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RC Circuit Filtering: Understanding Low-Pass Filters and Bode Plots, Lab Reports of Introduction to Sociology

The use of rc circuits for filtering time-varying signals through the analysis of a low-pass filter and a second-order chebyshev filter. The theory behind the circuits, their transfer functions, and the concept of the bode plot. Students will learn how to calculate the gain and phase of the filters and understand the significance of the cutoff frequency.

Typology: Lab Reports

2009/2010

Uploaded on 03/28/2010

koofers-user-eml
koofers-user-eml 🇺🇸

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Download RC Circuit Filtering: Understanding Low-Pass Filters and Bode Plots and more Lab Reports Introduction to Sociology in PDF only on Docsity! ELVIS Experiment #4 – Filtering Introduction: This experiment demonstrates how circuits involving resistors and capacitors (RC circuits) can be used to filter time-varying signals. In the first part of the experiment, a sine wave is used as an input to the circuit shown in Figure 1. R 100 kOhm Vs A cos (wt) C 100 nF Vo Figure 1: RC low-pass filter. In the second part of the experiment, an RC filter involving two capacitors and an Op Amp is added to the summer circuit from experiment 3. This filters out high frequencies from the music being played as well as the noise added by the function generator. This is demonstrated by increasing the frequency of the added noise, and noticing that as the frequency increases, the volume of the noise decreases. Circuit Analysis: The circuit in Figure 1 can be analyzed using Laplace domain circuit analysis. The impedance of the resistor is R and the impedance of the capacitor is sC 1 . The circuit can then be treated as a voltage divider, so that ( ) ( ) ( )sV s sV sC R sC sV s RC RC so 1 1 1 1 + = + = . The input-output relationship ( ) ( ) ( )sV sV sT s o! is called the transfer function of the circuit. The transfer function describes how the circuit acts when the input is a sine or cosine wave with a frequency of ! rad/sec. Because the circuit is linear, the output will be a sine or cosine wave of the same frequency as the input, but the amplitude of the output may be different from that of the input, and the two waves may not reach their peaks at the same time. Stated mathematically, if the input is ( )tAV s !cos= , then the output will be of the form ( )!" += tBV o cos . The ratio of B to A and the value of the angle ! change with frequency. We can determine these two values by using the transfer function and setting !js = . This will give a complex function of ! . The ratio of B to A is called the gain, and is the length of the complex function. The angle ! is called the phase, and is the angle that the complex function makes with the positive real axis in the complex plane. The gain and phase of the RC circuit are calculated below. ( ) ( )212 1 1 1 RC RC RC RC j jT +! = + = "" " ( ) ( ) ( )RCj j jT RC RCRC RC RC ! ! ! ! ! arctanarctan0 1 11 1 1 ="" # $ %% & ' (=+)()=* + , - . / + )=) The plots of the gain and phase are together called the frequency response, or Bode plot of the circuit. The Bode plot of the circuit is shown below. (Note that the vertical scale of the gain plot is in units of decibels, which is a logarithmic unit. The horizontal scales of both plots are also logarithmically spaced.) Figure 4: Implementation of RC low-pass filter. Figure 5: Input to the RC low-pass filter (Channel B) and output from the filter (Channel A) at approximately twice the cut-off frequency. RC filter Capacitor Input Output To implement the second part of the experiment, an Op-Amp implementation of a second order Chebyshev filter is added to the summer from experiment 3, allowing noise above around 5,000 Hz to be eliminated. The complete summer with added filter is shown in Figure 6. Figure 6: Implementation of Chebyshev filter. Chebyshev filter RC filter Summer from experiment 3
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