NATIONAL COLLEGE OF SCIENCE AND TECHNOLOGY Amafel Bldg. Aguinaldo Highway Dasmariñas City, Cavite EXPERIMENT # 1 Passive Low-Pass and High-Pass Filter Balane, Maycen June 28, 2011 Signal Spectra and Signal Processing/ BSECE 41A1 Score: Eng’r. Grace Ramones Instructor
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NATIONAL COLLEGE OF SCIENCE AND TECHNOLOGY
Amafel Bldg. Aguinaldo Highway Dasmariñas City, Cavite
EXPERIMENT # 1
Passive Low-Pass and High-Pass Filter
Balane, Maycen June 28, 2011
Signal Spectra and Signal Processing/ BSECE 41A1 Score:
Eng’r. Grace Ramones
Instructor
OBJECTIVES
1. Plot the gain frequency response of a first-order (one-pole) R-C low-pass filter.
2. Determine the cutoff frequency and roll-off of an R-C first-order (one-pole)
low-pass filter.
3. Plot the phase-frequency of a first-order (one-pole) low-pass filter.
4. Determine how the value of R and C affects the cutoff frequency of an R-C low-
pass filter.
5. Plot the gain-frequency response of a first-order (one-pole) R-C high pass
filter.
6. Determine the cutoff frequency and roll-off of a first-order (one-pole) R-C
high pass filter.
7. Plot the phase-frequency response of a first-order (one-pole) high-pass filter.
8. Determine how the value of R and C affects the cutoff frequency of an R-C
high pass filter.
COMPUTATION
(Step 4)
−0.01 dB = 20 log A
−0.01 dB
20=
20 log A
20
−0.05 × 10−3 = log A
10−0.05×10−3= 10log A
10−0.05×10−3= A
A = 0.99988 ≅ 1
(Step 6)
𝑓𝐶 =1
2𝜋𝑅𝐶=
1
2𝜋(0.02µ𝐹)(1𝑘Ω)
= 7.957747𝑘𝐻𝑧 ≅ 7.958𝑘𝐻𝑧
(Question – Step 6)
%𝑑𝑖𝑓𝑓𝑒𝑟𝑒𝑛𝑐𝑒 = |(7.958𝑘𝐻𝑧 − 7.935𝐾𝐻𝑧
7.958𝑘𝐻𝑧|
× 100% = 0.29%
Question – (Step 7 )
(−2.998dB) – (20.108 dB) = 17.11dB
(Step 15)
0 dB = 20 log A
0 dB
20=
20 log A
20
0 = log A
100 = 10log A
100 = A
A = 1
(Step 17)
𝑓𝐶 =1
2𝜋𝑅𝐶=
1
2𝜋(0.02µ𝐹)(1𝑘Ω)
= 7.957747𝑘𝐻𝑧 ≅ 7.958𝑘𝐻𝑧
Question (Step 17)
%𝑑𝑖𝑓𝑓𝑒𝑟𝑒𝑛𝑐𝑒 = |(7.958𝑘𝐻𝑧 − 7.935𝐾𝐻𝑧
7.958𝑘𝐻𝑧|
× 100% = 0.29%
Question (Step 18 )
20.159 dB − (−2.998dB) = 18.161dB
DATA SHEET
MATERIALS
One function generator
One dual-trace oscilloscope
Capacitors: 0.02 µF, 0.04µF
Resistors: 1 kΩ, 2 kΩ
THEORY
In electronic communication systems, it is often necessary to separate a specific
range of frequencies from the total frequency spectrum. This is normally
accomplished with filters. A filter is a circuit that passes a specific range of
frequencies while rejecting other frequencies. A passive filter consists of passive
circuit elements, such as capacitors, inductors, and resistors. There are four basic
types of filters, low-pass, high-pass, band-pass, and band-stop. A low-pass filter is
designed to pass all frequencies below the cutoff frequency and reject all frequencies
above the cutoff frequency. A high-pass is designed to pass all frequencies above the
cutoff frequency and reject all frequencies below the cutoff frequency. A band-pass
filter passes all frequencies within a band of frequencies and rejects all other
frequencies outside the band. A band-stop filter rejects all frequencies within a band
of frequencies and passes all other frequencies outside the band. A band-stop filter
rejects all frequencies within a band of frequencies and passes all other frequencies
outside the band. A band-stop filter is often is often referred to as a notch filter. In
this experiment, you will study low-pass and high-pass filters.
The most common way to describe the frequency response characteristics of a filter
is to plot the filter voltage gain (Vo/Vi) in dB as a function of frequency (f). The
frequency at which the output power gain drops to 50% of the maximum value is called
the cutoff frequency (fC). When the output power gain drops to 50%, the voltage gain
drops 3 dB (0.707 of the maximum value). When the filter dB voltage gain is plotted
as a function of frequency on a semi log graph using straight lines to approximate the
actual frequency response, it is called a Bode plot. A bode plot is an ideal plot of filter
frequency response because it assumes that the voltage gain remains constant in the
passband until the cutoff frequency is reached, and then drops in a straight line. The
filter network voltage in dB is calculated from the actual voltage gain (A) using the
equation
AdB = 20 log A
where A = Vo/Vi
A low-pass R-C filter is shown in Figure 1-1. At frequencies well below the cut-off
frequency, the capacitive reactance of capacitor C is much higher than the resistance
of resistor R, causing the output voltage to be practically equal to the input voltage
(A=1) and constant with the variations in frequency. At frequencies well above the
cut-off frequency, the capacitive reactance of capacitor C is much lower than the res-
istance of resistor R and decreases with an increase in frequency, causing the output
voltage to decrease 20 dB per decade increase in frequency. At the cutoff frequency,
the capacitive reactance of capacitor C is equal to the resistance of resistor R,
causing the output voltage to be 0.707 times the input voltage (-3dB). The expected
cutoff frequency (fC) of the low-pass filter in Figure 1-1, based on the circuit
component value, can be calculated from
XC = R 1
2𝜋𝑓𝐶 𝐶= 𝑅
Solving for fC produces the equation 1
2𝜋𝑅𝐶= 𝑓𝐶
A high-pass R-C filter is shown in figure 1-2. At frequencies well above the cut-off
frequency, the capacitive reactance of capacitor C is much lower than the resistance
of resistor R causing the output voltage to be practically equal to the input voltage
(A=1) and constant with the variations in frequency. At frequencies well below the cut-
off frequency, the capacitive reactance of capacitor C is much higher than the
resistance of resistor R and increases with a decrease in frequency, causing the
output voltage to decrease 20 dB per decade decrease in frequency. At the cutoff
frequency, the capacitive reactance of capacitor C is equal to the resistance of
resistor R, causing the output voltage to be 0.707 times the input voltage (-3dB). The
expected cutoff frequency (fC) of the high-pass filter in Figure 1-2, based on the
circuit component value, can be calculated from 1
2𝜋𝑅𝐶= 𝑓𝐶
Fig 1-1 Low-Pass R-C Filter
When the frequency at the input of a low-pass filter increases above the cutoff
frequency, the filter output drops at a constant rate. When the frequency at the
input of a high-pass filter decreases below the cutoff frequency, the filter output
voltage also drops at a constant rate. The constant drop in filter output voltage per
decade increase (x10), or decrease (÷10), in frequency is called roll-off. An ideal low-
pass or high-pass filter would have an instantaneous drop at the cut-off frequency
(fC), with full signal level on one side of the cutoff frequency and no signal level on the
other side of the cutoff frequency. Although the ideal is not achievable, actual filters
roll-off at -20dB/decade per pole (R-C circuit). A one-pole filter has one R-C circuit
tuned to the cutoff frequency and rolls off at -20dB/decade. At two-pole filter has
two R-C circuits tuned to the same cutoff frequency and rolls off at -40dB/decade.
Each additional pole (R-C circuit) will cause the filter to roll-off an additional -
20dB/decade. Therefore, an R-C filter with more poles (R-C circuits) more closely
approaches an ideal filter.
In a pole filter, as shown the Figure 1-1 and 1-2 the phase (θ) between the input and
the output will change by 90 degrees and over the frequency range and be 45 degrees
at the cutoff frequency. In a two-pole filter, the phase (θ) will change by 180 degrees
over the frequency range and be 90 degrees at the cutoff frequency.
Fig 1-2 High-Pass R-C Filter
PROCEDURE
Low-Pass Filter
Step 1 Open circuit file FIG 1-1. Make sure that the following Bode plotter