Eberhart's Manual of High Frequency Currents
Noble M. Eberhart
Chapter Six
General Technique; Vacuum Tubes; Lubrication; Cautions; Asepsis; Method of Standardizing Dosage; Author’s Unit for Measuring Auto-Condensation; Preparation of Patient; Technique for Skin Diseases or Surface Lesion; for Relief of Pain; Cauterization; Orificial Technique; Cataphoresis; Bi-Polar Tesla Technique; Selection of Most Suitable Form of Current; Fulguration; Constitutional Treatment; Auto-Conduction; Auto-Condensation; Portable Pads; Home-Made Couches and Pads; D;’Arsonval “Surgings”; Water Spray; Local Auto-Condensation; Indirect Sparks; Taking the Blood Pressure; Miscellaneous Suggestions; Diathermy.
   One author gives upwards of twenty different methods of using high frequency currents.  This is apt to prove confusing to the ordinary user of these currents, and I have reduced the headings under which to discuss technique to those methods most commonly in vogue.

Classification of Technique:
   1.  Vacuum tube technique.  (Tube excited by Oudin or Tesla currents.)
   2.  Fulguration.
   3. Constitutional (auto-condensation and auto-conduction).
   4. Diathermy.  (Direct D’Arsonval; electro-coagulation; thermo-penetration.)

   This involves the use of the tubes by direct contact, by effleuve (fine spray) and by actual sparks, from the mildest form to the sharp caustic forms.  It may be classified otherwise according to its use as in (a) skin diseases, ulcers, inflammatory processes, etc.; (b) relief of pain, as in neuralgias, etc.; (c) orificial application.
   Vacuum tubes are employed where an essentially local effect is desired.
   Lubrication of Tubes.  Any of the lubricating jellies, unguents or cerates may be employed on tubes used within the urethra, vagina or rectum.
   Vaseline answers very well, for, although it is a non-conductor of ordinary electricity, the thin coating required on these tubes is absolutely no bar to high frequency currents.
   Cautions.  1.  As stated in Chapter V., high frequency currents are capable of producing annoying but not ordinarily serious surface burns.  These effects are especially quick to appear when mucous surfaces are treated, as in rectal, vaginal, urethral or nasal applications, and also in treating diseased areas about the lips.  On this account the application should be relatively short and mild if a spark is employed in treating within the various orifices.  Make it a general rule never to allow a vacuum tube to remain in contact with a mucous membrane for more than seven minutes at one treatment.
   2.  When the current is one of relatively high amperage, the spark will set fire to any easily inflammable material.  This may be illustrated by lighting the gas with the spark, as previously referred to.  On this account care must be exercised in treating certain areas.
   3.  When introducing glass sounds into the male urethra great care must be exercised not to use any undue force and thereby break off the glass tube within the canal.  These tubes are made of strong glass, but may be broken by unusual pressure, or by a sudden jerk.  If difficult of introduction it is better to pass steel sounds first to a size larger than the glass sound, as suggested in Chapter VII under Urethral Technique.
   Care of Vacuum Tubes. Asepsis.  Although the spark or effleuve from the vacuum tube is germicidal in character, still it is the duty of the physician to use the utmost care and cleanliness in employing it in order to guard against any possibility of spreading infection from one patient to another.
   In other words he would better follow some definite system of sterilizing and disinfecting the tubes, and the nearer this is to surgical asepsis the better.
   Wiping off the tubes on a cloth or towel or simply rinsing in water is not enough.
   Apply the test to yourself.  How would you like to be treated with a tube that had been used in contact with a specific disease and which had received no further cleaning than mere dipping in water and then being wiped off with a towel that had already done similar service an indefinite number of times?
  Let your technique be so careful and conscientious that you need never blame yourself for spreading contagion or infection of any kind.
   This is a subject that I have not seen mentioned in any treatises on high frequency currents.
   Do not use the same tube for specific and non-specific orificial cases.  This alone will do much toward lessening the danger of infection.
   As these tubes bear heating, they may be sterilized by boiling, just as surgical instruments are sterilized.
   This, however, is not necessary, as immersion in strong antiseptic solutions will be sufficient.
   A tube that is to be used in contact with a mucous membrane, such, for instance, as a vaginal or urethral electrode, should be immersed in pure carbolic acid or in pure crethol, benetol or lysol, before again using, if it has been in contact with the discharge from a specific disease.
   In cases such as acne, psoriasis, eczema, neuralgia, non-specific diseases of the urethra, rectum or vagina, etc., it will suffice if the tube is immersed for a few moments, or kept permanently, when not in use, in a strong solution of any one of the three antiseptics mentioned in the preceding paragraph.
   For this purpose a glass jar, large enough to take in the various electrodes, should be filled with a twenty percent solution of carbolic acid (a five per cent solution is not enough); or as its equivalent, one of crethol, benetol or lysol containing a tablespoonful of either to the pint of water.
   An ideal way would be to have two jars, one containing the full strength antiseptic, for the tubes employed in infectious cases, and the other for those used in non-contagious diseases.
   Personally I prefer crethol or lysol to carbolic acid, because equally satisfactory and not caustic if any of the full strength liquid accidentally comes in contact with the operator’s hands.
   If the tubes are immersed in the pure antiseptic they should be thoroughly rinsed in alcohol and water, or in water alone before using.  From the weaker solutions, water alone is necessary, but in both cases hot water is preferable.
   The conveniences of most of our modern office buildings make the technique of sterilizing the tubes a simple one in the large cities, but in smaller towns the physician will find it somewhat more of a task.
   In the absence of large jars to keep the two solutions in, with the tubes constantly immersed, wide mouthed bottles may be employed for use before and after each treatment.
   By sterilizing in this manner both before and after, the tube not only receives a double sterilization, but also if it has been taken care of immediately after use, if such a thing should happen that it should be used again without remembering about sterilizing it, the danger would be slight, and furthermore the tube is easier sterilized immediately after using, than it is when the secretions or discharges have dried upon it.
   I have spoken of using the same care that you would with a surgical instrument, although the danger with these tubes is not as great as with surgical instruments for several reasons.  In the first place, they are not employed ordinarily in a fresh wound: secondly, the danger is in carrying infection from one patient to another and not the additional danger which accompanies a surgical operation, of infecting the wound from the individual as well, and finally, in the majority of the cases treated there is practically no serious danger of infection.
   If one had a sufficient number of tubes it would be desirable to keep an individual tube for each patient, which was used for no other.  Immersion in the weaker solutions referred to above and rinsing, or even ordinary cleanliness would be sufficient; but at the close of the course of treatments, before the tube was used for another case it then should receive vigorous and thorough sterilization, in proportion to the danger of infection involved in the case.
   The sterilizer shown in Fig. 28 is an excellent one.  A basin of formalin solution keeps the tubes always sterile.
   Some of my readers may think I am devoting too much space to this subject, but it is an important one, and my early surgical training has made me a “crank” on this point, and really, could you ever excuse yourself if through your carelessness you spread, say a specific infection, even in one single instance.
   Measuring Dosage.  One problem that confronts the physician who is beginning to use the high frequency is a method of measuring dosage.  There is no meter which will measure the output of the vacuum electrode, or in other words the unipolar current.  For auto-condensation and for diathermy the hot-wire meter is used and proves relatively satisfactory.  For the vacuum tube, in order to convey an idea that would apply, no matter what size or make of apparatus might be employed, I have made use of the length of spark which it is possible to draw from the vacuum tube as a simple method of giving some idea of the strength of current employed.  This is a very crude method, and open to some serious objections, but will answer the purpose in a general way and convey a more intelligent idea than any method other than a meter.
   With a definite amount of current passing through the apparatus, there is a positive point near the tube that represents its utmost sparking distance, that is, the longest spark that can be drawn from that tube, and this will remain constant as long as the current is constant – lessening the current shortens the spark; increasing it, lengthens it.  Therefore, if I say I employ for skin diseases a tube capable of yielding a one-quarter inch or one-half inch spark, I give to the physician a definite idea of the amount of current I would employ in the tube.
   This does not take into consideration the sharpness of the spark, which must be adjusted in accordance with individual susceptibility and the type of machine used.
   With the Tesla type of apparatus and particularly with small machines, the spark is apt to be sharper in proportion, and is designated frequently as a “hot” spark.  With these outfits it is often impossible to employ a spark more than a quarter of an inch in length.  With other types, a longer spark will be tolerated, and with the Oudin type of apparatus we have what may be called a “cold” spark, and frequently one three-quarters or an inch long may be more easily borne than a quarter-inch “hot” spark.  The cold spark is dehydratory and the hot spark caustic.  In interpreting my suggestions for dosage in Chapter VIII, these facts should be taken into consideration.  Ordinarily if the dose is given one-fourth to one-half inch the first would be for the “hot” and the second for the “cold” spark.
   The Eberhart.  Author’s Unit of Measurement for Auto-Condensation.  For a long time both physicians and manufacturers have felt the need of a standard unit for measuring auto-condensation; one that would fairly represent the auto-condensation output of any type of machine.  I believe I have solved this problem, and have a standard of measurement that will prove acceptable to the manufacturers of any form of apparatus.  It will be found convenient for the manufacturer to state with the directions for auto-condensation that the output of the machine is so many Eberharts per minute to each 100 milliamperes registered on the hot-wire meter.  In this way with the dosage given as a certain number of Eberharts, it is easy to note by the meter how many Eberharts are passing per minute and by noting how many times this number will go in the total dose stated the number of minutes required for the treatment is ascertained.
   There are three essential elements entering into auto-condensation.  First, the pressure or potential (voltage); second, the rate or meter reading (amperage); and third, the time.  When the voltage is high the amperage is correspondingly low, and vice versa.  In a general way the effectiveness of any machine for auto-condensation may be expressed in terms representing the product of the voltage and the meter reading (equivalent of amperage).  Thus 50,000 volts at 500 is the same as 25,000 volts at 1,000; each representing an auto-condensation effectiveness of 25,000,000.
   My unit of measurement for auto-condensation is based on the passage of 1,000 volts at a rate of 100 milliamperes in one minute of time.  This unit I call the Eberhart and abbreviate it E.
   We have two types of apparatus for auto-condensation, the one high voltage and comparatively low amperage; the other low voltage and high amperage.  In a general way I assume that the first represents a current of about 50,000 volts delivered at a rate of 350 to 500 milliamperes as shown on a hot-wire meter.  The second averages 25,000 volts, potential, and is ordinarily delivered at a rate averaging 750 to 1,200; 1,000 being a frequent rate.  Applying our unit it will be seen that 50,000 volts equal 50 E. For each 100 milliamperes meter reading, and if the meter read 500, there would be delivered 5 times 50 or 250 E. For each minute of time, and this would give 2,500 E in a ten-minute treatment.  With the other machine 25,000 volts equal 25 E. Per 100, and with meter at 1,000 would give 10 times 25 E. Or 250 E. Per minute, or 2,5000 E. Would require a ten-minute treatment.
   The manufacturer may state the voltage of his machine, if desired, but the simpler way is to give the number of Eberharts to each 100 milliamperes meter reading.  He should also state the average meter reading at which the apparatus is to be operated.  If he states the voltage, to compute a required dose, multiply the meter reading by the number of thousand volts, and divide this product by 100.  This is the number of Eberhart units being given per minute, and by dividing the dose as given in Eberharts by this, we have the number of minutes required.  Going back to our previous example: to give 2,500 E. auto-condensation on a machine of 50,000 volts with enough current passing to raise meter to 500, multiply number of thousand volts, 50 by meter reading 500, and product is 25,000.  Divide by 100, which is done by cutting off two ciphers, and we have 250, which is the number of Eberharts per minute–250 goes into 2,500 ten times, therefore it takes ten minutes to give the required dose of 2,500 E.
   It will be seen that it would be much simpler if the manufacturer stated with this machine that the auto-condensation output was 50 Eberharts per minute for each 100 milliamperes registered by the meter.  Then if the dose to be given is 2,500 E. And the meter registers 500, or five times the 100 rate, it is easy to figure then that 500 is five times 50 or 250 E., and this goes in 2,500 ten times, therefore it takes ten minutes to give that amount.
   With the other type of machine we will say that the output is 25 E. Per minute per 100 milliamperes; but this machine will ordinarily be operated at about 1,000 milliamperes, or ten times 100, therefore it is also delivering ten times 25 E. Or 250 E. per minute, and it will also take ten minutes to give 2,500 E.  In Chapter VIII the dosage of auto-condensation will be stated in Eberharts.
   It is well to remember that there is essentially no danger in auto-condensation and therefore no over-dose, so that the dosage stated may be greatly increased if results are not obtained.
   The only cases in which caution is necessary, are those where a patient is carrying a high temperature or where the pulse pressure is 20 or lower.
   Preparation of Patient.  When the surface of the body is to be treated, the question of removing the clothing arises.  If no spark is desired, the electrode must be in contact with the skin, and any clothing covering the part must be removed.
   All metal, such as chains, corset-steels, wire hairpins, etc., with which the tube comes in contact or within sparking distance of, will be charged with the current and give rise to sharp and disagreeable sensations.  If they cannot be avoided they should be removed.
   Applications to the body, calling for a mild spark, may be given through thin underclothing, or the patient stripped and covered with a sheet, through which the spark is employed.
   Aside from the reason spoken of above (chains, etc.), when a sharp spark is required there is no especial need of removing the clothing, in fact, a definite thickness insures a definite length of spark.
   When the tube sticks on the skin, dust on talcum powder or lay over the surface a very thin cloth, such as a handkerchief.  In vaginal treatments no disrobing is necessary.
   General Technique in Skin Diseases and Surface Lesions.  In applying the high frequency spark over the surface of the body, as in acne, eczema, etc., I employ a current of sufficient strength to produce a spark one-quarter to three-quarters of an inch in length.  The discharge from the smaller Tesla coils is relatively sharper than from the resonator or larger Tesla outfits, and a shorter spark is used, as the patient cannot tolerate quite as much current in these instances.  With a vacuum electrode capable of delivering a spark of the length given, I do not try to make use of the full length spark, but keep the tube in light contact with the skin, thus giving a sufficient intensity of current, but avoiding the pain that would result if the tube were held at full sparking distance from the surface.  The tube is passed rapidly back and forth over the area treated, and this will be accomplished in the easiest manner by holding the tube handle lightly with the fingers, with the thumb extended along the handle.  A side to side motion with the wrist will soon become a matter of habit to the operator and the tube will pass lightly over the surface without any sudden jerks or elevations to cause annoying sparks.

Fig. 28b - Vacuum Electrode Technique.

   If the skin is moist and the tube sticks, it may be dusted with talcum or other dusting powder to obviate this difficulty.  Another method is to place a thin cloth over the surface, which will enable the tube to be used smoothly and at the same time does not remove it far enough from the surface to make an unpleasant spark.
   Where itching is marked, the tube is raised from the skin and as sharp a spark applied as the patient will tolerate for a short period of time.  This quickly relieves the itching and also quickly produces the characteristic reaction of the current (hyperemia, etc.).
   In treating epithelioma, lupus and any chronic ulcers, a spark is employed in the same manner, that is, as sharp as the patient can stand, but not for a long period, say from two to three up to occasionally five minutes.  Unless cauterization is sought, the tube should be kept moving rapidly over the surface and not allowed to expend its full effect steadily over any minute area.  At the present time fulguration (caustic) would be employed more frequently for epithelioma and lupus.
   Technique for Relief of Pain.  In congestive headaches, neuralgias and other painful conditions, the beneficial action of the high frequency current seems to be largely the result of counter-irritation.  Therefore, it makes very little difference whether a sharp spark is used with the rapidly moving tube at full sparking distance, or whether with the same intensity of current, the tube is kept in contact with the skin.  It depends upon the sensitiveness of the patient and also upon the location of the area treated.  A long sharp spark occasionally exerts a slight caustic effect, and the surface will be covered with tiny blebs, which are followed by minute scabs, making the skin sore and uncomfortable.  Unless the case to be treated is a severe one, it is not permissible to push the treatment to this degree.
   Cauterization.  If a hot spark is held steadily over the spot for from thirty seconds, up to two or three minutes, varying with the patient, it will have a cauterizing effect.  The reaction is severe and the destruction of the tissue may be carried to a marked degree.  Such applications have been used in the treatment of warts, moles, etc.
   I have treated epitheliomas in this manner and have had them separate from the surrounding tissue and peel out as smoothly as if cut out with a die.  It is too severe a measure, however, for the average case.  Fulguration involves the same principles, and is preferable.  The spark is derived from a metal point and anesthesia may be employed if desired.  The technique of this will be considered in another section.
   Orificial Technique.  The technique of the application to the orifices of the body involves the use of tubes suited to the various areas, and also involves the question of sterilization and lubrication.  In these cases the tube is in contact with the mucous membrane and there is no sensation to the treatment except usually that of warmth.  There is in these cases greater danger of producing burns, and the tube should seldom be left in contact for a longer period than seven minutes at any single treatment.  (See the section on vacuum tube burns in Chapter V.)  The technique is so peculiarly that of the special organ involved that it will be given under its appropriate heading in Chapter VII.  It is desirable to remember that tubes should always be inserted before the current is turned on, and the latter turned off again before the tube is removed, thus avoiding all pain and shock to the patient.
   Cataphoresis.  For cataphoresis a special electrode is employed.  See Fig. 29.  The substance to be carried into the tissues is in solution, and cotton gauze or felt wet in the solution is placed in the depression on the face of the tube when the latter is placed in contact with the desired area and the current passes for from five to ten minutes or more as required.  I caution against the use of solutions containing alcohol or other inflammable substance because of the danger of setting same afire with the current.

Fig. 29 - Cataphoresis Electrode.

   In one form an insulating ring prevents loss of current and is a great improvement on the older style of tube.
   See Chapter XII for special electrodes used by dentists.
   Although strong claims have been made concerning the value of high frequency currents for the purpose of carrying substances into the tissues, I believe they are so far inferior to the galvanic current for use for these purposes that they are entitled to comparatively little consideration.
   The principle upon which cataphoresis depends is the separating of the particles (ions) composing the fluid by reason of the attraction possessed for them by the poles of the battery; thus all positive elements remain at or are drawn through the tissues toward the negative pole, and vice-versa.  Now, in using high frequency currents, which are alternating, the attraction would be first in one direction and then in the other and as a result practically nothing would be accomplished.
   The claim is made that the high frequency current drives substances into the tissues by “molecular bombardment.”  I maintain, however, that the cataphoric action of the high frequency current is too feeble to commend it for general use, for which purpose nothing takes the place of the galvanic current.
   The use of dental electrodes for cataphoric purposes has given good results.  See Chapter X.  It is really an electrical diffusion, rather than true cataphoresis.
   Bi-polar Tesla Technique.  Ordinarily the vacuum tube is attached to one pole of the Tesla outfit.  In some coils the sharpness of the spark is regulated by drawing off a certain amount of the current from the active pole by bringing the sparking rod near it, thus lessening the available current.
   If it is desired to intensify the action of the Tesla coil, the indifferent pole should be attached to the patient or grounded by connecting to a gas or water pipe.
   Selection of Most Suitable Form to Use.  Where a local effect is more essential, vacuum tubes, metal electrodes, etc., are employed, but if a systemic or constitutional effect is desired, auto-condensation is to be selected, or the diathermic treatment may be used.


   Fulguration.  A long sharp spark for escharotic or destructive purposes was employed for a long time by high frequency operators, but the use of a metal electrode devised by Keating-Hart for this purpose, which he termed fulguration, gave an unusual impetus to the method.
   Fulguration as employed at the present time may be considered under two forms: 1.  Caustic or hot fulguration, employed with D’Arsonval or Tesla apparatus, and giving a hot, caustic or cauterizing spark.  The D’Arsonval fulguration is particularly suitable in orificial work, such as papilloma of the bladder, etc.  The Tesla is especially advantageous in surface work, such as moles, warts and other superficial growths.
   2.  Dehydratory or cold fulguration, employed with Oudin apparatus.  The destruction of tissue is through a drying process and there is no sloughing.  There is essentially no pain, but its range is necessarily limited.
   Dr. W. F. Clark of Philadelphia employs a method of cold fulguration with the static machine, to which he has applied the term dissication.

Fig. 30 - An Outfit Combining High Frequency with Numerous Other Modalities, Twenty-one in All.
Fig. 31 - Application of Vacuum Electrode to Chest.

   General Caustic Fulguration.  The technique which I employ for warts, moles and small growths is as follows:
   The fulguration electrode is attached and the current turned on gradually, while the length of spark from the metal point (Fig. 33), is tested by bringing the point nearly in contact with a piece of metal, such as a coin.  Without an anaesthetic it is impossible to employ one more than one-thirty-second to one-eighth or occasionally three-sixteenths of an inch in length.  This spark is hot, and actually sears or burns the tissue, as noted by the eye and usually by the odor.

Fig. 32 - Fulguration Electrode.
Fig. 33 - Fulguration Electrode.

   It is not desirable to keep this spark in steady contact, as it is too painful, but if the point is touched to the surface and quickly brought away beyond sparking distance, the patient is better able to stand it, and by a series of rapid sparks produced by a tapping motion of the point, thorough fulguration my be achieved without unbearable pain to the patient.  Ordinarily I pass around the margin of the growth first, and then fulgurate the center.  It should be done thoroughly, and the growth will present a brown, burned appearance.  There is seldom any hemorrhage, but usually some serious oozing.  A crust or scab forms which separates in a week or ten days (average eight), leaving no scar.  It is well to bear in mind that if you do not get it all off the first time you can fulgurate again, but if you remove too much you cannot place it back again.
   For more extensive work, local or general anaesthesia is necessary.
   It is fair to state that very satisfactory caustic (hot) fulguration may be accomplished with small machines.
   In papillomata of the bladder, fulguration has been particularly valuable.
   Fulguration of Papillomata of Bladder.  The hot or caustic fulguration may be employed, using wire insulated with rubber tubing, or the D’Arsonval method, which is bi-polar, may be used, as follows:  One terminal of the apparatus is connected to the fulguration wire, which is passed through the cystoscope, and the other terminal is connected to an indifferent flat metallic electrode placed on the abdomen.  The fulguration wire or electrode consists of a steel wire insulated with pure gutta-percha.  As this wire is to be passed through the channel of an ordinary catheterizing cystoscope, it should not be larger in gauge than No. 6 French.
   The patient is prepared with green soap and water and bichlorid, and the bladder distended with water.  After the cystoscope is introduced, the tumor is brought in view and the fulguration wire passed through the catheter channel of the cystoscope until the end of the wire is in view.  The wire is then plunged into the tumor and the current turned on.  (Before introducing the wire into the cystoscope, cut the wire so that the insulation is flush with the end of the wire.)  Just as soon as the high frequency current is turned on, bubbles (presumably hydrogen) are seen emanating from the tumor.  If the tumor is small, or the electrode has been placed near the top of the tumor, an immediate blanching of the tumor is seen.  This treatment can readily be carried out under the guidance of the eye, providing the insulation of the fulguration wire is intact; unless the insulation is intact, a short-circuit in the cystoscope and subsequent burning out of the cystoscope lamp may result.
   After allowing the current to pass into the tumor for about twelve to fifteen seconds, the current is shut off, the fulguration wire withdrawn and re-applied to another part of the tumor.  In large tumors, this procedure can be repeated until many different areas of the tumor have been treated in one sitting.  As long as five or six minutes may be consumed in one sitting.  Naturally, the duration of each treatment will depend on the size of the tumor.  For example, in one case, one sitting consisting of three 12-second applications was enough to completely destroy a small papilloma.
   As long as the intra-vesical electrode remains in contact with the tumor no pain is experienced by the patient.  When working near the base of the tumor, or if the electrode comes in contact with the bladder-wall, the patient frequently complains of pain.  So that during the first fulgurations there is no pain, whereas, toward the end f the treatment, while working near the bladder in treating the remaining tags, the patient at times complains of pain.  It is also necessary to consider the pain incident to cystoscopy.  This is variable in different persons, so that some of the patients cannot tolerate long sessions as well as others.  The number of treatments or sittings, as previously stated, is determined by the size of the tumor, some cases requiring as many as six sittings.
   Attention is called to the burning off of the insulation near the end of the fulguration wire.  After the current has been turned on and the treatment carried on for a little while, sometimes only ten seconds, the insulation becomes soft, and falls off or burns off from the end of the wire, so that it becomes necessary to withdraw the wire and cut the end off squarely.  Unless this is done, there is danger of the bare wire causing a short-circuit in the cystoscope.
   Usually when the high frequency current is applied the tissues become white and shrivel up.  Sometimes the tumor surface appears dark, as though it were baked.  Not infrequently after an application a larger or smaller piece of the tumor adheres to the end of the fulguration wire.  At other times these small pieces may be passed at the next urination, and often they are obtained from the wash water.  These are carefully saved and examined microscopically.
   It is suggested that papillomata should be considered malignant in all cases; that in all cases of long standing cystitis which has persisted even in the presence of careful treatment, or with the history of frequent relapses, papilloma should be suspected, and the diagnosis confirmed or contradicted by cystoscopy.  It is the consensus of opinion that the fulguration method is followed by remarkable results, but as yet sufficient time has not elapsed for us to make a definite statement as to an absolute guarantee that this treatment will prevent recurrences.  (Abstracted from an original article,

Fig. 34 - Portable Outfit.

“Fulguration Treatment of Bladder Tumors,” by Herman L. Kretschmer, M. D., of Chicago.  Illinois Medical Journal, April, 1913.)


   Auto-conduction.  In auto-conduction the patient is placed within a large solenoid or coil, constituting a cage.  The patient is not in contact with this cage at any point and the high frequency currents in the patient’s body are produced by conduction.
   The cages are of several types, some in perpendicular form, and others in a horizontal position.  In the latter the patient is either placed on a board which slides into the cage, or the top of the latter is hinged like the cover of a basket.  Some of the perpendicular forms are collapsible, others are fitted with a door, the patient standing or sitting on a stool.
   Small cages are also made into which the arm or leg may be introduced, thus producing localized auto-conduction effects.
   The dosage is the same as with auto-condensation.

Fig. 35 - Horizontal Auto-Conduction Cage.  Now Seldom Used.

   Owing to an inherent objection on the part of the human race to being incarcerated in a cage, even for a short time, this method of treatment, although excellent in results, is used comparatively little at the present time; furthermore, it has no advantage over auto-condensation.
   Auto-condensation.  In auto-condensation, one of the terminals of the apparatus is attached to the metal forming one plate of a condenser and the other to the patient, who becomes in this manner the other condenser plate.

Fig. 36.
Fig. 37.

   The patient is insulated from the metal plate by silk floss, rubber, mica, glass, or other form of dielectric.
   In Figure 36 is shown a cross-section of a plate condenser.  In Figure 37 the body of a woman is substituted for the upper plate, thus showing the principle involved in auto-condensation.
   Auto-condensation is administered by means of a couch or pad designed for the purpose and may include the whole body or be constructed to influence only a part of it.
   The original couch was in a form similar to that of a Morris chair (Fig. 38), the plates of zinc being under the cushions on back and seat, the cushions themselves being stuffed with silk floss or with Spanish moss.  The plates connect with one binding post of the apparatus, and the other is connected to a rod from which wires run to metal handles on each side, which are held by the patient, who receives the charge whether one or both handles are grasped.
   In that part of the circuit that is connected to the handles a hot wire meter is placed to measure the dosage.  No other form of electrical treatment gives so high an amperage, except diathermy, the dose running from 150 to 1,500 milliamperes, with occasional reports of the use of even a stronger dose.
   It is well to remember that there are two types of machines used in producing auto-condensation.  One has high voltage, but comparatively low amperage, requires a cushion at least three inches thick and has great penetration, so that a vacuum tube will light up within an area of several feet surrounding the patient.  With this type the average meter reading to obtain satisfactory result is 350 to 500.  It is seldom necessary or desirable to secure a higher reading.  Lower readings, 150 to 200, would be used where it was desired to influence nutrition without particularly lowering blood-pressure.

Fig. 37a - Portable High Frequency, Telatherm Type.

   The other type machine has comparatively low voltage, but high amperage.  It may be used with a thin pad if desired.  The meter will read 750 to 1,000 on an average, and up to 1,200 or 1,500, according to the potential of the apparatus.  Auto-condensation is measured in Eberharts, as stated in a preceding section in this chapter.

Fig. 38 - Auto-Condensation couch with Oudin Resonator and Induction Coil.  Original Type.  Now Obsolete.

   As long as the patient is in electrical contact with the handles, that is, perfect contact, no sensation is felt except occasionally a slight tingling or sensation of warmth.  Sparks may be drawn from the patient, and these may be quite painful.  In type No. 1 a vacuum tube held in operator’s hand will draw a spark from patient which is known as one form of indirect spark.  In general, a feeling of warmth pervades the body after a few moments, and the temperature is shown by the clinical thermometer to be from one-half to one degree higher than before the treatment.

Fig. 38a - Portable Outfit.

   The couch or cushion is connected to one terminal of the apparatus, the patient to the other.  The static machine with hyper-static transformer does not give a sufficient amperage for the satisfactory operation of a couch; neither does the average portable outfit, although the latter has more amperage than the static machine.  Both of these may be used for charging small pads for restricted areas, and some types of the larger portable coils I have found capable of operating a good-sized pad, if the dielectric is thin.
   In 1903 I designed the first portable body pad, which folded together when not in use.  It consisted essentially of the top of the couch and was intended to save the space required for the latter.
   About the same time Piffard produced a condenser pad for the set of an ordinary chair (Fig 41)
   It is a well-known fact that the thinner the di-electric is, as long as it is a perfect di-electric, the greater the corresponding charge that may be held on each layer of condenser.  This caused me to substitute flexible mica for the material used in the ordinary pad and thus produce a portable auto-condensation pad only half an inch thick, and capable of being slipped under the leather cushion of the ordinary office treatment table, converting the latter into an auto-condensation table.  At the same time a much greater charge of electricity may be condensed in the patient than with the thicker pads.
   Pads less than three inches thick have been condemned by the standardization committee of the American Electro-therapeutic Association, therefore, at the present time I employ only the thick cushion.
   Many ingenious operators construct their own chair or couch, and from an article of mine on this subject in Popular Electricity, November, 1909, I make a few excerpts:
   “A glass slab, four or five feet in length, twenty inches wide and about one inch thick, such as is used in a glass-topped operating table, is fitted in a wooden frame and to the under surface is attached a strip of zinc or of sheet lead 1/32 of an inch thick.  This strip should be about ten or twelve inches wide, so that when placed on the lower surface of the glass it will leave a margin of about four or five inches between the edge of the zinc and the edge of the glass.  It should extend lengthwise to within six inches of either end of the glass slab.  The zinc or lead plate is connected by an ordinary covered conducting wire say, not smaller than No. 10 or 12, to one pole of the high frequency apparatus and the patient connected by an ordinary metal electrode to the other pole.  The patient may be placed directly on the glass, but it is preferable to place him on a thin cushion upon the glass, for sake of comfort.

Fig. 39 - Portable Coil.
Fig. 40 - Portable coil.
Fig. 41 - Condenser Cushion for Chair.

   “Another method is to take a wooden table long enough for the patient to lie on and place underneath the table top a layer of plate glass the full size of the top of the table with a strip of lead or zinc attached to the under surface of this glass, always bearing in mind that the essentials of an auto-condensation pad are to have a di-electric with a layer of condenser below it, and the patient attached to the apparatus to form the upper layer.  Thus, an ordinary Morris chair or steamer-chair may be used and a layer of lead or zinc fastened underneath the back and seat of the chair, the two strips being fastened together with metallic connections (chain or wire) and underneath the ordinary cushion of the chair, four or five layers of rubber are placed to serve as the di-electric, although the cushions themselves, if they remove the body beyond the sparking distance of the charge on the zinc plate, would really make the air space intervening serve as a di-electric.  This is not as satisfactory as when the layers of rubber are placed between.  The patient then is connected by the ordinary metallic hand electrode and conducting cord or metallic handles may be fastened on the arms of the chair, the two connected by a bifurcated conducting cord to the one pole, the zinc plates to the other.
   “Lastly, a pad may be constructed on the same plan as the one which I have designed, using one or more layers of sheet mica large enough to permit the body of the patient to rest on and making use of a layer of condenser either lead or zinc underneath the mica, taking care that it does not extend near enough to the edge of the mica to allow the charge to leak over.  On top of the mica place three or four layers of felt or cover with leather as desired.  Should the mica be insufficient to prevent some sparking through, it may be obviated by placing another thin cushion on top of this pad.”
   The patient is placed on the couch or pad and connected to the apparatus before the current is turned on, and then the current turned off before the patient lets go of the handles, thus avoiding all shock.
   If the patient questions whether he is getting any current or not a few sparks drawn from his body readily convinces him.
   Another form of treatment which the patient feels to the extent of strong muscular contractions may be made by introducing a spark-gap into the patient’s circuit.  This I describe in another section as D’Arsonval surgings.
   The value of auto-condensation depends upon its remarkable effect upon general metabolism (see Chapter V).  In nearly all cases of hypertension the blood-pressure is lowered.
   Auto-condensation treatments average ten to thirty minutes in duration (2,500 to 7,500 Eberharts), and should be given daily, or six times a week at first, in nearly all cases, gradually decreasing as improvement takes place.  Less than three treatments per week at the start are, in my opinion, practically useless.  Longer treatment may be given if the physician desires.
   Cautions.  There is practically no danger of an over-dose of auto-condensation, the only danger being in cases where the patient has a high temperature that will be raised still higher, where a small dose, if any, is given, and in case of a pulse pressure below 20.  See section Taking the Blood Pressure, and under Arterio-sclerosis, Chapter VIII.  In low pulse pressure there is danger of obliterating the pulse by auto-condensation.
   Author’s D’Arsonval Surgings.  I have alluded to the fact that placing a spark-gap in the patient’s circuit causes strong muscular contractions.  The similarity between this and static “surging” caused me to apply the term of “D’Arsonval surging” to this form of treatment.
   I first noticed it when adjusting the sliding rod on a D’Arsonval-Oudin resonator.  This rod enables the operator to balance the current between the coarse solenoid and the resonator, or “tune” the coil.  Doing this with the patient on the auto-condensation couch caused the latter to exclaim at the resulting muscular jerks.

Fig. 42 - Author’s D’Arsonval Surgings.
Separating the Sliding Rod at A or Introducing a Spark-Gap
Anywhere Between A and the Patient, Produces This Effect.
   The effect of separating the point of this rod from the solenoid is to introduce a spark-gap in the patient’s circuit and to lower the frequency to the point of causing gross muscular contractions.  An outline of the method is shown in Fig. 42.
   It really is in line with the original experiments of D’Arsonval, who first doubled the number of solenoids, thus producing auto-conduction; then doubled the condensers, as in auto-condensation; and now this form doubles the spark-gap, the only remaining element employed in the D’Arsonval circuit.
   High Frequency Water Spray.  V. Laughter has devised an ingenious method of connecting the high frequency current to hydro-therapeutic apparatus in such a manner that the stream or spray of water emerging from the latter is charged with the current and when this strikes the body of the patient he receives the effect of the high frequency current as well as that of the water.
   Local Auto-Condensation.  The “Plate Glass Method.”  Various methods have been devised for applying auto-condensation locally over small areas.  Sheets of rubber with a pocket in which to slip a flat lead or zinc plate are one form.  A very popular way, known as the “plate-glass” method, consists in using as an electrode a metal point or ball and applying the sparks through thick plate glass held in contact with the patient’s body.  The glass is the di-electric, the electrode corresponds to one plate of a condenser, and the surface of the body next to the glass the other.
   Indirect Sparks.  If a resonator is connected directly to a patient with a metallic electrode and a vacuum tube is then brought near the patient’s body sparks will fly from the latter to the tube.  These are called indirect sparks.  See Figure 43.
   Attaching the patient in a similar manner to one pole of the Tesla coil, while the tube held by the operator is grounded by connecting to water pipe or gas jet, accomplishes the same result.
   Another method of deriving an indirect spark and one with which I have been experimenting considerably during the past few years is obtained from the patient when lying on the auto-condensation pad.
Fig. 42a - Local Auto-Condensation.

   I use a high-voltage, low-amperage type of machine with a thick pad.  Enough current is turned on to give a meter reading of about 250 (125 E.).  A vacuum electrode is held in the operator’s hand and the length and strength of spark tested by touching the metal handle which the patient is holding, before the tube is applied to the patient’s body.  The current is then raised or lowered to provide a suitable intensity and length of spark, after which the electrode is applied to the portion of the body to be treated.  The spark is drawn from the patient’s body, is disruptive in character, and is particularly suitable for various skin diseases, having also the advantage of the patient’s nutrition and general metabolism being benefitted by the auto-condensation which accompanies it.  In other words, it is both local and general in its effects.
   Taking the Blood Pressure.  As a knowledge of the patient’s blood pressure is vitally necessary to the physician using high frequency currents it is important that he should have an instrument for its rapid and accurate determination.  The instrument used for this purpose is called a sphygmomanometer and a number of satisfactory machines are on the market.  The diaphragm type is shown in Figs. 44 and 44b
   The mercury type is shown in Fig. 44a.  Its action depends on opposing the pressure of a column of mercury with the pressure of the blood in an artery.  For this purpose the brachial artery, in the arm above the elbow, is selected.
   A cuff or band containing a rubber sack is fastened around the arm above the elbow, with that part from which the rubber tube emerges lying in front over the artery.  Ordinarily the sleeve is rolled up before the band is applied, but if the clothing is thin this is unnecessary.  A small rubber hose runs from the cuff to the machine, which has a U-shaped tube containing mercury, with a gauge between.  The zero mark on the scale is placed on a level with the top of the mercury.
   A rubber bulb is attached by a small tube to the machine, and the physician holds this bulb in one hand, while with the other he keeps a finger on the pulse in the patient’s wrist.  The bulb is now compressed and immediately air fills the cuff and the column of mercury begins to rise.  The operator continues to slowly inflate the cuff until the pressure of the latter shuts off the blood in the brachial artery and the pulse can no longer be felt at the wrist.  When this occurs the pressure of the column of mercury has balanced the pressure of the blood in the artery and the reading on the scale opposite the top of the column is the patient’s blood pressure.
   In using the instrument it is customary to force the mercury a little above the point where the pulse ceases to be felt and then wait two or three seconds until the column settles to the point of the reappearance of the pulse.  By doing this one, two, or three times an absolutely accurate reading may be depended on.

Fig. 43 - Indirect Sparks.

   The scale reads from 0 to 300.  The normal is 120.  The numbers refer to millimeters of mercury.  A variation of 10 millimeters up or down would not necessarily imply abnormal pressure, but 140 or more would be presumptive of the presence of or tendency to arteriosclerosis.

Fig. 44 - Taking Blood Pressure with Diaphragm Type of Sphygmomanometer.
Fig. 44a - Taking Blood Pressure with Mercury Sphygmomanometer.

   Another instrument for accurately determining blood pressure is the tycos diaphragm type of instrument, shown in Fig. 44.
   This is not a mercury instrument, but the readings are obtained by indirect, internal pressure on sensitive diaphragm chambers, so sensitive indeed that every action of the heart is shown plainly by the hand on the dial, as the hand works co-incidently with the heart.
   With this instrument the observer can accurately determine complete blood pressure, by that we mean maximal or systolic; minimal or diastolic, and pulse pressure (the difference between the two).  This is not easy with a mercury instrument, because the great inertia of mercury renders it difficult to obtain a diastolic pressure, for mercury requires one and one-half seconds to recover itself, while in one second we have had one and one-fourth heart impulses, so you can see that mercury does not act quickly enough to accept the second impulse.  Diastolic pressure with a mercury machine may be obtained by the auscultatory method described later on.
   The minimal or diastolic pressure is fully as essential as the maximal or systolic, for without an exact diastolic to subtract from the systolic we cannot get the most important thing in blood pressure, that is the pulse pressure, for by pulse pressure alone can it be determined whether a pathological condition is compensated for or not.

Fig. 44b - Portable Outfit with Novel X-Ray tube for surface Treatment.

   The normal pulse pressure (difference between diastolic and systolic) should be from 20 to 55 millimeters.
   The determining of pulse pressure by those using the high frequency current is absolutely essential, for, as said before, by this we can tell whether a condition is compensated for, and whether the use of high frequency current is indicated or contraindicated.
   As an illustration, we will say that we have a case with a systolic pressure of 170, and a diastolic pressure of 140.  This shows, by subtracting one from the other, that the pulse pressure is 30, therefore normal.  No matter then if the systolic be 170, for the pulse pressure being normal shows that the condition is compensated (or the pulse pressure could not be normal), and in these cases any further reduction of systolic blood pressure must be accompanied by a corresponding decrease in diastolic pressure or compensation will be interfered with.
   Of course, if the systolic was reduced to 160 and the diastolic remained 140, compensation would still exist, but would be at its low limit, and the patient would probably not be as comfortable as with 165 or 170, with 140 as the diastolic.  If however, under auto-condensation both systolic and diastolic pressures decreased, if not always the same reduction, at least without the pulse pressure going below 20, the treatment may be persisted in until the systolic pressure is normal.
   Whenever the pulse pressure reaches 20 and stays there, after carefully giving one to three additional treatments auto-condensation should be abandoned.  It has been carried as far as it can be of benefit to the patient, no matter what the systolic pressure then may be, and I would suggest spinal sparks to raise it slightly, that pulse pressure may be at least 25.
   Where the systolic reading is high it sometimes happens that the pulse pressure will, when auto-condensation is employed, drop to 20, or even 18, but after a few days the diastolic will reduce enough to give an increased pulse pressure, and thereafter both systolic and diastolic keep reducing in proportion, in which case the treatment is kept up.  See further discussion and examples under Arteriosclerosis, Chapter VIII.
   There are two methods of determining blood pressure with the tycos type, which I have taken from Dr. Cowing’s book, “Blood Pressure Technique Simplified.”
   First, the method of oscillation.
   Place the bag over the arm with the two tubes well under the arm and over the brachial artery.  Wrap the remainder of the sleeve around the arm much the same as you would apply a bandage, tucking at least six inches of the sleeve under the last fold.  Then place the sphygmomanometer in one tube and the bulb in another and you are ready for reading.  Care should be taken not to put the sleeve on tight enough to cause any apprehensive feeling in the patient.  Place the fingers lightly over the radial artery and send the pressure in the cuff up to the point where the pulse disappears or is obliterated.  This is the systolic or maximal reading.
   It is desirable that the patient’s wrist be supported from below by the palm of the doctor’s hand, while the first and second fingers lie with their tips over the artery.  Thus the weight of the hand is prevented from shutting off the pulse too soon.
   Second, the method of auscultation.  This is, by far, the most practical method of accurately determining blood pressure, as the dangers of personal equation are greatly lessened.  See Fig. 44c.
   Bare the arm, adjust the sleeve well up (as above described), place the stethoscope over the brachial artery.  Now gradually inflate the bag, and the first and second sounds of the heart will become audible.  Increase the pressure in the bag to the point where all sounds cease.  At this point will be the exact systolic or maximal pressure.

Fig. 44c - Auscultation Method.

   Having obtained this, gradually release the air by means of the valve, and the first and second sounds of the heart will become apparent, increasing in volume as they approach the diastolic point, at which point the second sound will entirely disappear.
   The above method cannot be employed where aortic insufficiency exists or where there is a dilatation of the vessels.  These conditions being observed, when the pressure is first increased on the brachial, as soon as a slight pressure is placed on the artery, a pistol-shot tone is heard, and will continue with but little variation throughout the observation.  When this condition exists it is absolutely necessary to resort to the oscillatory method.  It is also necessary to use the method by oscillation when the pulse is feeble.
   Having now accurately determined both systolic and diastolic pressure, we compute the pulse pressure.
   Pulse pressure is obtained by subtracting the diastolic from the systolic, for example:
   Systolic pressure, 120; diastolic pressure, 90; the difference, pulse pressure, 30, and, as previously stated, it should not be less than 20, and would also indicate a pathological condition as probable if over 55.
   In about 7,000 cases Cowing obtained the following average normals:

   Children from 10 to 17, 85 to 110 mm.
   Adults from 21 to 40, 120 to 130 mm.
   Adults from 40 to 50, 120 to 135 mm.
   Adults from 50 to 60, 135 to 145 mm.

   It is well to remember that there is an ever increasing hardening of the arteries as one grows older, and a person of 65 or over can very easily have a blood pressure of 160 and still be a comparatively healthy individual.  At the same time if these changes were not taking place the blood pressure would remain the same, no matter what the age of the patient might be.  Female pressure is 10 mm. Lower than that of males.  Any blood pressures, however, between the ages of 21 and 50, lower than 100 or higher than 150,can safely be termed pathological cases.
   Leading life insurance companies now insist on the examiner taking the blood pressure.  Most of them reject applicants whose pressure is 160 or higher, whether any other reason is apparent or not; just as they do where the pulse is persistently above 90.
   An easy method of keeping the range of blood pressure in mind, which I have employed in my classes, is as follows:
   Consider 120 the normal.  At 20 above or below that is 140 or 100, the warning signal is out, and at 20 more either way (160 or 80) the brink of the precipice has been reached and a pathological condition, and probably a dangerous one, exists.
   It has been noted that enlargement of the heart or degeneration of the kidneys cause a comparatively high blood pressure and when both are present the pressure may be extraordinarily high, often (280-325), or higher than is provided for on many of the instrument scales.
   One observer reports a study of the blood pressure in seventy men.  At forty years of age the average pressure was 115; at sixty it was 135, and at eighty it was 150.
   Another physician found the average in 100 men to be a little over 118.
   An increased determination of blood to the surface of the body lowers the pressure, and, conversely, driving the blood from the surface raises the blood pressure.
   It is important that the sphygmomanometer be used, as in one series of 1,000 tests it was observed that abnormal pressure existed in many cases that a competent and experienced observer failed to detect without.
   In taking the systolic pressure I have occasionally found that just as I had determined the pressure there would be a sudden increase, running up 5 to 20 millimeters.  This I have concluded is due to a spasm of the artery, causing sudden contraction.
   Miscellaneous Suggestions.  When a resonator is employed in connection with an induction coil on the direct current and a mercury interrupter is used, if it is difficult or impossible to secure a steady spark in the spark-gap of the resonator, it is a sign that the mercury in the interrupter is dirty and needs cleaning.
   With this same apparatus, the spark may be made sharper by increasing the number of turns of wire in use in the coarse or primary coil of a resonator.  This increases the size of the solenoid and consequently its induction.  This is true of any Oudin resonator having the sliding rod to regulate the size of the coarse coil.
   When using vacuum tubes care should be exercised to prevent the connecting cord from touching the patient, as annoying sparks will result.  It is almost impossible to find a cord so well insulated that the high frequency current will not soon find its way through.
   Diathermy.  The fourth division of my classification of technique involves the methods known under the several terms, electro-coagulation, thermo-penetration, direct D’Arsonval current and diathermy.  The method of employment is given in Chapter XI.