Coulomb`s Law
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Transcript Coulomb`s Law
Minute Paper
• If you know the input and the output, but you don’t know
the circuitry, using the transfer function can you figure out
the circuitry without seeing it?
• In the lab, which variable was frequency, w or f?
• What did the DC voltmeter say when it got AC power?
• Do you use HP and LP filters in stereo to send the high
frequencies to the tweeters and the low frequencies to
subwoofer?
• Can you give some practice exams?
RLC Band-pass Filters
V0 jw
ZR
Vi jw
ZC Z L Z R
H V jw
R
1
j wL R
jw C
jwRC
2
1 jw LC jwRC
Aw
w
w
1 j 1 j
w1
w2
1
1
1
LC ;
RC
w1w2
HV jw
Aw
w
1
w1
2
w
1
w2
2
e
w
w
j arctan arctan
w1
w2
2
w1
w2
Band-pass Filters and Resonant Circuits
HV jw
w w
1 Q 2 0
w0 w
1
LC
w0 L
R
w w
1 jQ 0
w0 w
1
w0
Q
1
w0
B
2
e
w w
arctan Q 0
w0 w
Resonant frequency
w0
w2 w1
Quality factor
RLC Resonant
when w w0
wL
1
wC
jwL
1
jwC
Z L ZC
I jw
V ( jw )
Z R Z L ZC
At resonance:
• current is max.
• Zeq =R
• current and voltage
are in phase.
• the higher Q, the
narrower the resonant
peak.
V
1
R j wL
wC
V
V
I
2
R
1
2
R wL
wC
Applications:
tuning circuit
Concept Check: ac Circuit Resonance
The current in an RLC series circuit leads the ac voltage source.
To bring the circuit to resonance, should the capacitance be
increased or decreased?
Answer: ICE, it is capacitive, reduce the impedance of the
capacitor, i.e. increase the capacitance. Alternatively, inductance
can be increased to offset the impedance of the capacitor.
Ex: Notch filter, p303
Decibel Measure
•
•
Amplifier gain and filter loss are often specified in decibels (dB), a logarithmic
measure of ratios. Most generally dB are specified for power ratios,
– power gain in dB= 10 log10 (Pout/Pin)
– More generally in this course, we are interested in voltage gain;
since P ~ V2, voltage gain in dB= 20 log10 |Vout/Vin|
Advantages of decibel measures:
– Ease of handling large quantities that can vary over many orders of
magnitude.
• However, keep this compression firmly in mind! For example, the
Richter scale for earthquake intensity is logarithmic -- a 7 on the
Richter scale actually has an amplitude 10 times more powerful than a
6, corresponding to a factor of about 31-32 times more energy.
– In cascaded amplifier/filter systems, the overall gain is the product
of each stage's gain. Since log(A.B) = log(A) + log(B), if one
wishes to consider the overall gain of several stages, one simple
adds the gain of each in dB measure.
– As we will see below, the frequency dependence of an amplifier or
filter is most often summarized on a Bode plot. For a Bode plot,
the log of the |gain| is plotted against the log of the frequency. Thus
in dB measure the vertical axis becomes a linear axis.
Bode Plots
Consider a RC low-pass filter:
Let us plot filter gain vs. the dimensionless frequency w' = wRCw/w0
w'
Vout/Vin
0.01
1.000 =
0 dB
0.1
0.995 =
0 dB
1
0.707 =
- 3 dB
10
0.100 =
- 20 dB
100
0.010 =
- 40 dB
• At low enough frequencies the gain flattens off at unity,
0 dB.
• At large enough frequencies, the gain is falling off at
the rate of - 20 dB per decade of frequency (a factor of
10 increase in frequency). This fall-off is also often
referred to as - 6 dB per octave (a factor of 2 increase in
frequency.) Convince yourself of the equivalence!
w'
Vout/Vin
Bode Plots: cont.
0.01
1.000 =
0 dB
0.1
0.995 =
0 dB
1
0.707 =
- 3 dB
10
0.100 =
- 20 dB
100
0.010 =
- 40 dB
• cutoff frequency, where w' = 1, i.e. ww0=1/RC, the
gain is - 3 dB. The - 3 dB point is considered to be the
breakpoint.
•The Bode plot for the RC low-pass filter is often sketched
by drawing a horizontal line up to the breakpoint followed
by a line falling off at - 20 dB per decade as shown by the
blue line in the graph below. The actual gain curve is
shown in red for comparison; the largest error in the
approximation is at the breakpoint. This type of
approximate plot is known as an asymptotic Bode plot.
Bode Plot: High-pass filter
3db point
20 dB/Decade