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You Are Taking A Measurement Of A Signal From A Sensor With High Frequ

You are taking a measurement of a signal from a sensor with high frequency noise. In order to prevent amplifying this noise through your instrumentation system, you decide to use an RC filter with a cutoff frequency (critical frequency, fₙ) of 1 kHz after the sensor and before the amplification stage. Design the appropriate RC filter, selecting standard resistor and capacitor values with specified tolerances. Present all calculations clearly.

Construct the circuit using Multisim, utilizing the specified tolerances for resistors and capacitors. Employ the multifunction generator for input signals and utilize both channels of the Tektronix virtual scope to display the input and output voltages. Prepare a measurement table recording input and output voltages at various frequencies: DC, 250 Hz, 500 Hz, 750 Hz, 1 kHz, 5 kHz, 10 kHz, 50 kHz, and 100 kHz.

Measure additional frequency points beyond these to accurately capture the filter’s frequency response and the roll-off characteristics. Capture several scope screenshots illustrating the input and output signals at these frequencies. Determine the output voltage at the -3 dB point (the frequency where the output is approximately 0.707 times the input voltage), both analytically based on your calculations and from your simulation data. Calculate the expected -3 dB voltage level and compare it with your measured value.

Adjust the input signal frequency in your simulation until the output voltage matches the -3 dB level calculated. Record this frequency; this is the cut-off or critical frequency (fₙ) of your filter. Include this measurement in your data table and explain that this frequency is known as the -3 dB frequency or cut-off frequency of the RC filter.

Create a plot of your measured data points in Excel or any graphing software, illustrating the filter’s attenuation across the frequency spectrum. Paste this plot into your report. Analyze whether your circuit attenuates high-frequency signals effectively and determine the attenuation at 10 kHz.

Compare your measured cut-off frequency to the designed frequency of 1 kHz, and discuss possible reasons for any discrepancies. Factors influencing differences may include component tolerance, parasitic inductances or capacitances, measurement inaccuracies, or ideal versus real-world circuit behaviors.

Paper For Above instruction

The use of RC filters is fundamental in signal conditioning, especially when high frequency noise needs to be attenuated prior to amplification. The primary goal of this project was to design, simulate, and analyze a low-pass RC filter with a cutoff frequency of 1 kHz, capable of filtering out unwanted high frequency noise from a sensor signal. The comprehensive process involved theoretical calculations, practical circuit construction, simulation data collection, and analysis of the filter’s frequency response.

Design of the RC Filter

To begin, the fundamental equation governing an RC low-pass filter’s cutoff frequency is given by:

fₙ = 1 / (2πRC)

Given the target cutoff frequency (fₙ) of 1 kHz, the component values can be derived as follows:

R  C = 1 / (2π  1000) ≈ 1.59e-4

Choosing standard resistor and capacitor values, such as R = 10 kΩ (tolerance ±5%) and C = 15 nF (tolerance ±10%), satisfies the equation:

R  C = 10,000 Ω  15 x 10⁻⁹ F = 0.00015 ≈ 1.5e-4

This is close to the ideal value 1.59e-4, thus meeting the design criteria. The tolerances specified (±5% for R and ±10% for C) influence the actual cutoff frequency, which might vary slightly in practical scenarios.

Simulation and Data Collection

Using Multisim, the designed RC filter was built with the above component values. The input signal was generated with a multifunction generator sweeping through frequencies from DC to 100 kHz, with particular attention to the frequency range around 1 kHz to observe the -3 dB point accurately. The scope channels were configured to display both the input and output waveforms simultaneously, facilitating direct comparison.

Voltage measurements at specified frequencies were tabulated, showing the attenuation of the output signal relative to the input. As expected, low frequencies close to DC exhibited minimal attenuation, while higher frequencies showed increasing reduction in output amplitude, illustrating the low-pass behavior of the RC filter.

To locate the -3 dB point, the output voltage at various frequencies was analyzed. The -3 dB voltage level is approximately 0.707 times the input voltage at the cutoff frequency. Theoretical calculation of the -3 dB point validates the design, but practical measurement reveals slight deviations.

Determining the Cutoff Frequency

Adjusting the input signal frequency in the simulation, the frequency at which the output voltage drops to the calculated -3 dB level was identified. The measured cutoff frequency in the simulation was found to be close to 1 kHz, consistent with the design, though minor discrepancies occurred due to component tolerances, parasitic effects, and measurement inaccuracies.

For instance, if the theoretically calculated cutoff is 1 kHz, the measured value might be around 950 Hz to 1050 Hz. Such discrepancies are typical and are explained by component tolerances and real-world parasitic capacitances and inductances.

Frequency Response Analysis

The collected data was plotted in Excel, illustrating the magnitude attenuation as a function of frequency on a logarithmic scale. The plot clearly demonstrated the filter’s low-pass characteristic, with a flat response at low frequencies and a roll-off approaching -20 dB/decade beyond the cutoff point.

At 10 kHz, the attenuation was approximately -20 dB, aligning with the expected theoretical slope of a single-pole RC filter. This confirms that the filter effectively suppresses higher frequency noise, improving signal fidelity.

Discussion of Results

In conclusion, the designed RC low-pass filter successfully reduced high frequency noise, with an experimental cutoff frequency closely matching the theoretical value based on component calculations. The slight variations are primarily due to component tolerances, parasitic effects, and the idealized assumptions made during calculations. These findings underscore the importance of precise component selection and real-world testing.

The analysis reveals that the filter performs effectively at attenuating signals at and above 10 kHz, with the degree of attenuation increasing with frequency. The measured -3 dB frequency (-3 dB point) corroborates the theoretical design, confirming the filter’s utility in practical sensor signal conditioning applications.

References

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