Ludium
Sign In
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
01One Complex Root Is Enough: Conjugates and Real Solutions02When a Damped Spring Oscillates: p Below ω₀03Damped Oscillations: Pseudo-Period and ω₁² + p² = ω₀²Problem set0/10Problem set 20/10MIT problem set0/1
01Superposition: Why Linearity Makes c₁y₁ + c₂y₂ a Solution02The Wronskian and Abel's Theorem: Fitting Any Initial Values03Normalized Solutions: Why cosh x and sinh x Solve y'' − y = 004Uniqueness: Why c₁y₁ + c₂y₂ Is Every SolutionProblem set0/10Problem set 20/10

Perpendicular Isoclines: The Circles of y' = -x/y

Why do the line elements along every isocline of $y' = -x/y$ stand perpendicular to the isocline itself?


Loading…

←Previous Integral Curves and the Isocline MethodNext Isocline Corridors and a Trap for Solutions →

Your summary note

    1. 1

      Isoclines as lines y=−(1/C)xy = -(1/C)xy=−(1/C)x

      Set −x/y=C-x/y = C−x/y=C, rewrite as y=−(1/C)xy = -(1/C)xy=−(1/C)x, draw the C=1C = 1C=1 and C=−1C = -1C=−1 cases, and show the elements of slope CCC are perpendicular to each isocline.

    2. 2

      Recovering the axes: Cy=−xCy = -xCy=−x

      Rewrite the isocline as Cy=−xCy = -xCy=−x to get the yyy-axis at C=0C = 0C=0 with horizontal elements, and record that the xxx-axis is excluded but included by convention as 'C=∞C = \inftyC=∞' with vertical elements.

    3. 3

      Integral curves x2+y2=c12x^2 + y^2 = c_1^2x2+y2=c12​

      State that curves perpendicular to the rays are circles centred at the origin, and confirm by separating variables y dy=−x dxy\,dy = -x\,dxydy=−xdx and integrating to those circles.

    4. 4

      Limited domain of y=c12−x2y = \sqrt{c_1^2 - x^2}y=c12​−x2​

      Write the explicit solution, note its domain runs only from −c1-c_1−c1​ to c1c_1c1​, and record that a solution's domain cannot be read off the differential equation in advance.

    Attempt 1 of 2