a−bi)eiθ(a-bi)e^{i\theta}(a−bi)eiθ

      Show Re⁡[(a−bi)(cos⁡θ+isin⁡θ)]=acos⁡θ+bsin⁡θ\operatorname{Re}[(a-bi)(\cos\theta + i\sin\theta)] = a\cos\theta + b\sin\thetaRe[(a−bi)(cosθ+isinθ)]=acosθ+bsinθ, write a−bi=a2+b2 e−iϕa - bi = \sqrt{a^2+b^2}\,e^{-i\phi}a−bi=a2+b2​e−iϕ, multiply in polar form, and take real parts.

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