May 1961 Popular ElectronicsTable of Contents
People old and young enjoy waxing nostalgic about and learning some of the history of early electronics. Popular Electronics was published from October 1954 through April 1985. All copyrights are hereby acknowledged. See all articles from Popular Electronics.
Fundamentals of resonant tank circuits has not changed since they were first investigated more than a century ago. This "After Class" tutorial that ran in the May 1961 edition of Popular Electronics is typical of the series where the author speaks as though he was giving an impromptu lesson to a gathering of students after the scheduled classroom period was over or, in this instance as though he was having a casual discussion with a friend who was perplexed by a particular electronics phenomenon. Figures and equations are often drawn by hand to augment the informal setting rather than being typeset. Here, "Larry" is amazed by the great performance of his Ham radio with its ability to filter out adjacent channel interference. Mentor "Ken" takes the opportunity to explain the mathematics and physics of resonant circuits both to tuning antennas and for filtering unwanted frequencies while passing desired frequencies.
By Saunder Harris
Coil and capacitor combinations lie behind every tuned circuit, and some do a better job than others. Here's the complete story of how they work and why.
Larry was busy listening to the chatter of the 40-meter band on Ken's receiver. An old hand on the air, Ken watched as his young friend delicately turned the bands pre ad dial.
"Smooth-operating gadget, isn't it, Larry?"
"You said it, Ken. Boy, the way this thing separates signals is amazing. Listening to 40 meters on my receiver is like trying to count the noodles while the soup is being stirred. With this one, not only can you count the noodles, but you can pick the particular noodle you want out of the soup at any time."
"You're always thinking about eating." Ken shook his head. "Well, Larry, you can thank the tuned circuits in this baby for separating signals. As a matter of fact, if it weren't for tuned circuits, you and I would be collecting stamps for a hobby instead of guiding electrons through wires. There wouldn't be any radio ... or TV for that matter. Some horrible thought, eh ?"
"Now that you've mentioned it, Ken, I've always wondered how receivers separate one frequency from another - especially two frequencies almost on top of each other." Larry flipped off the receiver and sat back. "Can you make with some explaining on the topic, friend?"
"Since you put it so nicely, I'll be glad to. As usual, we'll start off with some basic facts."
Ken took up paper and pencil as he said, "Tuned circuits in receivers are combinations of inductance, capacitance, and resistance. These three elements are usually arranged in a two-leg parallel circuit, like this." He passed the drawing he had made over to Larry.
Larry studied the drawing for a moment. "So receiver tuned circuits are made up of coils, capacitors, and resistors ?"
"Not exactly, Larry. Actually," Ken explained, "the resistance is not deliberately added. It pops up in the circuit because the wire making up the coil, L, and the connecting leads and solder joints all insert some resistance into the tuned circuit. We try to avoid unintentional resistance by keeping leads short and making good solder connections."
"I'm with you so far, but I still don't see how receiver tuned circuits work. What happens when I turn the tuning knob of a receiver?"
"Let's not get ahead of ourselves, Larry." Ken paused a moment. "Now, one of the things that makes a tuned circuit possible is the fact that both a coil and a capacitor oppose the flow of alternating current through them. This opposition to current flow can be considered as resistance, but in a.c. circuits it's called reactance.
"As you increase the frequency of an alternating current passing through a capacitor, it becomes easier for that current to get through - in other words, the capacitive reactance decreases. For the coil, however, the higher the frequency, the rougher it is for the current to get through - the inductive reactance increases as the frequency rises."
Ken paused again to see if everything he had said so far was understood. At a nod from Larry, he went on.
"The second thing that makes tuned circuits possible is that, unlike pure resistance, both capacitive and inductive reactances have directional properties. Take a look at that parallel-tuned circuit I showed you and imagine an alternating current flowing through it.
"Each element in the circuit will have a current flowing through it, the amount of current depending on the reactance of the circuit component. The thing to keep in mind, though, is that the current through the coil will always be opposite in 'polarity' to the current through the capacitor ... "
At this point, Larry yelled, "Whoa up! I'm beginning to get lost!"
"Relax, the hard part's over now." Ken took a ruler from the workbench and handed it to Larry. "Here, let's see you balance this on your finger."
Larry took it, looking puzzled. "What has balancing a ruler got to do with tuned circuits?" He shrugged, "Okay, so I've got it balanced. What happens now?"
"A tuned circuit is very similar to the situation you have with the ruler balanced on your finger. Can you imagine how you might get a similar electrical balance in this parallel-tuned circuit?"
Larry frowned; then a big grin suddenly appeared on his face. "Wait a minute! Suppose I put a voltage of a certain frequency across the circuit. Let's say that at that frequency the capacitive reactance is greater than the inductive reactance ... "
Ken nodded encouragingly.
"As I raise the frequency, the capacitive reactance gets smaller and the inductive reactance gets larger ... "
"Right, Larry! Go on."
"If I keep raising the frequency, I'll eventually reach a point where the capacitive reactance and the inductive reactance are equal. This part is easy, but what happens inside the parallel-tuned circuit when we have this electrical balance?"
"The frequency at which the capacitive and inductive reactances are equal is called the resonant frequency. To see what happens inside the parallel-tuned circuit at resonance, look at this diagram, Larry."
"Do you recall Kirchhoff's law about currents that enter and leave any point in a circuit adding up to zero? Well, at resonance, since the inductive and capacitive reactances are equal, the currents in L and C are also equal but opposite in phase; so they add up to zero. Now, if IL and IC add up to zero at resonance, what is the value for Iant?"
Larry began to think aloud. "Let's see ... the three currents have to add up to zero. That means IC plus IL plus Iant equals zero. But at resonance, IC and IL add up to zero, so that leaves only v to equal zero ... hey, the current from the antenna is zero!"
"Right you are, Larry." Ken sounded pleased. "But let's put that mental solution of yours down on paper to be sure we have it cold."
"Say, Ken," Larry asked, "if the antenna can't pass any current through the parallel-tuned circuit at the resonant frequency, then the tuned circuit behaves exactly like an open circuit. Is that correct?"
"Sure thing - so far you're batting a thousand. Now let's draw the schematic diagram of a receiver front end, and come to some conclusions." In a moment the sketch was done.
Ken continued with his explanation. "First off, let's see what happens at the resonant frequency. The tuned circuit behaves like a very high impedance or high-value grid resistor at this frequency, and very little of the signal picked up by the antenna passes to ground through the tuned circuit. Instead, the control grid of the vacuum-tube stage connected to the top of the tuned circuit sees nearly all of this signal and amplifies it.
"Other signals picked up by the antenna which are lower than the resonant frequency do not meet with this high impedance. They are bypassed to ground through the coil, L, which offers very little impedance. Hence, the control grid sees no signal developed across the tuned circuit. True, there is some signal, but it is probably smaller than the noise generated in the tube and will not be amplified. Signals higher than the resonant frequency are bypassed to ground because the capacitor, C, offers very little impedance, and again the control grid receives no useful signal."
"Fine, Ken, I think I'm beginning to understand. But I noticed that you made the capacitor in the diagram a variable job ... "
"And with good reason," Ken shot back. "Think a moment. If we use fixed values for Land C, only one frequency will resonate across this circuit. And ... "
Larry didn't let him finish, but broke in, saying, "Oh, I see! If we couldn't vary the C, we could only listen to one frequency; and if no station were transmitting on this frequency, we wouldn't hear anything."
"Right again. So we use a variable capacitor and vary the value of C so we can pick out the frequency at which we want to resonate the tuned circuit. This way, we pick the station we want - not let the station find us."
"I get you," said Larry. "Now where do we go from here?"
Well, now that we've tackled tuned circuits in words, I'd like to show you how they work out in terms of equations for reactances and resonance. That's the best way to see what's going on."
Larry winced, and Ken laughed at the uncomfortable look on his young friend's face. "You might as well get the equations down for figuring resonant frequencies," he said. "They're handy to know, and you'll need them if you take the General Class ham exam. I guarantee they're easy to understand."
Ken did some writing, then pushed the paper over so Larry could read it.
"I'll bet I can figure out how we find the resonant frequency for a tuned circuit from those two equations. This isn't bad after all," Larry admitted.
"Go to it, and good luck," said Ken. "Well, I guess the ƒ in the formulas stands for the frequency, the C for capacitance in farads, and the L for inductance in henrys."
"Okay. And ... ?"
"A few minutes ago you mentioned that at the resonant frequency the capacitive and the inductive reactances are equal. So, if we set each of the reactance formulas equal to each other, and do a little fancy algebra work, we should get one formula for the frequency, ƒ, in terms of L and C."
"Nice going, Larry - that's 100% correct." Ken was really pleased. "I'll save you some brainwork and show you how it works out." He took the scratch paper from Larry and wrote:
"Now I solve for ƒ by simple algebra and come up with an equation worth remembering." Ken wrote down:
"In this equation, Larry, you must remember that the frequency comes out in cycles per second. The capacity must be expressed in farads and the inductance in henrys. You'll get all fouled up if you use the wrong units. Pi (π) is just your old friend from geometry, 3.14."
"Isn't there any formula in micro-farads and microhenrys we can use, Ken? Changing all the units around could make an awful mess."
"I'm glad you asked that, Larry. There sure is. Here, let me write it out for you."
"This formula is real easy to use," said Ken, passing the paper to Larry. "The capacitance units you substitute for Care micromicrofarads (μμƒ.); the inductance units you substitute for L are expressed in microhenrys (μh.). These are the values you'll most likely use in practical work. Your answer then comes out in megacycles."
"It's all clear now," observed Larry, as he finished studying the equations.
"Say, before we call it a night, Ken, would you do me a favor and explain what they mean by the Q of a tuned circuit ?"
"I sure will; Q is an important part of any discussion of tuned circuits and we shouldn't forget to clear up any doubt as to what it means. Do you remember what you said about the sharp tuning of my receiver a while back?"
"Do I!" replied Larry. "It was terrific."
"It was the Q of the circuit that made it that way. But I cheated before, Larry," Ken admitted. "I drew the front end of a receiver showing the tuned circuit without the resistance. Let's draw it again, and patch up our thinking. At the same time, you'll get a clear understanding of exactly what Q is." He began to sketch quickly.
"Before," Ken continued, "we said that at the resonant frequency the currents IC and IL added up to zero. This just ain't so. The resistor, R, causes a phase shift in the coil leg of the tuned circuit. Since this resistance is small, the phase difference between the currents IC and IL is slightly less than 180 degrees, and summing up these two currents will not give us zero. A very small current will be left. Back to friend Kirchhoff ..."
Again Larry interrupted, "I get it!
The sum of the currents entering and leaving anyone point in a circuit must be zero - so since the sum of IC and IL is a very small current, a current of equal size but opposite phase must be supplied to the tuned circuit by the antenna."
"Atta boy, Larry," said Ken beaming.
"Antenna current flows in spite of the fact that the circuit is at resonance. The tuned circuit, instead of being an open circuit, now exhibits some high resistance. This will always be the case since we can never get rid of the resistance in the coil or at soldered connections. But we can keep the resistance down to some low value where it won't bother us."
"Why?" Larry asked.
"The more resistance in the circuit, the less selective the circuit. That's why your receiver has trouble separating close stations and mine doesn't. Mine is more selective.
"We can say the same thing in a different way," Ken pointed out. "The more resistance in a tuned circuit, the lower its Q. The Q of a circuit is a numerical way of expressing the merit of a tuned circuit. Look at these curves. The top one shows a low-Q tuned circuit in operation. You can see how broad the curve is. If you tune the receiver correctly, the station you want to listen to will be right on top of the curve. But note that a nearby station, which you don't want to hear, will have almost the same signal strength - the tuned circuit will not reject it. This shows poor selectivity." Pointing to the top drawing, Ken added, "That's your receiver!"
"I see yours right below it," Larry said. "The curve is more peaked, so the tuning is sharper. Also, the nearby station is almost rejected. In fact, I bet it won't be heard at all."
"You get the point, Larry. So the Q is only a means of expressing the quality of the tuned circuit. To compute it, you divide the inductive reactance by the resistance in the circuit.
"You can see that the less resistance, the higher the Q; and the higher the Q, the more selective the circuit. When you're building a set, you should be careful to keep leads as short as possible, make good solder joints, and do everything possible to keep the resistance down and the Q up."
"I guess that's a lesson I'll remember the next time I heat up the old soldering iron." Larry tried to hide a yawn.
"If that's a hint you've had enough, I can take it, buddy." Ken laughed as he got up. "Let's call it a session. But before you run off, let me remind you to go over what we've talked about. You took such a big bite of theory, you'd better chew on it a while."
Posted April 16, 2014