INGENIA

ODE-02

Harmonic oscillator

Undamped.

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ODESHO

Governing equation

y=Acos(omegat+phi)y=A\\cos(\\omega t+\\phi)

t∈[0,10]t \in \left[0, 10\right]

where

A
A (—)
\omega
ω (rad/s)
t
t (s)
y
y (—)

The figure, part by part

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ODE-02 · pendulum
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①

Governing law — red

y=Acos(omegat+phi)y=A\\cos(\\omega t+\\phi)

t∈[0,10]t \in \left[0, 10\right]

t=0t = 0y=1y = 1

②

Domain of the variable — blue

tmin⁡=0,tmax⁡=10t_{\min} = 0,\quad t_{\max} = 10

t∈[0,10]t \in \left[0, 10\right]

t=0t = 0t=0t = 0

③

Response curve — green

y=Acos(omegat+phi)y=A\\cos(\\omega t+\\phi)

t∈[0,10]t \in \left[0, 10\right]

t=0t = 0y=1y = 1

④

Rate of change — amber

dydt\frac{\mathrm{d}y}{\mathrm{d}t}

t∈[0,10]t \in \left[0, 10\right]

t=0.063t = 0.063y′=−0.25y^{\prime} = -0.25

Lecture brief

Historical brief

Exponential decay, the harmonic oscillator, SIR epidemics, Lotka–Volterra and Bessel are the first solvable ODEs of nature and populations. The lab is rate, period and phase portrait in closed form. This sheet (ODE-02 — Harmonic oscillator) is the form associated with SHO. Working symbols: AA, ω\omega, tt →\rightarrow yy. Undamped.

Purpose

Purpose: compute yy from AA, ω\omega, tt in Differential equations via y=Acos(omegat+phi)y=A\\cos(\\omega t+\\phi) Undamped. Use it when a real differential equations question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given A=1.000 —A = 1.000\,\mathrm{—}, ω=2.000 rad/s\omega = 2.000\,\mathrm{rad/s}, t=1.000 st = 1.000\,\mathrm{s}, the governing relation y=Acos(omegat+phi)y=A\\cos(\\omega t+\\phi) yields y=−0.4161 —y = -0.4161\,\mathrm{—}. Undamped. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • y y-0.4161 —
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ODE-02 · pendulum
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Narration of this film

Undamped.

Undamped.

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