Mathlets

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

Amplitude and Phase: 1st order

The tide in a harbor lags behind that of the open ocean, and is controlled by a first order linear equation. Bode and Nyquist plots illustrate the steady state solution and method of solution.

Amplitude and Phase: 2nd order I

A spring/dashpot/mass system is driven sinusoidally through the spring. The sinuoidal system response has predictable amplitude and phase lag, which can be understood using Bode and Nyquist plots.

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