Audio Measurements Course--Part 14 (March 1967)

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by NORMAN H. CROWHURST

Fig. 14-1. Deductions from stage-by-stage waveform measurement. At (A) the distortion first shown between the 2nd and 3rd stages is due to grid-current loading by the 3rd stage. At (B) a quite similar (but not identical) effect is due to curvature (approaching cut-off) in the 2nd stage.

Fig. 14-2. Some of the peculiarities that may show up in measurements associated with split-load phase inverters (here shown with tube). In each of the pairs of waveforms, center and right, the "Z" represents the location of the measuring instrument (voltmeter, scope, or both), while the waveforms are those at both places while the instrument is so connected.

ALL THE MEASUREMENTS discussed in earlier installments concern complete units of equipment: we have not discussed the making of measurements where you have to get "inside" an item of equipment, for either service or development purposes. Yet both of these uses are important in audio work.

Measurements on the old-fashioned tube amplifiers were relatively simple.

although some erroneous conclusions could be drawn even there from incorrect interpretations of the voltage indications observed, using either a voltmeter or a scope. But the transistor circuits multiply the possibility for such misinterpretation, which is one reason why transistors took so long to find extensive application in audio work.

Voltage Readings, Tubes and FET's

We shall regard tubes and FET's (Field Effect Transistors) as essentially similar, because for measurement purposes they have both the same kind of characteristics. Both are essentially voltage amplifiers, or devices in which the controlling input signal is a voltage rather than a current.


Fig. 14-3. If duplicate identical instrumentation cannot load both outputs of the split-load inverter identically, use a dummy, so the loading is identical while each measurement is made.

Only one measurement (across emitter half of load) is shown here. Reverse places to measure other half.

The kind of mistakes sometimes made are obvious-once you have either made them and found your own mistake, or else had them carefully explained to you. Two examples will illustrate. The first relates to finding out where distortion occurs in a multistage amplifier (Fig. 14-1). Checking waveform at various points through an amplifier shows that flattening first occurs at a certain point.

The logical--obvious, but often erroneous-deduction is that the distortion occurs in the stage between the latest point where no distortion is indicated and the one where it first appears. Quite often it is not in this stage at all, but the one following it is the cause. In tube circuits, grid-current loading will flatten the output of the previous stage, although without this loading it would show no distortion at all at this point.

On the other hand, if the distortion is due to cut-off, rather than saturation (grid saturation) , the reverse situation applies: the distortion will show ...

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Fig. 14-4. Checking a single transistor stage, the audio performance will verify prediction from the load-line construction quite closely.

Fig. 14-5. Now couple tie following stags, and the condition changes, as part ally explained oy a new load line.

Fig. 14-6. Use a linear resistance of approximately the same average value of the following-stage base resistance, to predict effect of loading on the first-stage output.

Fig. 14-7. A simple way to make the substitution in the following stage.

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... following the stage running into cutoff, not before it [(B) in Fig. 14-1].

The other frequent cause of error in simple amplifier measurements concerns phase-inverter balance (Fig. 14-2). Voltmeters and scopes used nowadays have high input impedances, that do not appreciably load the circuits to which they are connected. But they may have a capacitive input, if only due to the shielded input lead, that produces an effect that is not quite negligible.

Several things can happen. First the loading caused at high frequencies may destroy balance at those frequencies, although such loss of balance does not occur until the external load (due to the measuring device) is connected. This may have a greater effect on one half of the push-pull than the other, due to asymmetrical internal impedance, and thus cause an indicated lack of balance that does not actually happen until the voltmeter or scope is connected.

Also the instrument loading may unbalance the circuit to a point where the "other half" of the load reaches saturation and reflects a change of waveform into the measured half that does not otherwise occur. The best way to guard against these misleading indications is either to use identical instrumentation to measure both sides of the inverter output simultaneously, or to make up a simulated input circuit, so each can be measured with the "other side" similarly loaded (Fig. 14-3). Current Amplification, Transistors Those things, and more like them, are "old hat" to most readers. Now we turn to the problems that only begin to show when we start using circuits primarily built around current amplification, with transistors. If you just dive in and start making waveform and voltage measurements, the results may be very puzzling at first.

To make the picture clearer, we'll assume you are starting from scratch, because it's easier to understand that way.

Suppose you are checking out a simple amplification stage (Fig. 14-4). Bias is chosen to ensure maximum available swing in each direction, so the collector voltage is approximately half the supply voltage, and an input resistance may be used to simulate the driving impedance of a preceding stage. The previous stage, we'll presume, behaves according to prediction--it probably will.

Now we couple the next stage (Fig. 14-5) . Three things may now happen: first, the voltage swing disappears, because the following stage loads the collector circuit right down; second, what voltage is left is quite distorted, mainly because the input resistance of the following stage is quite non-linear (even when its amplification is linear); and third, it may be found that the first stage is running into overload at an input level considerably lower than it could handle successfully before the second stage was coupled.

To check, approximately, the true performance of the first stage when loaded by the second, either the current delivered to the second stage must be measured, which is never as easy to do as measuring voltage and its waveform; or the voltage can he measured across a linear resistance of approximately the same value as the average input resistance of the following stage (Fig. 14-6) . If plug-in transistors are used, inserting of such a substitute resistor value for measurement can readily be achieved by removing the transistor and pushing a pair of wires (of the same gauge) cut from new transistors, into the base and emitter sockets. To these wires an appropriate low-value resistor is soldered, across which the waveform can be measured (Fig. 14-7). This measurement will separate the three effects for ready analysis. Both voltage swing and current swing can now be determined at this point. Voltage swing is measured directly, but means little, because the linear resistance across which it is measured is in reality a substitute for a non-linear resistance which will change both the value and magnitude of the voltage waveform. But the waveform across the substitute resistor will be reliable indication of current waveform, and its magnitude can be calculated from the resistance value used.

If the loading down by this low input resistance representing the following stage asymmetrically increases current swing of the stage being measured (Fig. 14-5), this will allow excessive level and/or distorted waveform to occur at this point, which can be observed across this substitute resistor. Where this occurs, the original current swing (without the loading) can be restored by changing the collector resistor R so collector voltage is much lower, but the same current swing is available (Fig. 14-8). Usually the collector resistor needs to he almost double, but the bias remains almost the same (in current), However, an improved way of obtaining it is to employ voltage feedback, which controls voltage of the operating point without causing appreciable current feedback (Fig. 14-9). The bias resistor will need to have about 1/10th the value needed for the condition of Fig. 14-4.

Putting Stages Together

Operating individual stages under independently simulated conditions, both for source and load resistance, can take a big step toward securing correct operating conditions throughout a multistage amplifier. But things can still happen when stages are connected together that do not show up when the stages are checked separately. This may not seriously invalidate the over-all projected performance, but is far more likely to do so where feedback parameters are involved.

Individual stages can be checked for current gain, available swing, and the cut-off points of coupling networks by this substituted-load process.

Tolerably linear values, such as collector-circuit resistances, are arranged to swamp the effects of non-linear resistances, such as base inputs. If necessary, emitter resistors can to some extent linearize effective base input resistance (Fig. 14-10) by adding an approximately linear value found by multiplying their actual value by the working current gain of the transistor.

So far, so good, but now, when you put the whole thing together, the total response is not the sum of its parts.

Maybe the mid-hand current gain adds up nicely, but the frequency turnovers on which the feedback stability or over-all effect is based don't add up so nicely.

This is because transistors reflect impedance both ways, as well as contributing current and voltage gain. For the emitter-follower (common-collector) stage, this reflection is fairly simple and predictable: impedances, including resistance and capacitance (or inductance, if present) effects are multiplied or divided by the operating current gain of the stage (Fig. 14-11). This can be checked by impedance measurement, each way Fig. 14-12) . There are limits to which this reflection effect follows with any accuracy, even in an emitter follower, which coincide reasonably well with the limits at which its current gain begins to change. This too is fairly predictable and verifiable by measurement.

But most amplifier stages use the common-emitter configuration, which alters the picture. In this mode, the input resistance is lowest when the output load is highest ( voltage swing highest) so as to approximate constant-current output ( voltage rather than current output). When the output is loaded down so output voltage no longer swings, but there is a maximum output current swing, the reflected input impedance is much higher.

This means that output load reflects into the input circuit as an inversion:

high value reflects as a low value, and inductance looks like capacitance, and vice versa. A series capacitor (coupling) reflects an impedance component similar to shunt inductance, and so on.

The same thing happens in the reverse direction, to reflected collector impedances, due to actual base-circuit elements.

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Fig. 14-8. Changing the collector coupling resistor to get back to the proper conditions, when the following stage is coupled. Dashed lines show the condition of Fig. 14-5 repeated for comparison with the revised condition, in solid lines.

Fig. 14-9. A better way of deriving bias, (one that provides voltage feedback), to stabilize the working position shown in Fig. 14-8, without producing appreciable current feedback, in the output-loaded-down condition.


Fig. 14-10. Including emitter resistors to stabilize, or linearize, the base-input resistance reflected to the previous stages.

Fig. 14-11. In an emitter follower, resistances and impedances are reflected both ways, multiplied or divided by the working current gain of the stage, with considerable faithfulness.

Fig. 14-12. A method of checking the results predicted in Fig. 14-11 by actual measurement. The resistance meter should measure a.c. resistance and in (B) provide a current path. In each case, the resistance meter will measure the reflected value change when the real value R is changed.

Fig. 14-13. Equivalent circuit reflection with common-emitter stage. The inset schematics represent the equivalents for the circuit in that "side" of the stage. The elements in the dashed lines are those representing reflected values from the other side.

Fig. 14-14. For reasonable prediction, each stage should be measured with both coupling elements included (responses 1, 2, and 3). When adding the results together, the duplication must be eliminated by subtracting the effects of C2 and C3.

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The equivalent circuit makes it look as if resonance, in either base or collector circuit, if not both, inevitable (Fig. 14-13). But the relative values preclude actual resonance effects. The reflected elements (in this case inductive, due to actual capacitance) are invariably of changing magnitude equivalent to an inductive reactance that does not represent a simple inductance value) and always of an order well removed from resonance, so they merely effect a progressively changing effective value for the actual circuit capacitances.

If prediction is attempted in any terms at all, it should be on the basis of magnitude and phase response, rather than on equivalent circuit values, which are continuously changing with frequency. A careful series of measurements on a stage-by-stage basis can help "put the circuit together" but the prediction is limited, because stages can only be measured integrally: each with both of its equivalent coupling elements; when the whole circuit is "put together," each coupling element is present in relation to both the stage preceding it and the one following it.

If, from the measured stage-by stage responses, added together, the theoretical effects of the individual coupling networks, which are thus included twice each (except the first and last) as part of the preliminary measurements, are subtracted from the whole, an approximation close to the true over-all effect will be predicted, on which over-all feedback parameters can be later figured (Fig. 14-14). Even then, the over-all effect may differ from prediction, as more feedback is applied, because the relative input and output levels are changed at the couplings to those stages, so the response contributed in the presence of feedback differs from that contributed by the same elements in the absence of feedback, or with less of it.

This whole procedure, to be effective, requires close working between measurement and calculation at every stage, to approach a practical operating circuit design. In the next installment we shall pursue this further, by detailing some practical feedback "cutting and fitting."

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Number 42 in o series of discussions by Electro-Voice Engineers

CARDIOID IS NOT ENOUGH

ROBERT F. HERROLD, III

Microphone Project Engineer It is frequently assumed that a unidirectional microphone exhibiting a perfect cardioid pattern is ideal for reducing unwanted noise pickup. While there is an element of truth in this assumption, normal studio practices usually dictate that a microphone with a polar pattern that deviates from the classic cardioid shape is more effective.

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Dynaco. 3912 Powelton Ave. Philadelphia, Pa. 19104, U.S.A.

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The man with the golden ear 17 1/2 cubic feet of sound in your living room requires two basic essentials. The first is a Golden Ear to catch every nuance. The second, rather obviously, is a permissive wife. Some men have both (unbelievably) and have installed the actual Altec A7 "Voice of the Theatre" in their living rooms. This is the same system that has become standard for recording studios, concert halls and theatres.

However, if your wife is something less than permissive, Altec has the answer.

We have taken all A7 speaker components and put them in a single package.

Half the size. The same high-frequency driver. The same cast aluminum sectoral horn. The same 15" low frequency speaker.

The same crossover network. Frequency response is unbelievably wide ( beyond the range of human hearing, if that's of any interest). The midranges are "in person" and that's where 90% of the sound is. Basses don't growl and groan.

Trebles don't squeal. Styling? The hand-rubbed walnut Valencia has a delicately curved wood fretwork grille. The oak Flamenco is pure Spanish. Send for your '67 Altec catalog or pick one up from your dealer. Compare. Buy. If the wife complains, tell her about your Golden Ear.

A Division of , Yir C Ling Altec, Inc., Anaheim, California

SPECIFICATIONS--FREQUENCY RESPONSE: 35-22,000 Hz; IMPEDANCE: 8/16 ohms; CROSSOVER FREQUENCY: 800 Hz; DIMENSIONS: 29%" H. x 27W' W. x 19" D. (Flamenco is two inches lower); COMPONENTS: 416A 15" low-frequency speaker with a frequency response of 20-1600 Hz and a cone resonance of 25 Hz; 806A high-frequency driver; 811 B high frequency sectoral horn with 90° horizontal and 40° vertical distribution; N800G dividing network with continuously variable HF shelving attenuation.

PRICE: 846A Valencia, $333; 848A Flamenco, $345.


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Now... eliminate background noise pickup at a new low price UNIDYNE/ UNIDIRECTIONAL PROBLEM-SOLVING ABILITY AT AN OMNIDIRECTIONAL PRICE Never before such quality at so low a price! Controls background noise confusion, "thumping" sound from percussion instruments, and "hollow" sound associated with omnidirectional microphones.

You'll be amazed and impressed by the clear, life-like tapes you can make with the new Shure Unidyne A ... a low-cost, fine quality, wide-response unidirectional microphone with a truly symmetrical pickup pattern that picks up sound from the front only, at all frequencies. Only $35.40 net.

SEND FOR LITERATURE: SHURE BROTHERS, INC. 222 HARTREY AVENUE, EVANSTON, ILL. MATCHED PAIRS FOR STEREO RECORDINGS, TOO



Unidyne A pairs (matched in both frequency and output) detect the subtle differences that "localize" sound for realistic, spatially-correct stereo tapes.

Only $70.80 net for the factory-matched pair, complete with plugs attached.

(Note: The famed Unidyne II & III are also available in matched pairs).

SHURE MICROPHONES WORLD STANDARD WHEREVER SOUND PERFORMANCE AND RELIABILITY ARE PARAMOUNT

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When you've got a reputation as a leader in transistor technology, you don't introduce a transistor amplifier that is like someone else's. We didn't. The new Sony TA-1120 integrated stereo amplifier is the case in point. We considered the few remaining shortcomings that have kept today's transistor amplifiers from achieving the quality of performance of the best tube amplifiers and set out to solve them. To do it, we even had to invent new types of transistors. The result: the first truly great solid-state stereo amplifier.

Distortion is lower than in the finest tube amplifiers at all frequencies and power levels.

Signal-to-noise ratio: better than 110 db.


Damping factor is extraordinarily high (140 at 16 ohms). Frequency response: practically flat from 10 to 100,000 HZ (+0 db/-1 db). Plenty of power, too (120 watts IHF at 8 ohms, both channels). With an amplifier as good as this, the preamp section has a great deal to live up to. It does, magnificently! Solid-state silicon circuitry throughout coupled with an ingenious design achieve the lowest possible distortion. Sensible arrangement of front panel controls offers the greatest versatility and ease of operation with any program source.

Finally, to protect your investment in this superb instrument, an advanced SCR (silicon-controlled rectifier) circuit prevents possible damage to the power transistors due to accidental shorting of the outputs.

The Sony TA-1120 stereo amplifier/preamp at $399.50 and the TA-3120 stereo power amplifier, $249.50 are available at a select group of high fidelity specialists who love and cherish them. And will get as much enjoyment out of demonstrating them as you will from their performance. So visit your dedicated Sony high fidelity dealer and enjoy. Prices suggested list. Sony Corporation of America Dept. H 47-47 Van Dam St. L.I.C., N.Y. 11101.

With so many fine amplifiers our first had to be something special.

It is!


Sony

The new Sony Solid State 350 adds professional performance to home entertainment systems Selecting the brilliant new Sony Solid State 350 to fulfill the stereo tape recording and playback functions of your professional component music system will also enduringly compliment your impeccable taste and passion for music at its finest. With an instant connection to your other stereo components, the versatile two-speed Sony 350 places at your pleasure a full array of professional features, including: 3 heads for tape and source monitoring. Vertical or horizontal operation. Belt-free, true capstan drive. Stereo recording amplifiers and playback pre-amps. Dual V U meters. Automatic sentinel switch.

Frequency response 50-15,000 cps-{2db. S.N. ratio plus 50db. Flutter and wow under 0.15%. Richly handsome gold and black decor with luxurious walnut grained low profile base. This remarkable instrument is yours at the equally remarkable price of less than

$199.50. Should you want to add portability to all this, there's the Model 350C, mounted in handsome dark gray and satin-chrome carrying case, at less than

$219.50, For information write Superscope, Inc.. Sun Palley, Calif.

SONY SUPERSCOPE--The Tapeway to Stereo Portable Model 350C


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Sony adds an exciting new dimension to home entertainment for less than $14950 Now, from World-famous Sony, the perfect playmate for your record player-the new Sony model 250 solid state stereo tape recorder. With a simple, instant connection to your record player you add the amazing versatility of four track stereo recording and playback to complete your home entertainment center and create your own tapes from records, AM or FM Stereo receivers, or live from microphones-61/4 hours of listening pleasure on one tape ! This beautiful instrument is handsomely mounted in a low-profile walnut cabinet, complete with built-in stereo recording amplifiers and playback pre-amps, dual V.U. meters, automatic sentinel switch and all the other superb features you can always expect with a Sony. All the best from Sony f or less than $149.50. Send today for our informative booklet on Sony PR-150, a sensational new development in magnetic recording tape. Write: Sony/Superscope, Magnetic Tape, Sun Valley, California.

For literature or name of nearest dealer write to Superacope, Inc., Dept. 17. Sun Valley, Catifornia.

SONY SUPERSCOPE--The Tapeway to Stereo

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1. Now...a remarkable demonstration.

4. So perfectly counter-balanced

7. turning over to a complete...

2. This is the BSR McDonald 50C ... PLAYS UPSIDE DOWN

5. ...it will play upside down!

8. upside-down position. Still playing.

3. precision engineered in England.

6. Here's proof...you see it...

9. Featured at leading hi-fi stores.

Did you catch this amazing act on the Johnny Carson "Tonight" Show? This almost unbelievable demonstration of the tracking ability of the BSR McDonald 500 automatic turntable is being telecast on the popular NBC-TV Johnny Carson "Tonight" Show as well as the "Today" Show starring Hugh Downs. It demonstrates the BSR precision engineered automatic turntable doing a complete 180° turn ... while it continues to play a record perfectly even when it reaches the completely upside-down position! (The secret is the tone arm that is perfectly counter-balanced horizontally and vertically!) See this remarkable automatic turntable and see its many other unique features. Write for free literature.

McDONALD. 500 Precision crafted in Great Britain BSR (USA) Ltd., Blauvelt, N.Y. 10913

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Some plain talk from Kodak about tape:

Uniform magnetic sensitivity (or the lack thereof)

Uniformity for a tape is like kissing babies for a politician. Without it, you're hardly in the running. We take uniformity in all of tape's characteristics very seriously at Kodak. Maybe it's all those years of putting silver emulsions on film that's made us so dedicated to the idea. Uniformity in terms of magnetic sensitivity is one of the most important measures of a tape's performance. Non-uniformity can result in all sorts of bad things like level shifts, instantaneous dropouts, periodic non-uniformity, output variations, distortion, and variations from strip to strip.

Testing for all these possible flaws on a tape is a simple procedure in the lab. Standard industry practice is to record a long wavelength signal (37.5 mil) at a constant input level. The signal from the playback amplifier is then filtered and the output at particular critical wavelengths is permanently charted by a high-speed pen recorder which registers variations on a chart.

Instantaneous dropouts caused by foreign matter on the tape surface, for example, would look like this:

The long and the short of it:

The low frequency procedure gives a good picture of variations in oxide thickness. We take it one step further ... also test for short wavelength-1.0 mil. This helps evaluate surface smoothness and tape-to-head contact.

Taken together, they aid in evaluating the level of lubrication, slitting, and oxide binder characteristics. The smoother the lines, the more uniform the magnetic sensitivity. Guess which graph below is KODAK Sound Recording Tape (the other two graphs represent quite reputable brands of other manufacture) :

What looks good sounds good.

Congratulations if you picked brand A, Kodak tape. It is notably more uniform

...doesn't vary more than 1/4 db within the reel ... no more than 1/ db from reel to reel.

You benefit as follows:

1. Within-reel uniformity.

(a) Less instantaneous and short term amplitude modulation of the signal, which results in a cleaner signal on playback.

(b) Reduced drift gives less variation in frequency response.

(c) Better uniformity across the strip width (no lengthwise coating lines) results in a more nearly balanced output for stereo recordings.

2. Reel-to-reel uniformity.

(a) Better coating uniformity gives a more uniform low-frequency sensitivity. This allows splicing of sections of tape from one reel with tape from other reels without obvious signal level changes.

(b) Better coating uniformity also results in a minimum change in optimum bias which allows the professional to establish an operating bias nearer the optimum bias.

KODAK Sound Recording Tapes are available at most camera, department, and electronic stores. New 24-page comprehensive "Plain Talk" booklet covers all the important aspects of tape performance, and is free on request. Write: Department 940, Eastman Kodak Company, Rochester, N.Y. 14650.

KODAK SOUND RECORDING

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Also see:

AUDIO in General

Program Your Listening for Up To Thirty Hours

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Updated: Friday, 2026-05-15 11:52 PST