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. |