Difference between revisions of "TF EIM Chapt3"

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The voltage changes in between point <math>a</math> and DC are passed according to what you select for the break frequency (<math>\omega_B = \frac{1}{RC}</math>)
 
The voltage changes in between point <math>a</math> and DC are passed according to what you select for the break frequency (<math>\omega_B = \frac{1}{RC}</math>)
 +
 +
In the above pulse picture it was assumed that \tau >> \frac{1}{\omega_B}
  
 
=Integrator=
 
=Integrator=

Revision as of 17:38, 8 February 2011

Differentiator circuit

Consider the effect of a low-pass filter on a rectangular shaped input pulse with a width [math]\tau[/math] and period [math]T[/math].


TF EIM PulsedRCHighpass.png


The first thing to consider is what happens to the different parts of the square pulse as it travels to the circuit.

You know that the circuit, as a high pass filter, will tend to attenuate low frequency (slow changing) voltages and not high frequency (quick changing) voltages.

This means no DC voltage values pass beyond the capacitor.

This means that points [math]a[/math] and [math]b[/math] in the pulse shown below should pass through the circuit.

TF EIM SquarePulseDifferentiated.png

The voltage changes in between point [math]a[/math] and DC are passed according to what you select for the break frequency ([math]\omega_B = \frac{1}{RC}[/math])

In the above pulse picture it was assumed that \tau >> \frac{1}{\omega_B}

Integrator

TF EIM PulsedRCLowpass.png

TF EIM SquarePulse.png

Forest_Electronic_Instrumentation_and_Measurement