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Unformatted text preview: 32 Class 2: Capacitors and RC Circuits Topics:
0 new:
~ Capacitors: dynamic description
— RC circuits
0 Time domain: )
° step response
0 integrator, diﬁerentiator (approximate)
0 Frequency domain: ﬁlters
Capacitors Today things get a little more complicated, and more interesting, as we meet frequency
dependent circuits, relying on the capacitor to implement this new trick. Capacitors let us
build circuits that “remember” their recent history. That ability allows us to make timing
circuits (circuits that let this happen a predetermined time after that occurs); the most
important of such circuits are oscillators—circuits that do this timing operation over and
over, endlessly, in order to set the frequency of an output waveform. The capacitor’s
memory also lets us make circuits that respond mostly to changes (dzﬁerentiators) or mostly
to averages (integrators), and—by far the most important—circuits that favor one frequency
range over another (ﬁlters). All of these circuit fragments will be useful within later, more complicated circuits. The
ﬁlters, above all others, will be with us constantly as we meet other analog circuits. They
are nearly as ubiquitous as the (resistive—) voltage divider that we met in the ﬁrst class. insulator. can be Vrcuum, 15:42‘ I's // may an last/am "c/Ie/a'cfn'c” mafen'al such as crank, [Jest12:, or a Digital oxide 79in give: greater capacitance fer amt area.
Figure N2.1: The simplest capacitor conﬁguration: sandwich
This capacitor .is drawn to look like a ham sandwich: metal plates are the bread, some
dielectric is the ham (ceramic capacitors really are about as simple as this). More often,
capacitors achieve large area (thus large capacitance) by doing something tricky, such as
putting the dielectric between two thin layers of metal foil, then rolling the whole thing up like a roll of paper towel (mylar capacitors are built this way).
Text sec. 1.12 p
A static description of the way a capacitor behaves would say
. Q = CV ,
where Q is total charge, C is the measure of how big the cap is (how much charge it can
store at a given voltage: C = Q/V), and Vis the voltage across the cap. _ N 2 — 2 Class 2: Capacitors & RC Circuits 33 This statement just deﬁnes the notion of capacitance. It is a Physicist’s way of describing
how a cap behaves, and rarely will we use it again. Instead, we use a dynamic description—a statement of how things change with time:
I = C dV/dt .
This is just the time derivative of the “static” description. C is constant with time; I is
deﬁned as the rate at which charge ﬂows. This equation isn’t hard to grasp: it says ‘The
bigger the current, the faster the cap’s voltage changes.’ .
Again, ﬂowing water helps intuition: think of the cap (with one end grounded) as a tub that can hold charge: Figure N22: A cap with one end grounded works a10t like a tub of water
A tub of large diameter (cap) holds a lot of water (charge), for a given height (V). If you fill
the tub through a thin straw (small I), the water level—V—will rise slowly; if you ﬁll or drain through a ﬁre hose (big I) the tub will ﬁll (“charge”) or drain (“discharge”) quickly. A
tub of large diameter (large capacitor) takes/longer to ﬁll or drain than a small tub. Self evident, isn’t it? Timedomain Description
Text sec. 1.13
Now let’s leave tubs of water, andanticipate what we will see when we watch the voltage
on a cap change with time: when we look on a scopescreen, as you will do in Lab 2. An easy case: constant 1 Text sec. 1.15;
+v ’
1' ,
i large I
Vcap V
c T see Fig. 1.43
"time Small I Figure N23: Easy case: constantI—> constant dV/dt This tidy waveform, called a ramp, is useful, and you will come to recognize it as the
signature of this circuit fragment: capacitor driven by constant current (or,“current source”). 34 Class 2: Capacitors & RC Circuits N2 — 3 This arrangement is used to generate a triangle waveform, for example: Compare Text sec.1.15,
Fig. 1.42: ramp generator V+ aha rye cha rse dlmhar‘ge v_' dISC/JEIJC Figure N2.4: How to use a cap to generate a triangle waveform: ramp up, ramp down But the ramp waveform is relatively rare, because current sources are relatively rare. Much
more common is the next case. A harder case but more common: constant voltage source in series with a resistor 1"IDV 1k . small: 8‘!" 5y across R: 5‘4 time.
at [by across 3: zanA W I  Iona"? '
(75"? ' W = “V/m) Figure N25: The more usual case: cap charged anddischarged from a voltage source, through a series resistor Here, the voltage on the cap approaches the applied voltage—but at a rate that diminishes
toward zero as Vca approaches its destination. It starts out bravely, moving fast toward its
Vin (charging at 16 mA, in the example above, thus at lOV/ms); but as it gets nearer to its
goal,'it' loses its nerve. By the time it is 1 volt away, it has slowed to 1/10 its starting rate. (The cap behaves a lot like the hare in Xeno’s paradox: remember him? Xeno teased his
fellowAthenians by asking a question something like this: ‘If a hare keeps going halfway to
the wall, then again halfway to the wall, does he ever'get there?’ (Xeno really had a hare
chase a tortoise; but the electronic analog to the tortoise escapes us, so we’ll simplify his
problem.) Hares do bump their noses; capacitors don’t: Vcap never does reach VapPhed, in an ,
RC circuit. But it will come as close as you want.) ' N2 — 4 Class 2: Capacitors & RC Circuits 35 Here’s a fuller account: 1. 0
99% 0.75 ‘0 1 2 3 '1 5
+I'ma (wills 47f +nbe—cons7‘amls; xc)
Fimlre N2.6: RC charge. discharge curves Don’t try to memorize these numbers, except two: 9 in one RC (called “one timeconstant”) 63% of the way
.4 in ﬁve RCs, 99% of the way If you need an exaCt solution to such a timing problem: Vcap = Vapplied _ (t/RQ)
In case you can’t see at a glance what this equation is trying to tell you, look at
> (z/RC)
e by itself: 9 when t= RC, this expression is 1/e, or 0.37.
6 when 't = very large (» RC), this expression is tiny, and Vmp == Vapphed A tip to help you calculate time—constants:
I M9 and 11F give timeconstant in seconds
k9 and uF give time—constant in milliseconds In the case above, RC is the product of 1k and lqu'l ms. Integrators and Differentiators
I 14.713 n11. ,1 —_L
K V C out
out infejr‘afar ,? diff’eren'h'ai'or? Figure N2.7: Can we exploit cap’sl = C dZ/dt to make differentiator &. integrator?
The very useful formula, I = CdV/dt will let us ﬁgure out when these two circuits perform
pretty well as differentiator and integrator, respectively. 36 Class 2: Capacitors & RC Circuits N2 5 Let’s, ﬁrst, consider this simpler circuit: Ill:
“"1?
. c
I Figure N2.8: Useless “differentiator”? The current that ﬂows in the cap is proportional to dVin/dt: the circuit differentiates the input
signal. But the circuit is pretty evidently useless. It gives us no way to measure that
current. If we could devise a way to measure the current, we would have a differentiator. Here’s our earlier proposal, again. Does it work? “"1 “avg?
/ C .2
% \Vaul‘:
4t 2 \ ﬁtth — diﬁbrentiafor‘ > Figure N23: Differentiator'? —again ‘
Answer: Yes and No: Yes, to the extent that Vcap = Vin (and thus chap/dt = dVin/dt), because
the circuit responds to dv/dt across the cap, whereas what interests us is de/dt——that is,‘
relative to ground. So, the circuit errs to the extent that the output moves away from ground; but of course it
must move away from ground to give us an output. This differentiator is compromised. So
is the RC integrator, it turns out. When we meet operational ampliﬁers, we will manage to
make nearly—ideal integrators, and pretty good differentiators. The text puts this point thisway: Text sec. 1.14 for the differentiator: n
“. . .choose R and C small enough so that dV/dt, « dVin/dt. . .».”
Text sec. 1.15 for the integrator: '
“. . .[make sure that] Vout<<Vin. . .mRC » 1.” We can put this simply—perhaps crudely: assume a sine wave input. Then, the RC differentiator (and integrator, too) works pretty well if it is
murdering the signal (that is, attenuates it severely), so that Vout (and dVom)
is tiny: hardly moves away from ground.  It follows, along the way, that differentiator and integrator will impose a 90° phase shift on
a sinusoidal input. This result, obvious here, should help you anticipate .how RC circuits
viewed as “ﬁlters” (below) will impose phase shifts. N2 — 6 ‘ Class 2: Capacitors & RC Circuits 37 Integrator ASSUme Vi), is Car/stint ...
Mn L I Lot constarrt, +9 #15 exfeni: Kwé moves
R .
1M Shea/J [Se Conséahz‘.
Vaut if
C I Fui‘ 1': if ,7
L'm‘ejrafar ?
Figure N2.10: Integrator?—again
One can make a similar argument to explain the limitations of the RC integrator. To keep
things simple, imagine that you apply a step input; ask what waveform out you would like
to see out, and what, therefore, you would like the current to do.  RC Filters These are the most important application of capacitors. These circuits are just voltage
dividers, essentially like the resistive dividers you have met already. The resistive dividers
treated DC and timevarying signals alike. To some of you that seemed obvious and
inevitable (and maybe‘you felt insulted by the exercise at the endof Lab 1 that asked you to
conﬁrm that AC was like DC to the divider). It happens because resistors can’t remember
what happened even an instant ago. *They’re little existentialists, living in the present. (We’re talking about ideal R’s, of course.) The impedance or reactance of a cap
' A cap’s impedance varies with frequency. (“Impedance” is the generalized form of what
we called “resistance” for “resistors;” “reactance” is the term reserved for capacitors and
inductors (the latter usually are coils of wire, often wound around an iron core)). Compare Text sec. 1.12 , It’s obvious that a cap cannot conduct a DC current: just recall what the cap’s insides
look like: an insulator separating two plates. That takes care of the cap’s “impedance” at
DC: clearly it’s inﬁnite (or huge, anyway).  _ It is not obvious that a rapidlyvarying voltage can pass “through” a capacitor, but that
does happen. The Text explains this difﬁcult notion at sec. 1.12, speaking of the current
that passes through the cap. Here’s .a second attempt to explain how a voltage signal passes
through a cap, in the high—pass conﬁguration. If you’re already happy with the result, Skip
this paragraph. . . ‘ ' v When we say the AC signal passes through, all we mean is that a wiggle on the left
causes a wiggle of similar size. on the right: ' (oily/E; Iii... .z Lava/e out
”L —l "1
\Some cumn‘ﬁ flows)
but mi [0717 emu/9},
'7 74’" Vcap 1'0 CAMje
aP/smct'a/i/y Figure N2.11: How a cap “passes” a signal The wiggle makes it “across” the cap so long as there isn’t time for the voltage on the cap to
change much before the wiggle has ended—before the voltage heads in the other direction. In other words, quick wiggles pass; slow wiggles don’t. 38 ' ‘ Class 2 Capacitors & RC Circuits ‘ N2 — 7 We can stop worrying about our intuition and state the expression for the cap’s reactance: " XC = —j/ch = 4/2an And once we have an expression for the impedance of the cap—an expression that shows
it varying continuously with frequency—we can see how capacitors will perform in voltage
dividers. RC Voltage dividers
Text sec. 1.18 You know how a resistive divider works on a sine. How would you expect a divider
made of capacitors to treat a‘timevarying signal? dine in sine in
)2, I C,
24.43 vane
C
‘ Ra I 2 t Figure N212: Two dividers that deliver ‘1/2 of vin If this case worries you, good: you’re probably worrying about phase shifts. Turns out they
cause no trouble here: output is in phase with input. (If you can handle the complex
notation, write XC= —j / CDC, and you’ll see the j’s wash out.) But what happens in the combined case, where the divider is made up of both R and This turns out to be an extremely important case.
Text sec. 1.19 . ' This problem is harder, but still ﬁts the voltage—divider model. Let’s generalize that
model a bit: “m jenemh'zed ’ voltage: divv’Jer
Figure N2.13: Generalized voltage divider, and voltage dividers made up of R paired with C The behavior of these voltage dividers—which we call ﬁlters when we speak of them in
frequency terms, because each favors either high or low frequencies— is easy to describe: 1. See what the ﬁlter does at the two frequency extremes. (This looking at extremes
is a useful trick; you will soon use it again to ﬁnd the ﬁlters’ worstcase Zin and Zout') . ‘ ’U" W “lea . _> = 1
1775
’U'out
Dams
Ye hu 8
eta/til}: _
Urn ' Figure N214: Establishing the endpoints of the ﬁlter’s frequency response curve
At f = 0: what fraction out? At f = very high: what fraction out? N2 — 8 Class 2: Capacitors & RC Circuits 39 2. Determine where the output “turns the comer” (corner deﬁned arbitrarilyl) as the
frequency‘where the output is 3dB less than the input (always called just “the 3 dB
point”; “minus” understood). Knowing the endpoints, which tell us whether the ﬁlter is highpass or low—pass, and
knowing the 3dB point, we can draw the full frequency—response curve: (awfass #(fer , 65767255 2471‘» 153.43 7923mm] ‘ . 2923mm )1 Figure N2.15: RC ﬁlter’s frequency response curve
The ‘S3dB oint,” the fre uency wherethe ﬁlter “turns the corner” is
, P Beware the more elegant formulation that uses 03: t , CD3dB = That is tidy, but is very likely to give you answers off by about a factor of 6, since you will
be measuring period and its inverse in the lab: frequency in hertz (or “cyclespersecond,”
as it used to be called), not in radians. '
_____________—_.___——————————————————————————'—— ,
Two asides: 
Caution!
Do not confuse these frequency—domain pictures with the earlier RC step—response picture,
(which speaks in the timedomain). V , time ﬁle
® V ,' frEZJJCVICJ , Figure N216: DeceptiVe similarity between shapes of time— and frequency— plots of RC circuits
Not only do the curves look vaguely similar. _ To make things worse, details here seem _ tailor—made to deceive you: ' 9 Step response: in the time RC (timeconstant), Vcap moves to about 0.6 of the
applied step voltage (this is 1 — l/e). .
0 Frequency domain: at f3'dB, a frequency determined by RC, the ﬁlter’s Mun/Vin is
' about 0.7 (this is 1/42)   Don’t fall into this trap. A note K Log Plots You may wonder why the curves we have drawn, the curve in Fig. 1.59, and those you
see on the scope screen (when you “sweep” the input frequency) .don’t look like the tidier
curves shown in most books that treat frequency response, or like the curves in Chapter 5 of 1. Well, not quite arbitrarily: a signal reduced by 3dB delivers half its original power. 40 ' Class 2: Capacitors & RC Circuits N 2 — 9 the Text. Our curves trickle off toward zero, in the low—pass conﬁguration, whereas these
other curves seem to fall smoothly and promptly to zero. This is an effect of the logarithmic
compression of the axes on the usual graph. Our plots are linear; the usual plot (“Bode
plot”) is log—log: m 1. o 2.521}
717'? i 0 ; “ENC
fmzafjcf; I j ([3 sax/e) Figure N2.17: Linear versus loglog frequency—response plots contrasted Input and output impedance of an RC Circuit If ﬁlter A is to drive ﬁlter B—or anything else, in fact—it must conform to our 10X rule
of thumb, which we discussed last time, when we were considering only resistive circuits.
The samereasons prevail, but here they are more urgent: if we don’t follow'this rule, not
only will signals get attenuated; frequency response also is likely to be altered. But to enforce our rule of thumb, we need to know Zin and Zout for the ﬁlters. At ﬁrst glance, the problem looks nasty. What is Zout for the low—pass ﬁlter, for example? A novice
would give you an answer that’s much more complicatedthan necessary. He might say, Zout = XC ParauelR = "j/wC‘R / (“j/03C + R)
Yow! And then this expression doesn’t really give an answer: it tells us that the answer is
frequencydependent.  We cheerfully sidestep this hard work, by considering only worst case values. We ask,
‘How bad can things get? ' We ask, ‘How bad can Zin get?’ And that means, ‘How low can it get?’
We ask, ‘How bad can Zout get?’ And that means, ‘How high can it get?’ This trick delivers a stunningly—easy answer: the answer is always just R! Here’s the
argument for a lowpass, for example: Zh=?\> R I_JW\/_IC .R, C(Zout=?
l l ‘ R I R (Zuni: ZR
l ‘ (open)
I
L f’ _ i '7 ﬂint 2:0 ' '
worst Zin: cap looks like a short Zin = R worst Zout: cap doesn’t help at all; we look through to
(this happens at highest frequencies) the source, and see only R: Zout = R (this happens at ' lowest frequencies) Figure N2.18: Worstcase Zin and Z” for RC ﬁlter reduces to just R Now you can string together RC circuits just as you could suing together voltage dividers,
without worrying about interaction among them. N2 — 10 Class 2: Capacitors & RC Circuits 41 Phase Shift You already lcnow roughly what to expect: the differentiator and integrator showed you
phase shifts of 90°, and did this when they were severely attenuating a sinewave. You need ‘
to beware the misconception that because a circuit has a cap in it, you should expect to see a
90° shift (or even just noticeable shift). That is not so. You need an intuitive sense of when
phase shifting occurs, and of roughly its magnitude. 'You rarely will need to calculate the
amount of shift. Here is a start: .a rough account of phase shift in RC circuits: If the amplitude out is close to amplitude in, you will see little or no phase
shift. If the output is much attenuated, you will see considerable shift (90° is maximum) And here are curves saying the same thing: Text sec. 1.20,
ﬁg. 1.60, p. 38 0.001 I
amfads mfg}; fads W343 100F315 Figure NZJB: Attenuation and phase shift (loglog plot)
Why does this happen? Here’s an attempt to rationalize the result: 0 I voltages in R and C are 90° out of phase, as you know.
0 the sum of the voltages across R and C must equal, at every instant, Vin.
’ 0 as frequency changes, R and C share the total Vin differently, and this alters the phase of Vout relative to Vin: » Consider a lowpass, for example: if a lot of the total voltage, Vin, appears across the cap,
then the phase of the input voltage (which appears across the RQ series combination) will be
close to the phase of the output voltage, which is taken across the cap alone. In other words,
R plays a small part: Vout is about the same as Vin, in both amplitude and phase. Have we
merely restated our earlier proposition? It almost seems so. 42 ' Class 2: Capacitors & RC Circuits , N2 — 11 But let’s try a drawing: l’iz/\/\,/ IM
%W M 25/0; Haj I * P2557}? Figure N220: R and C sharing input voltage differently at two different frequencies
Now let’s try another aid to an intuitive understanding of phase shift: phasors. Phasor Diagrams These diagrams let you compare phase and amplitude of input and output of circuits that
shift phases (circuits including C’s and L’s). They make the performance graphic, and
allow you to get approximate results by use of geometry rather than by explicit
manipulation of complex quantities. The diagram uses aXes that represent resistorlike (“real”) impedances on the horizontal
axis, and capacitor or inductorlike impedances (“imaginary”—'but don’t let that strange
’name scare you; for our purposes it only means that voltages across such elements are 90°
out of phase with voltages across the resistors). This plot is known by the extrafrightening
name, “complex plane” (with nasty overtones, to the untrained ear, of ‘too—complicated
for—you plane’ l). But don’t lose heart. It’ s all very easy to understand and use. Even better,
you don’t need to understand phasors, if you don’t want to. We use them rarely in the
course, and always could use direct manipulation of the complex quantities instead. 'Phasors
are meant to make you feel better. If they don’t, forget them. 15k "imagine?" axis: madame/or
v ml 33¢ amass C ourL  OP "r23 ("37:15. res;s‘1‘ancg_ or
chlﬁsk vvoh‘age across a resistance —'i Kc = 45sz
anyway)
15k ;
r Cmimed Impedance (Series; a; voHaje urns: R+C Figure N231: Phasor diagram: “complex plane;" showing an RC at £3“ The diagram above shows an RC ﬁlter at its 3dB point, where, as you can see, the
magnitude of the impedance of C is‘ the same as that of R. The arrows, or vectors, show
phase as well as amplitude (notice that this is the amplitude of the waveform: the peak
value, not a voltage varying with time); they point at right angles so as to say that the
voltages in R and C are 90° out of phase. “Voltages?,” you may be protesting, “but you said these arrows represent impedances.”
True. But in a series circuit the voltages are proportional to the impedances, so this use of
the ﬁgure is fair. ' N2 — 12 Class 2: Capacitors & RC Circuits 43 The total impedance that R and C present to the signal source is not 2R, but is the vector
sum: it’s the length of the hypotenuse, RN/Z. And from this diagram we now can read two
familiar truths about how an RC ﬁlter behaves at its 3dB point: 0 the amplitude of the output is down 3dB: down to 1N2: the length of either the R or the C vector, relative to the hypotenuse.
o the output is shifted 45° relative to the input: R or C vectors form an angle of 45° with the hypotenuse, which represents the phase of the input voltage. So far, we’re only restating what you know. But to get someadditional information out ot
the diagram, try doubling the input ﬁequency several times in succession, and watch what happens:
each time, the length of the XC vector is cut to half what it was. First doubling of frequency: X: = half w/taf I} was . R/Z Figure N222: RC after a doubling of frequency, relative to the previous diagram The ﬁrst doubling also affects the length of the hypotenuse substantially, too, however; so
the amplitude relative to input is not out quite so much as 50% (6dB). You can see that the
output is a good deal more attenuated, however, and also that phase shift has increased a good deal.
Second doubling of frequency Figure N223: RC after a doubling of frequency, relative to the previous diagram This time, the length of the hypotenuse is changed less, so the output shrinks nearly as the
XC vector shrinks: nearly 50%. Here, we are getting close to the —6dB/octave slope of the
ﬁlter’s rolloff curve. Meanwhile, the phase shift between output and input is increasing,
too—approaching the limit of 90°. We’ve been assuming a lowpass. If you switch assumptions, and 'ask what these
diagrams show happening to the output of a highpass, you ﬁnd all the information is there
for you to extract. No surprise, there; but perhaps satisfying to notice. 44 Class 2; Capacitors &RC Circuits N2— 13 LC circuit on phasor diagram
Finally, let’s look at an LC trap circuit on a phasor diagram. {60> 14E : XL domrnaﬁs 12 ' R (Ibducfor like)
35. WT Mint “in wut
C V
: m
L. 2 0F '\
Comblncd _ resonance
_ LC
Series LC "traf" . x w < wra . Xc domina'its (ca/pacifor‘ Like)
Figure N224: LC trap circuit. and its phasor diagram
This is less familiar, but pleasing because it reveals the curious fact—which you will see in
Lab ‘3 when you watch a similar (parallel) LC circuit—that the LC combination looks
sometimes like L, sometimes C, showing its characteristic phase shift—and at resonance,
shows no phase shift at all. We’ll talk about LC’s next time; but for the moment, see if you can enjoy how concisely this phasor diagram describes this behavior of the circuit (actually
a trio of diagrams appears here, representing what happens at three sample frequencies). To check that these LC diagrams make sense, you may want to take'a look at what the old
voltagedivider equation tells you ought to happen: l?
127]} Want A}
ZoF com brned
LC Figure N225: LC trap: just another voltage divider Here’s the expression for the output voltage as a fraction of input: I Vout/ Vin = Zcombinaliori / (Zcombination + R ) But ‘
Zcombination = (0C + mL' And at some frequency—where the magnitudes of the expressions on the right side of that last equation are equal—the sum is zero, because of the opposite signs. Away from this magic frequency (the “resonant frequency”), either cap or inductor dominates. Can you see all this on the phasor diagram? Better Filters Having looked hard at RC ﬁlters, maybe we should remind of the point that the last
exercise in Lab 2 means to make: RC’s make extremely useful ﬁlters, but if you need a
better ﬁlter, you can make one, either with an LC combination, as in that circuit, or with
operational ampliﬁers cleverly mimicking such an LC circuit (this topic is treated in Chapter
5; we will not build such a circuit), or with a clever circuit called a ‘switchedcapacitor’
ﬁlter, a circuit that you will get a chance to try, in Lab 11, and again in Lab 21. Here is a _ sketch (based on a scope photo) comparing the output of an ordinary RC lowpass against a
5—pole Butterworth low—pass, like the one you will build at the end of Lab 2. N2 — 14 Class 2: Capacitors & RC Circuits 45 ‘5 ~ Tab" LC BvHerwor‘ﬁI low/nus RC [0925: a 5
\° i’ 5 o
~’5'
~§ Q 0 IDOkHz frezuency ( linear same/s)
Figure N2.26: Simple RC lowpass contrasted with 5pole Butterworth low—pass
(“S—pole” is a fancy way to say that it something like, ‘It rolls off the way 5 simple RC’s in
series would roll off’—~it’s ﬁve times as steep as the plain RC. But this nice ﬁlter works a
whole let better than an actual string of 5 RC’s.) Not only is the rolloff of the Butterworth much more abrupt than the simple RC’s, but
also the “passband” looks much ﬂatter: the fancy ﬁlter does a better job of passing. The
poor old RC looks sickly next to the Butterworth, doesn’t it? , Nevertheless, we will use RC’s nearly always. Nearly always, they are good enough. It
would not be in the spirit of this course to pine after amore beautiful transfer function. We
want circuits that work, and in most applications the plain old RC passes that test. _____________________.______..————————————————— i 46 Chapter 1: Worked Examples: RC Circuits Two worked exercises: 1. ﬁlter to keep “signal” and reject “noise”
2. bandpass ﬁlter 1. Filter to keep “signal” and reject “noise’ Problem: Filterrto remove fuzz: Suppose you are faced with a signal that looks like this: a signal of
moderate frequency, polluted with some fuzz ' 1. 2. 3. 9—1m: ————> Figure X2.1: Signal With Fuzz Added Draw a skeleton circuit (no parts values, yet) that will keep most
of the good signal, clearing away the fuzz. Now choose some values: If the load has value 100k, choose R for your circuit. a.
b. Choose fgdB, explaining your choice brieﬂy.
0. Choose C to achieve the f3dB that you chose. d. By about how much does your ﬁlter attenuate the noise
“fuzz”? What is the Circuit’s input impedance— a. at very low frequencies?
b. at very high frequencies?
C. at f3dB? What happens to the circuit output if the load has resistance 10k
rather than 100k? X2 — 2 Chapter 1: Worked Examples: RC Circuits 47 A Solution:
1 . Skeleton Circuit
You need to decide whether you want a lowpass or highpass, since the 'signal and noise are distinguishable by their frequencies (and are far enough apart so that you can hope to get
one without the other, using the simple ﬁlters we have just learned about). Since we have
called the lower frequency “good” or “signal,” we need a lowpass: I Figure X22: Skeleton: just alow—pass ﬁlter 2. Choose R, given the load > This dependence of R upon load follows from the observation that R of an RC ﬁlter
deﬁnes the worstcase input and output impedance of the ﬁlter (see Class 2 notes). We want
that output impedance low relative to the load’s impedance; our rule of thumb says that
‘low’ means low by a factor of 10. So, we want R S Rload/IO. In this case, that means R should be S 10k. Let’s use 10k. 3. Choose Edi; This is the only part of the problem that is not entirely mechanical. 'We know we want to
pass the low and attenuate the high, but does that mean put f3dB halfway between good and
bad? Does it mean put it close to good? ...Close to bad? Should both good and bad be on a steeplyfalling slope of the ﬁlter’sresponse curve? 0.1 ,
.IKH: M kllz {saw ,  . {BAD
, Figure X23: Where should we put fad}; 7 Some possibilities
Assuming that our goal is to achieve a large ratio of good to bad signal, then we should not
put f3dB close to the noise: if we did we would not do a good job of attenuating the bad.
Halfway between is only a little better.‘ Close to signal is the best idea: we will then
attenuate the bad as much as possible while keeping the good, almost untouched. An alert person might notice that the greatest relative preference for geod over bad comes
when both are on the steepest part of the curve showing frequency response: in other words, V put f3dB so low that both good and bad are attenuated. This is a clever answer—but wrong,
_ in most settings. The trouble with that answer is that it assumes that the signal is a single frequency.
Ordinarily the signal includes a range of frequencies, and it would be very bad to choose fgdB somewhere within that range: the ﬁlter would distort signals. So, let’s put f3dB at 2fsigml: around ZkHz. This gives us 89% of the original signal
amplitude (as you can confirm if you like with a phasor diagram or direct calculation). At 48 ' Chapter 1: Worked Examples: RC Circuits X2 —' 3 the same time we should be able to attenuate the l6klIz noise a good deal (we’ll see in a
moment how much). ' 4.. .Choose C to achieve the 1343 that you want This is entirely mechanical: use the formula for the 3dB point: fgdB —= 1/(21tRC) ==> c = 1/(21tf3dBR) z 1/(62~103~10~103) = 1/(120406) z 0.00810'5F
We might as well use. a 0.01 uF cap (“cap” E capacitor). It will put our f3dB about 25%
low—1.6Khz;'but our choice was a rough estimate anyway. 5. By about how muchdoes your ﬁlter attenuate the noise ( “ uzz” )? The quick way to get this answer is to count octaves or decades between f3dB and the
noise. f3dB is 2 kHz; the fuzz is around 16kHz: 8'f3dB. Count octaves: we could also say that the frequency is doubled three times (= 23) between
'f3dB and the noise frequency. Roughly, that means that the fuzz amplitude is cut in half the
same number of times: down to 1/(23): 1/8. This is only an approximate answer because a) near f3d3 the curve has not yet reached its
terminal steepness of —6dB/octave; b) on the other hand, even at f3dB, some attenuation
occurs. But let’s take our rough answer. (It happens that our rough answer is better than it
deservesto be: we called Vault/Vin 0.125; the'more exact answer is 0.124.) '6. What happens to the circuit output ifthe load has resistanceﬂc rather than I 00k?
Here’s a picture of such loading. r.— ‘ 70K #— Zoyr : worst C ase: I LOAA.
.___/\M__~— ..   10k _ J
l
L l =70k
0.04/41: I EMMA I _ _. 1 _ _ L. _. .  > Figure XZA: Overloaded ﬁlter
'If you have gotten used to Thevenin models, then you can see how to make this circuit look more familiar:
5K 9—“
effect/‘11: R
@ cut in [Iva/f
I 0.01 IMF I Figure X25: Loaded circuit, redrawn The amplitude is down; but, worse, f3dB has changed: it has doubled. You will ﬁnd a plot
showing this effect at the start of the class notes for next time: Class 3. X2 — 4 Chapter 1: Worked Examples: RC Circuits 49 7. What is the Circuit’s input impedance— 1. at very low frequencies? ‘
Answer: very large: the cap shows a high impedance; the signal source sees only the load—which is assumed very high impedance (high enough so we can neglect
it as we think about the ﬁlter’s performance) ‘ l 2. at very high frequencies?
; Answer: R: The cap impedance falls toward zero—but R puts a lower limit on the input impedance. 3. at ; This is easy if you are willing to use phasorsga nuisance to calculate, otherwise. If you recall that the magnitude of XC = R at f3dB, and if you accept the notion that the voltages
across R and C are 90° out of phase, so that they can be drawn at right angles to each other
on a phasor diagram, .then you get the phasor diagram you saw in the class notes (ﬁg. : N221):
[aha sar t/z‘ajram .
” 7c5.115 ‘ R . _ ZM/J: V/Xc/r'I‘R
I ZIN=VZR Figure X2.6: Phasor diagram showing an RC ﬁlter at its 3dB point
—.then you can use a geometric argument to show that the hypotenuse—proportional to
Zin—is RVZ. 2. Bandpass T ext exercise AE6
(Chapter 1 ) Problem: Bandpass ﬁlter I
Design a bandpass ﬁlter to pass signals between about 1.6 kHz and 8kI—lz (you may use these as 3dB frequencies)..
Assume that the next stage, which your bandpass ﬁlter is to drive, has an input impedance of l M ohms. 50 Chapter 1: Worked Examples: RC Circuits X2 — 5 Ilde lg“ {Hymn/(‘7
Figure X2.7: Bandpass frequency response Once you recognize that to get this frequency response from the ﬁlter you need to put high
pass and lowpass in series, the task is mechanical. You can put the two ﬁlters in either
order, Now we need to choose R values, because these will determine worst—case
impedances for the two ﬁlter stages. The later ﬁlter must show Zout low relative to the load,
which is 1M9; the earlier ﬁlter must show Zout low relative to Zm of the second ﬁlter stage. So, let the secondstage R = 100k; the ﬁrststage R = 10k: Choosing C’s v Here the only hard part is to get the ﬁlter’s right: it’s hard to say to oneself, ‘The high
pass ﬁlter has the lower f3dB;’ but that is correct. Here are the calculations: notice that we
try to keep things in engineering notation—writing ‘100103’ rather than ‘104.’ This form
looks clumsy, but rewards you by delivering answers in standard units. It also helps you
scan for nonsense in your formulation of the problem: it is easier to see that ‘10°103’ is a
good translation for"lOk’ than it is to see that, say, ‘105’ is not a good translation. Q c/mase Z} 7“!) keg/5 20W <4Z/u—luexr—STME _‘ __ —“ / (~_ I ,
yaw—«va—H Mr»;
' 0.001 , ILA/ant ﬁr. 700K I 72mm : {Mn
Cca'sctt i e £1001 . I : ,.
T  T L ,.
1
TM 1‘:
l .
{MsLOW = 8m“  FMS—HIE” : 75m“
I I
C: bun/01.1mm! I C= 17rl.:’xw§o.1xm‘
l l I —1
~— ~ ——— = .1
1:: 480xm‘ "’ 0."; xIo’ 7 “a l 2.. 0.00 F
2 00¢sz I ’I“ K
Figure X2.8: Calculating C values: a plug for engineering notation 51 A Note on Reading Capacitor Values Why you may need this note
Most students learn pretty fast to read resistor values. They tend to have more trouble ﬁnding, say, a 100 pF capacitor. That’s not their fault. They have trouble, as you will agree when you have ﬁnished
reading this note, because the cap manufacturers don’t want them to be able to read cap
values. (“Cap” is shorthand for “capacitor,” as you probably know.) The cap markings
have been designed by an international committee to be nearly unintelligible. With a few
hints, however, you can learn to read cap markings, despite the manufacturers’ efforts. Here are our hints: ' Big Caps: electrolytics These are easy to read, because there is room to write the value on the cap, including
units. You need only have the common sense to assume that —9— Figure CAP.1: A big cap is labeled intelliginy
means 500 micro farads, not what it would mean if you took the capital M seriously. All of these big caps are polarized, incidentally. That means the capacitor’s innards are not symmetrical, and that you may destroy the cap if you apply the wrong polarity to the
terminals: the terminal marked + must be at least as positive as the other terminal.
(Sometimes, violating this rule will generate gas that makes the cap blow up; more often,
you will ﬁnd the cap internally shorted, after a while. Often, you could get away with violating this rule, at low voltages. 'But don’t try.) Smaller Caps V
As the caps get smaller, the difﬁculty in reading their markings gets steadily worse. Tantalum I
These are the silver colored cylinders. They are polarized: a + mark and a metal nipple
mark the positive end. Their markings may say something like a— Figure CAP}: Tantalum cap ,
That means pretty much whatsitsays,:if you know that the “R” marks the decimal place: it’s a 4.7 uF cap.
The same cap is also marked, a—
Figure CAPS: Tantalum cap: second marking scheme on same part
Here you meet your ﬁrst challenge, but also the ﬁrst appearance of an orderly scheme for
labeling caps, a scheme that would be helpful if it were used more widely. . The challenge is to resist the plausible assumption that “k” means “kilo.” It does not; it is
not a unit marking, but a tolerance notation (it means i 10%). (Wasn’t that nasty of the
labelers to choose “K?” Guess what’s another favorite letter for tolerance. That’s right: M. Pretty mean!) 52 A Note on Reading Capacitor Values CAP — 2 The orderly labeling here mimics the resistor codes: 475 means
47 x ten to the ﬁfth. What units? 105 what? 105 of something small. You will meet this question repeatedly, and you must
resolve it by relying on a few observations: ’ ’ 1. The only units commonly used in this country are  microfarads: 10'6 Farad '
0 picofarads: 1012 Farad (You shOuld, therefore, avoid using “mF” and “nF,”yourself.) A Farad is a huge unit. The biggest cap you 'will use in this course is 500 uF. That
cap is physically large. (We do keep 3. IF cap around, but only for our freak show.)
So, if you ﬁnd a little cap labeled “680,” you know it’s 680 pF. 2. A picofarad is a tiny unit. You will not see a cap as small as 1 pF in this course.
So, if you ﬁnd a cap claiming that it is a fraction of some unstated
unit—say,“.01”——the unit is u‘F’s: “.01” means 0.01 'lLF. 3. Beware the wrong assumption that a picofarad is only a bit smaller than a
microfarad. A pF is not 109 F (103 uF); instead, it is 10421:: a million times 
smaller than a microfarad. So, we conclude, this cap labeled “475” must be 4.7><106 picofarads. That, you will
recognize, is a roundabout way to say ' 4.7 ><10'6 F .
We knew that was the answer, before we started this 'last decoding effort. This way of
labeling is indeed roundabout, but at least it is unambiguous. It would be nice to see it used more widely. You will see another example of this exponential labeling in the case of the
CKOS ceramics, below. \ ' Mylar
These are yellow cylinders, pretty clearly marked. .01M is just 0.01 “F, of course; and .lMFD is not a tenth of a megafarad. These caps are not polarized; the black band marks
the outer end of the foil winding. We don’t worry about that ﬁne point. Orient them at random in your circuits.
—o)' Figure CAPA: Mylar capacitor
Because they are long coils of metal foil (separated by a thing dielectric—the
“mylar” that gives them their name), mylar caps must betray their coillike construction at
very high frequencies: that is, they begin to fail as capacitors, behaving instead like
inductors, blocking the very high frequencies they ought to pass. Ceramics (below) do
better in this respect, though they are poor in other characteristics. CAP — 3 A Note on Reading Capacitor Values 5 3 Ceramic These are little orange pancakes. Because of this shape (in contrast to the coil format
hidden within the tubular shape of mylars) they act like capacitors even at high frequencies.
The trick, in reading these, is to reject the markings that can’t be units: Disc Figure CARS: Disc capacitor markings CKOS ZSU: Not a unit marking: cap type .02M, 560M That’s it: the M is a
tolerance marking, as you know (i 20%);
not a unit Common sense tells you units:
“.02?” microfarads. “560?” picofarads. 1kV Not a unit marking. Instead,
this means—as you would guess—that
the cap can stand 1000 volts. These are little boxes, with their leads 0.2“ apart. They are handy, therefore, for insertion into a printed circuit. 101k: This is the neat resistorlike
‘ marking. This one is 100 pF. Figure CAP.6: CKOS capacitor markings Tolerance Codes Just to be thorough—and because this information is hard to come 'by—let’s list all the
tdlerance codes. These apply to both capacitors and resistors; the tight tolerances are
relevant only to resistors; the strangelyasymmetric tolerance is used only for capacitors. Tolerance Code
Z——. —— N>mouwmwwg Z  Meanin +80%, —20% (for big ﬁlter capacitors, where you are assumed 
to have asymmetric worries: too small a cap
allows excessive “ripple;” more on this in Lab
3 and‘Notes 3) i 20% v i 10% i 5% i 2% i 1% i 0.5% i 0.25% i 0.1% i 0.05%
i 0.025 (precision resistors; context will show the asymmetric cap tolerance “Z” makes no sense here)
i 0.02% Figure CAP.7: Tolerance codes _______________——.___.————————— ...
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This note was uploaded on 11/15/2011 for the course PHYS 2300 taught by Professor Staff during the Summer '09 term at Auburn University.
 Summer '09
 Staff
 Physics, Electronics, RC Circuits

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