War in Space, 1939 – II: “Space War Tactics” in Astounding Science Fiction, by Malcolm Jameson (November, 1939)


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Three months after the appearance of Willy Ley’s article “Space War” in the August, 1939 issue of Astounding Science Fiction, Malcolm Jameson penned (well, in all probability, he typed – remember typewriters?) a follow-up article of similar length and concept, but focused on a different aspect of spacecraft-to-spacecraft combat:  The actual tactics of battle.  Thus, Jameson – perhaps reflective of his background as a naval officer – accords attention to the maneuvers utilized by opposing spacecraft, only later in his article discussing weapons, and unlike Ley, being an advocate of “rocket torpedoes”.

Jameson’s article is supplemented by two diagrams which illustrate the trajectories of opposing spacecraft engaged in combat.  (You can see his signature at the lower right in each.)  In both diagrams – here limited to two dimensions, and viewed from “below” – the track of “our” spacecraft is on the left, and the enemy ship to the right. 

In the first diagram, our craft is on a straight trajectory, with the enemy ship taking an abrupt “right” turn at position “7”, the weapons employed by our spacecraft presumably being rocket-torpedoes. 

In the second diagram, the pair of spacecraft are on a converging trajectory, the weapons being mines as well as rocket-torpedoes.

Paralleling my post about Willy Ley’s article about space war, here are some general “take-aways” from Jameson’s article:

1) Military conflicts, regardless of the era or the nature of weapons employed, can be expected to follow the same general principles.  Thus, though “space” is by nature a setting different from arenas of battle in the traditional sense, the same concepts and assumptions can be expected to hold there, as well.

However, two primary differences stand out:  “Space” differs from taken-for-granted terrestrial settings (any planetary setting, really) in terms of its (apparently limitless) extent, and, the speed of the craft involved.  The implications and challenges of the latter, in terms of even the nominal possibility of maneuver, as well as locating, tracking, aiming, and firing at enemy craft, cannot be underestimated.

2) Given the speed of combat between spacecraft, gunnery computations (like Willy Ley’s August article, Jameson’s analysis is based on the assumption that spacecraft armament will comprise some form of weaponry firing either simple mass weapons or explosive projectiles, rather than an energy weapon of unknown design and function) will demand the use of a “differentia calculator”.  Though he does not elaborate, Jameson seems to have been either anticipating or conceptualizing such a device as ENIAC (Electronic Numerical Integrator and Computer), the existence of which was announced to the public ten months after his death.  

3)  The spacecraft’s armament is simple, whether by the standards of the late ‘thirties or 2021:  The craft shoots projectiles comprised of “a simple sphere of meteoric iron”.  Due to the velocities involved, explosives are entirely unnecessary: The momentum of such a projectile is entirely adequate to damage or destroy an enemy spacecraft.

4) A substantial portion of Jameson’s text – specifically pertaining to Figure 1 – pertains to the manner in which “our” spacecraft will locate, identify, and track the enemy vessel, and, plot a firing trajectory for its weapons.  Here, Jameson description of the craft’s “plotting room,” the “most vital spot in the ship,” seems (unsurprisingly, given his naval background) akin to a description of a battleship or aircraft carrier’s combat information center, “the counterpart of the brain”.    

Then, his essay gets really interesting, for – in the context of describing the tracks of two spacecraft engaged in combat, as diagrammed in Figure 2 – he postulates about the nature of space-borne rangefinders and target-bearing transmitters, suggesting for the former determining distance – “sounding” by radio waves – and the latter something akin to a thermoscope, or simply put, a device showing changes in temperature, against a given background. 

In other words, he seems to have been respectively anticipating both radar, and, what is now known as IRST: Infrared Search and Track.      

5) Interestingly, unlike Willy Ley, Jameson is also an advocate of the use of some form of what he dubs “rocket torpedoes” rather than shells, due to the latter’s “advantage of auto-acceleration” and the “ability to build up speed to any desired value after having been launched,” versus the delay inherent to the sequence of events involved in the the actual firing and movement of a shell from a gun.  Of course, even assuming the enemy vessel is attacked with “rocket torpedoes”, such devices – in the context and era of Jameson’s article – would have no internal guidance or tracking system of their own, their “flight” path being entirely dependent on course adjustments of the firing platform – “our” spacecraft – itself.      

5) Where mentioned, I’ve included conversions of given velocities (“miles per second”) to velocities per hour, in both English and Metric systems, the former in statue miles.  These are denoted by brackets.  (e.g., [90,000 mph / 144,840 kph]).

As in the post covering Ley’s article, the most notable passages of the text are italicized and in red, like these last twelve words in this sentence.  The post concludes with links to a variety of excellent videos covering spacecraft-versus-spacecraft battles, and “space war”, in greater detail, in light of (quite obviously!) contemporary knowledge.   

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You can read the Wikipedia article about Malcolm Jameson here, while the Internet Speculative Fiction Database compilation of his writing can be found here

Jameson’s memorial tribute (I guess penned by John W. Campbell, Jr.?) from the July 1945 issue of Astounding, follows:

MALCOLM JAMESON
December 21, 1891 – April 16, 1945

Malcolm Jameson, a man possessed of more shear courage than most of us will ever understand, died April 16, 1945, after an eight-year writing career, initiated when cancer of the throat forced him to give up the more active life he wanted.  Any author can tell you that you can’t write good stuff when you’re feeling sick.  Jamie never quite understood that – perhaps because he began when he did.  X-ray and radium treatment controlled the cancer for a time, but only at a price of permanent severely bad health.

He sold his first story to Astounding in 1938.  [“Eviction by Isotherm“, August, 1938.]  That was followed by such memorable and sparklingly light stories as “Admiral’s Inspection,” the whole Commander Bullard series, and his many other stories in UNKNOWN WORLDS.

The man who could accomplish that under the conditions imposed on him was not of ordinary mold.

The Commander Bullard series grew out of Jameson’s own experiences as a Lieutenant in the United States Navy from 1916 till his retirement in 1927.  He had much to do with the development of modern naval ordnance; his work is fighting in this war, though he himself was not permitted to do so.

He is survived by his wife, his daughter, Corporal Vida Jameson, of the WAC, his son, Major Malcolm Jameson, in the Infantry and now overseas, and his brother, House Jameson, better known as “Mr. Aldrich” of the “Aldrich Family” program.

The Editor.

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You’ll notice that Hubert Rogers’ iconic depiction of a space fleet control center (for E.E. Smith’s “Gray Lensman”) as the cover of the November, 1939 issue of Astounding, appears below.  Further down in the post are two interior illustrations – from the November, 1941, and February, 1948 issues of Astounding, in which Rogers created views of the same scene for Smith’s “Second Stage Lensman” and “Children of the Lens”, respectively.  (The image of the control center in the 1948 issue was scanned from an original copy, and photoshopifically “niced up” to bring out the details, for this post.)  You can view other images of this nature, and more, at my brother blog, WordsEnvisioned.       

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And so, on to Malcolm Jameson’s “Space War Tactics” from the month of November, in the year 1939…

SPACE WAR TACTICS

Expanding on Willy Ley’s recent article, Jameson brings out some important details – not the least of which is that a space battle fleet gets one shot at the enemy in months of maneuvering!

By Malcolm Jameson

Illustrated by Malcolm Jameson

Astounding Science Fiction
November, 1939

I.

Ship to Ship Engagement

A working knowledge of the game of chess is a useful adjunct in understanding the art of war.  War is not a series of haphazard encounters hut a definite understanding governed by principles that never change, however much the weapons and uniforms and the colors of the flags may.  Like chess it is a continuing struggle between two opponents, each trying to estimate the strength of the other and to divine his purposes and most probable objective, and what his next move will be.  It is a marauding and movement of forces, a series of threats and feints, of advances and withdrawals, punctuated by sharp conflict as one or the other forces the issue.

As the rules of chess govern the movement of each piece, so does the field of operations in war, whether it is rocky terrain or swampy, the open sea or the cloud-streaked skies, or the vast reaches of space itself.  Tactics, and in a measure the weapons, are rigidly determined by the controlling environment.

We can, therefore predict with some assurance the general nature of space warfare, for we already know something of the properties of the void and what characteristics ships that traverse it arc likely to have.  With such ships and in such a theater of operations, we have only to apply the principles of warfare developed by men through centuries of strife to arrive at an approximation of the tactics they will use.  We can be fairly certain of the kind of weapons and instruments they will have, for the very advent of spaceships is presumptive of continued advance in science along much the same lines we have already come.

There are two great factors in space warfare that will set it off sharply from anything else in human experience, and those two factors will modify fighting-ship types, strategy and tactics profoundly. They are: (a) the extent of space, and (b) the tremendous speed of the vessels.

At the risk of boring those who have already read and thought a good deal about travel in space and who feel that they long ago formed a satisfactory idea of what the limitless reaches of the void are like, I want to dwell a moment on the subject of the vastness of space.  It deserves all the emphasis we can give it.

Psychologists assert that it is beyond the capacity of the human mind to conceive of quantities, extents or durations beyond rather close limits.  We may nod understandingly at hearing mention of a billion-dollar appropriation, but we grasp the idea solely because we are thinking of those billion dollars as a unit sum of money.  If we tried to visualize them as coins we would fail utterly.  The mind cannot picture ten hundred thousands of thousands of silver disks.  “Many” is the best it can do – there are too many dollars there for one mindful.  And so it is with distance.

It has been my good fortune to have traveled extensively; I have crossed oceans as navigator, stepping off the miles made good each day or watching them slide by under the counter.  Thus I have a hazy notion of the size of the Earth – it is oppressively huge.  What, then, of the two or three million-mile straightaway covered in a single day’s run of a rocket-ship – represented by a quarter-inch pencil mark on the astragator’s chart of the ecliptic?  The Earth he left but yesterday had already dwindled to a small bright disk and before the week is over it will be seen only as a brilliant blue star.  In that incredibly vast celestial sphere in which lie is floating – stretching as it does without limit before, behind and to every side, above and below – where and how can we hope to find his enemy?

For even if he passed another ship close aboard, he would not so much as glimpse it.  Speeds in space are as stupendous as the spaces they traverse.  Needing seven miles per second to escape the Earth and another twenty to make any reasonable progress between the planets, even the slowest vessels will have speeds of twenty-five miles per second [90,000 mph / 144,840 kph].  Warships. presumably. according to type, will have correspondingly higher speeds – perhaps as high as fifty miles per second [180,000 mph / 289,682 kph … or, 0.000268 c] for the faster scouts.

Speeds of that order are as baffling to the imagination as the depths of the void.  When we recall that the fastest thing most of us are familiar with is the rifle bullet, whizzing along at a lazy half-mile per second [1,800 mph / 2,897 kph], we see that we do have a yardstick.  The ships mentioned above proceed at from fifty to one hundred times that fast – invisible, except under very special circumstances.  It is barely possible, we know, for a quick eye to pick up twelve-inch shells in flight if he knows just where, when and how to look, but a momentary glimpse is all he gets.

When we talk of gunfire or any other means of offense, we have to bear these dizzy speeds firmly in mind.  The conclusion is irresistible that scouting, tracking, range finding and relative bearings will all be observed otherwise than visually.  Even on the assumption of attack from the quarter, the most obvious approach – and for the same reason that aviators “get on the tail” – the overtaking vessel must necessarily have such an excess of speed that the visual contact can last but a few seconds.  Each of the combatants must compute the other’s course from blind bearings and ranges and lay their guns or point their torpedo tubes by means of a differentia calculator.

However, in this blind tracking there is one peculiarity of these ships that while it is in one sense a source of danger to them, is of distinct assistance.  In the fleeting minutes of their contact, neither can appreciably alter course or speed!  This is a point that writers of fiction frequently ignore for the sake of vivid action, but nevertheless it is an unavoidable characteristic of the [e]ther-borne [?!] ship.

The human body can withstand only so much acceleration and the momentum these vessels carry has been built up, hour after hour, by piling increment of speed on top of what had been attained before.  In space there is no resistance.  Once the rockets are cut, the ship will soar on forever at whatever velocity she had at the moment of cutting.  Her master may flip her end over end and reverse his acceleration, but his slowing will be as tedious and cautious as his working up to speed.  Jets flung out at right angles merely add another slight component to the velocity, checking nothing.

Rocket experts have stated that an acceleration of one hundred feet per second per second can be withstood by a human being – perhaps one hundred and fifty in an emergency.  The master of a vessel proceeding at forty miles per second [144,000 mph / 231,745 kph] applying such an acceleration at right angles would succeed in deflecting his flight about one hundred miles by the end of the first minute, during which he will have run twenty-four hundred – a negligible turn, if under fire.  Applied as a direct brake, that hundred miles of decreased velocity would slow him by one twenty-fourth – obviously not worth the doing if the emergency is imminent.

With these conditions in mind, let us imagine a light cruiser of the future bowling along at forty miles per second on the trail of an enemy.  The enemy is also a cruiser, one that has slipped through our screen and is approaching the earth for a fast raid on our cities.  He is already decelerating for his prospective descent and is thought to be about one hundred and fifty thousand miles ahead, proceeding at about thirty-five miles per second [126,000 mph / 202,777 kph].  Our cruiser is closing on him from a little on his port quarter, and trying to pick him up with its direction finders.

So far we have not “seen” him.  We only know from enciphered code messages received several days ago from our scouting force, now fifty millions astern of us, that he is up ahead.  It would take too long here to explain how the scouts secured the information they sent us.  The huge system of expanding spirals along which successive patrols searched the half billion cubic miles of dangerous space lying between us and the enemy planet is much too intricate for brief description.  It is sufficient for our purposes that the scouts did detect the passage of the hostile cruiser through their web and that they kept their instruments trained on him long enough to identify his trajectory.  Being neither in a position to attack advantageously nor well enough armed – for their function is the securing of information, and that only – they passed the enemy’s coordinates along to us.  This information is vital to us, for without it the probability of contact in the void is so remote as to be nonexistent.

The ship in which we are rushing to battle is not a large one.  She is a bare hundred meters [328 feet] in length, but highly powered.  Her multiple rocket tubes, now cold and dead, are grouped in the stern.  We have no desire for more speed, having all that is manageable already, for after the few seconds of our coming brush with the enemy our velocity is such that we will far overrun him and his destination as well.  It will require days of maximum deceleration for us to check our flight and be in a position to return to base.

Our ship’s armament, judged by today’s standards, will at first sight appear strangely inadequate.  Our most destructive weapon is the “mine,” a simple sphere of meteoric iron about the size of a billiard ball, containing no explosive and not fused.  The effectiveness of such mines depends upon the speed with which they are struck by the target ship – no explosive could add much to the damage done by a small lump of iron striking at upward of thirty miles a second.  Then there will he torpedo tubes amidships, and perhaps a few guns, but it may lie well to postpone a discussion of the armament until we have examined the conditions at the place of battle.

Although we know in a general way where the enemy is and where he is going, before we close with him we must determine his course and speed very accurately, for our ability to hit him at all is going to depend upon extremely nice calculations.  Our speeds are such that angular errors of so much as a second of arc will be fatal, and times must be computed to within hundredths of seconds.

This falls within the province of fire-control, a subject seldom if ever mentioned by fiction writers.  There is no blame to be attached to them for that, for the problems of fire-control are essentially those of pure mathematics, and mathematics is notoriously unthrilling to the majority of readers.  Yet hitting with guns – or even arrows, though the archer solves his difficulties by intuition – requires the solution of intricate problems involving the future positions and movements of at least two bodies, and nothing more elementary than the differential calculus will do the trick.  In these problems interior ballistics, for all its interesting physics, boils down to a single figure – the initial velocity of the projectile, while exterior ballistics evaporates for the most part the moment we propel our missile into a gravityless vacuum.  In space we are to be concerned with the swiftly changing relationship of two rapidly moving vessels and the interchange of equally swift projectiles between them, the tracks of all of them being complicated curves and not necessarily lying in a plane.

In its simplest statement the problem of long-range gunnery is this: where will the enemy be when my salvo gets there?  For we must remember that even in today’s battles the time the projectile spends en-route to its target is appreciable – fully a minute on occasion, at sea, during which the warship fired upon may move as much as half a mile.  Under such circumstances the gunner does not fire directly at his target, but at the place it is going to be.  That requires very accurate knowledge of where the enemy is headed and how fast he is moving.

At sea that is done by observing successive bearings and ranges and plotting them as polar coordinates, bearing in mind that the origin is continuously shifting due to the ship’s own motion.  This work of tracking – the subsequent range-keeping and prediction of future ranges and bearings – is done in our times in the plotting room.  This is the most vital spot in the ship, for if her weapons may be likened to fists and her motive power to legs, her optical and acoustical instruments to eyes and ears, then the plotting room is the counterpart of the brain.  There all the information is received, corrected, digested, and distributed throughout the ship.  Without that co-ordination and direction the ship would be as helpless as an idiot.

Well, hardly that helpless today.  Our individual units, such as turret crews, can struggle on alone, after a fashion.  But not so with the ship of the future.  There the plotting room is everything, and when it is put out of commission, the ship is blind and paralyzed.  It will, of course, be located within the center of the ship, surrounded by an armored shell of its own, and in there will also be the ship control stations.

The best way to approach the problems our descendants will have to face is to consider a simple problem in tracking that our own warships deal with daily.  It is an absurdly simple one compared to the warped spirals to be handled in space warfare, but it will serve to illustrate the principle.  In Fig. 1. it is shown graphically, but in actual practice the elements of the problem are set up on a motor-driven machine which thereupon continuously and correctly delivers the solutions of problems that would take an Einstein minutes to state.  As the situation outside changes, corrections are cranked into the machine, which instantly and uncomplainingly alters its calculations.

In the figure we have the tracks of two ships, ours the left-hand one.  For the sake of clarity and emphasis I have made the ratio of speeds three to one, but the same trends would be shown at the more usual ratio of, say, 20:19

At positions “1,” “2,” “3” and so on, we observe the range and hearing of the target, and plot them.  By noting the differences between successive readings and the second differences between those, we soon have an idea of the type of curve the rates of changes would plot into.  In a short time we can also note that the rates themselves are changing at a certain rate.  This is a rough sort of differentiation – by inspection – and to one familiar with such curves these trends have a definite meaning.

For example, it is apparent that the series of observed angles “Beta” are steadily opening, signifying that we are drawing past the target.  Any sudden alteration of the second differences, such as occurs at “8,” at once indicates a change of condition on the part of the enemy.  He has either turned sharply away or slowed to half speed, for the bearing suddenly opens nearly two degrees more than the predicted beating.  We learn which by consulting our ranges.  It could be a combination of changed course and changed speed.

The ranges during the first seven lime-intervals have been steadily decreasing, although the rate of decrease has been slowing up, indicating we are approaching the minimum range.  At “8,” though, the range not only fails to decrease, but the rate of change actually changes sign.  We know without doubt that the enemy has turned away.

The importance of having the machine grind out predicted bearings and ranges, aside from the desirability of speed and accuracy, is that at any moment smoke, a rain squall, or intervening ships may obscure the target.  In that event the gunners need never know the difference – their range and bearing indicators arc ticking away like taximeters, fed figures by the controlling range-keeper.  It would not have mattered if sight had been lost of the enemy at “4”; the gun- fire would have been just as accurate up to the time he changed course as if they had the target in plain sight, t

As a matter of fact, the guns are not pointed at the target at all, but in advance of it, as is shown in Fig. 1 (a), both range and bearing being altered to allow for the forward movements of the target while the shells are in the air.  The projectiles may be regarded as moving objects bandied on a “collision course” with regard to the enemy vessel.

Speaking of collision courses, it is an interesting property of relative bearings that when the bearing remains constant – except in the special case of the vessels being on parallel courses at identical speeds – the vessels will eventually collide, regardless of what their actual courses and speeds are.  Hence, from the time the shots of the salvo left their guns – Fig. 1 (a) – until they struck their target, the target bore a constant angle of thirteen degrees to the right of the nose of the shells.  (This knowledge has some utility in estimating the penetration of armor at the destination.)

In the example above, all the movement can be regarded as taking place in a plane; the ships follow straight courses and they maintain constant speeds.  Our terrestrial problems are in practice much complicated by zigzagging, slowing down and speeding up, but at that they are relatively child’s play compared to what the sky-warrior of the future must contend with.

His tracks are likely to be curved in three dimensions, like pieces of wire hacked out of a spiral bed spring, and whether or not they can be plotted in a plane, they will nowhere be straight.  Moreover, whatever changes of speeds occur will be in the form of steady accelerations and not in a succession of flat steps linked by brief accelerations such as we know.  Computing collision courses between two continually accelerating bodies is a much trickier piece of mathematical legerdemain than finding the unknown quantities in the family of plane trapeziums shown in Fig. I.  Yet projectiles must be given the course and speed necessary to insure collision.

The gunnery officer of the future is further handicapped by rarely ever being permitted a glimpse of his target, certainly not for the purpose of taking ranges and bearings.  In the beginning of the approach the distances between the ships is much too great, and by the time they have closed, their relative speed will generally forbid vision.

Since optical instruments are useless except for astrogational purposes, his rangefinders and target-bearing transmitters will have to be something else.  For bearings, his most accurate instrument will probably be the thermoscope – an improved heat-detector similar to those used by astronomers in comparing the heat emission of distant stars.  It will have a spherical mounting with a delicate micro-vernier.  A nearby spaceship is sure to radiate heat, for it is exposed constantly to full sunlight and must rid itself of the excess heat or its crew will die.  Once such a source of heat is picked up and identified, it can be followed very closely as to direction, although little can be told of its distance unless something is known of its intrinsic heat radiation.

Ranges will probably be determined by sounding space with radio waves, measuring the time interval to the return of reflected waves.  It is doubtful whether this means will have a high degree of accuracy much beyond ranges of one light-second on account of the movement of the two vessels while the wave is in transit both ways.  At long range the need for troublesome corrections is sure to enter.

Such observations, used in conjunction with one another, should give fairly accurate information as to the target’s trajectory and how he bears from us and how far he is away.  This data will be fed into a tracking and range-keeping machine capable of handling the twisted three-dimensional curves involved, and which will at once indicate the time and distance of the closest point of approach.  Both captains will at once begin planning the action.  They may also attempt to adjust their courses slightly, but since the rockets evolve great heat, neither can hope to keep his action from the knowledge of the other owing to the sensitiveness of the thermoscopes.

The rangekeeping instrument suggested, while far surpassing in complexity anything we know of today, will represent a much smaller technical advance than the rockets which drive the ships that house them.  We already have similar machines, so that their counterparts of the future would seem much less mysterious to us than, say, the Walschaert’s valve gear to Hero or Archimedes, or the Jacquard loom to the weavers of the Gobelin tapestries.

Assuming we have, by observation and plotting, full knowledge of the enemy’s path and have come almost into position to commence the engagement, we find ourselves confronted once more with the two overwhelming factors of space warfare – great distance and immense speeds – but this time in another aspect.  We have come up close to our foe – in fact we are within twenty seconds of intersecting his trajectory – and our distance apart is a mere four hundred miles [643 km].  It is when we get to close quarters that the tremendous problems raised by these lightning-like speeds manifest themselves most vividly.

Look at Fig. 2.

The elapsed time from the commencement of the engagement until the end is less than twenty seconds.  Our ship is making forty miles per second, the other fellow is doing thirty-three.  We will never be closer than fifty miles, even if we regard the curves as drawn as being in the same plane.  If one rides over or below the other, that minimum range will be greater.  What kind of projectile can cross the two or three hundred miles separating the two converging vessels in time to collide with the enemy?  Shooting cannon with velocities as low as a few miles per second would be like sending a squadron of snails out from the curb to intercept an oncoming motorcycle – it would be out of sight in the distance before they were well started.

Projectiles from guns, if they were to be given velocities in the same relation to ships’ speeds that prevail at present, would have to be stepped up to speeds of three to four thousand miles per second!  A manifest impossibility.  It would be difficult, indeed, to hurl any sort of projectile away from the ship at greater initial velocities than the ship’s own speed.  Such impulses, eighty times stronger than the propelling charge of today’s cannon, would cause shocks of incredible violence.  It follows from that that an overtaken ship is comparatively helpless – unless she is in a position to drop mines – for whatever missiles she fires have the forward inertia of the parent ship and will therefore be sluggish in their movement in any direction but ahead.

Another difficulty connected with gunfire is the slowness with which it comes into operation.  This may seem to some to be a startling statement, but we are dealing here with astonishing speeds.  When the firing key of a piece of modern artillery is closed, the gun promptly goes off with a bang.  To us that seems to be a practically instantaneous action.  Yet careful time studies show the following sequence of events: the primer fires, the powder is ignited and burns, the gases of combustion expand and start the shell moving down the tube.  The elapsed time from the “will to fire” to the emergence of the projectile from the muzzle is about one tenth of a second.  In Fig. 2 our target will have moved more than three miles while our shell is making its way to the mouth of the cannon!  It looks as if guns wouldn’t do.

I come to that conclusion very reluctantly, for I am quite partial to guns as amazingly flexible and reliable weapons, but when we consider that both powders and primers vary somewhat in their time of burning, there is also a variable error of serious proportions added to the above slowness.  It is more likely that the rocket-torpedoes suggested by Mr. Willy Ley in a recent article on space war will be the primary weapon of the future.  They have the advantage of auto-acceleration and can therefore build up speed to any desired value after having been launched.

The exact moment of their firing would have to be computed by the tracking machine, as no human brain could solve such a problem in the time allowed.  But even assuming machine accuracy, great delicacy in tube-laying and micro-timing, the chances of a direct hit cm the target with a single missile is virtually nil.  For all their advanced instruments, it is probable that all such attacks will be made in salvos, or continuous barrages, following the time-honored shotgun principle.  For the sake of simplicity, only two such salvos are shown on the diagram, but probably they would be as nearly continuous as the firing mechanisms of the tubes would permit.  Any reader with a flair for mathematics is invited to compute the trajectories of the torpedoes.  The ones shown were fired dead abeam in order to gain distance toward the enemy as rapidly as possible.

It is desirable that these torpedoes should vanish as soon as practicable after having overrun their target.  To that end their cases are made of thin magnesium, and between the head and the fuel compartment is a space filled with compressed oxygen and a small bursting charge The tip of the head is loaded with liquid mercury.  Such a massive projectile would penetrate any spaceship with ease, but if it missed it would burst as soon as the fuel supply was spent and then consume itself in brilliant flame, thus avoiding littering the Spaceways with dangerous fragments.

Spotting, as we know it, would be impossible, for the target would be invisible.  Hits would have to be registered by the thermoscope, utilizing the heat generated by the impact.  The gunnery officer could watch the flight of his torpedoes by their fiery wakes, and see his duds burst; that might give him an idea on which side of the enemy they passed in the event the thermoscopes registered no hits.

If there were guns – and they might be carried for stratosphere use – they could be brought into action at about “15,” firing broad on the starboard quarter.  The shells, also of self-destroying magnesium, would lose some of their forward velocity and drift along in the wake of the ship while at the same time making some distance toward the oncoming enemy.  These guns would be mounted in twin turrets, one on the roof and the other on the keel, cross-connected so that they would be trained and fired together.  It the ships center of gravity lay exactly between them, their being fired would not tend to put the ship into a spin in any direction.  What little torque there might be, due to inequalities in the firing charge, would be taken care of by the ship’s gyro stabilizer, an instrument also needed on board to furnish a sphere of reference so that the master could keep track of his orientation. 

If upon arriving at point “16” the enemy were still full of fight and desperate measures were called for, we could lay down mines.  These hard little pellets would be shot out of mine-laying tubes clustered about the main driving jets.  They would be shot out at slight angles from the fore-and-aft line, and given a velocity exactly equal to the ship’s speed, so that they would hang motionless where they were dropped.  Being cheap and small, they could be laid so thickly that the enemy could not fail to encounter several of them.  If she had survived up to this point, the end would come here.

The end, that is, of the cruiser as a fighting unit.  Riddled and torn, perhaps a shapeless mass of tangled wreckage, she would go hurtling on by, forever bound to her marauding trajectory.  The first duty of our cruiser would be to broadcast warnings to the System, reporting the location of its own mine-field, and giving the direction taken by the shattered derelict.  Sweepers would be summoned to collect the mines with powerful electromagnets, while tugs would pursue and clear the sky of the remnants of the defeated Martian.

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Illustration by Hubert Rogers, for “Second Stage Lensman – Part I“, by Edward E. Smith, PhD., from Astounding Science Fiction, November, 1941, page 35.  (Cover also by Rogers.)

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Illustration by Hubert Rogers, for “Children of the Lens – Conclusion“, by Edward E. Smith, PhD., from Astounding Science Fiction, February, 1948, page 122.  (Cover by Alejandro Canedo)

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— References and Related Readings —

Malcolm R. Jameson, at Wikipedia

Malcolm R. Jameson, at International Science Fiction Database

Hubert Rogers, at SciFiGuy

Hubert Rogers, at International Science Fiction Database

Space War, at Atomic Rockets

Vacation in the Golden Age of Science Fiction, by Jamie Todd Rubin

Warfare in Science Fiction, at Technovology

Weapons in Science Fiction, at Technovology

— Here’s a book —

Wysocki, Edward M., Jr., An ASTOUNDING War: Science Fiction and World War II, CreateSpace Independent Publishing Platform, April 16, 2015

— Lots of Cool Videos —

Because ScienceKyle Hill

Why Every Movie Space Battle Is Wrong ((at Nerdist) 5/11/17)

The Truth About Space War (4/12/18)

Curious DroidPaul Shillito

Electromagnetic Railguns – The U.S Military’s Future Superguns – 200 mile range Mach 7 projectiles (11/4/17)

Will Directed Energy Weapons be the Future? (6/12/20)

Generation Films – Allen Xie

Best Space Navies in Science Fiction (2/10/20)

5 Most Brilliant Battlefield Strategies in Science Fiction (5/8/20)

5 Things Movies Get Wrong About Space Combat (5/12/20)

6 More Things Movies Get Wrong About Space Battles (5/28/20)

Why “The Expanse” Has the Most Realistic Space Combat (6/21/20)

It’s Okay To Be SmartJoe Hanson

The Physics of Space Battles (9/22/14)

PBS SpaceTimeMatt O’Dowd

The Real Star Wars (7/19/17)

5 Ways to Stop a Killer Asteroid (11/18/15)

 Science & Futurism with Isaac Arthur (SFIA) – Isaac Arthur

Space Warfare (11/24/16)

Force Fields (7/27/17)

Interplanetary Warfare (8/31/17)

Interstellar Warfare (3/8/18)

Planetary Assaults & Invasions (5/17/18)

Attack of the Drones (9/13/18)

Battle for The Moon (11/15/18)

The Infographics Show

What If There Was War in Space? (12/23/18)

Railguns and More! – The Battle of Thoth Station, in “The Expanse”

Rocinante Attack on Thoth Station (Episode “Doors & Corners”) “The Expanse”, Season 2, Episode 2 (Air Date 2/1/17), at DailyMotion

List of “The Expanse” Episodes, at Wikipedia

The Age of Science: Computer Memory, in Astounding Science Fiction – February, 1949

The preeminent science-fiction magazine of the mid-twentieth century was Astounding Science Fiction, which rose to prominence under the editorial reign of John W. Campbell, Jr.  First published in January 1930 as Astounding Stories of Super Science, the magazine has continued publication under the leadership of several editors and through various title changes, now being known as Analog Science Fiction and Fact.

Though by definition and nature a science fiction publication, Astounding (akin to its post-WW II counterparts and rivals Galaxy Science Fiction, and, The Magazine of Fantasy and Science Fiction (“F&SF”)) also published non-fiction material.  Such non-fiction material included leading editorials, book reviews, and letters, as well as articles – typically, one per issue – about some aspect of the sciences.  As in any serial publication, the nature of this content reflected the opinions and interests of the magazine’s readers, and, the intellectual and cultural tenor of the times.

A perusal of science articles in Astounding from the late 1940s reveals a focus on aerodynamics, astronomy, atomic energy, chemistry (organic and inorganic), computation, cybernetics, data storage, electronics, meteorology, physics, and rocketry.  (Biology it seems, not so much!)  Viewed as a whole, these subject areas  – in the realm of the “hard sciences” – reflect interests in space travel (but of course!), the frontiers of physics, information technology, and the creation and use of new energy sources.

Let’s take a closer look.

Here are the (non-fiction) science articles that were published in Astounding Science Fiction in 1949:

January: “Modern Calculators” (Digital and analog calculation), by E.L. Locke; pp. 87-106

February: “The Little Blue Cells” (The “Selectron” data storage tube), by J.J. Coupling; pp. 85-99

March: “The Case of the Missing Octane” (Chemistry of petroleum and gasoline), by Arthur Dugan; pp. 102-113 (Great caricatures by Edward Cartier!)

April: “9 F 19” (Hydrocarbons), by Arthur C. Parlett; pp. 46-162

May: “Electrical Mathematicians” (Machine (electronic) calculation), by Lorne MacLaughlan; pp. 93-108

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June: “The Aphrodite Project” (Determining the mass of the planet Venus), by Philip Latham; pp. 73-84. (Intriguing cover art by Chesley Bonestell.)

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July: “Talking on Pulses” (Electronic transmission of human speech and other forms of communication), by C. Rudmore; pp. 105-116.

August: “Coded Speech” (Electronic speech; noise reduction), by C. Rudmore; pp. 134-145

September: “Cybernetics” (Review of Norbert Wiener’s book by the same title), by E.L. Locke; pp. 78-87

October – First article: “Chance Remarks” (Communication research), by J.J. Coupling; pp. 104-111

October – Second article: “The Great Floods” (Review of great floods in human history), by L. Sprague de Camp; pp. 112-120

November: “The Time of Your Life” (Time; Determining the length of the earth’s day), by R.S. Richardson; pp. 110-121

December – First article: “Bacterial Time Bomb“, by Arthur Dugan; pp. 93-95

December – Second article:  “Science and Pravda“, by Willy Ley; pp. 96-111

Regardless of the topic, a notable aspect of the non-fiction science content of Astounding (likewise for Galaxy and F&SF) is that mathematics – in terms of equations and formulae, let alone Cartesian graphs – was kept to a minimum, if not eschewed altogether.  Science articles largely relied upon text to communicate subject material, and often included photographs (especially for issues published during the latter part of the Second World War) and diagrams as supplementary material. 

One such example – from February of 1949 – is presented below, in the form of J.J. Coupling’s article “The Little Blue Cells”. 

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This issue features great cover art by Hubert Rogers for Jack Williamson’s (writing under the pen-name “Will Stewart”) serial “Seetee Shock”.  The cover symbolizes adventure and defiance in the face of danger, by incorporating a backdrop of warning and admonition (“YOU WERE NOT EVOLVED FOR SPACE”; “BACK ADVENTURER”, and more) around the figure of a space-suited explorer, while cleverly using extremes of light and dark and a sprinkling of stars to connote “outer space”.  Like much of Rogers’ best work, symbolism is as important as representation.  (You can enjoy more of Rogers’ work at my brother blog, WordsEnvisioned.)

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    Coupling’s article is notable because it addresses a subject frequently addressed by Astounding, with continuing and likely indefinite relevance: recording, storing, preserving, and accessing information – computer memory.

      The article focuses on Dr. Jan A. Rajchman’s – then – newly developed “Selectron Tube”, which was developed in the late 1940s at RCA (Radio Corporation of America) and about which extensive and rich literature is readily available, particularly at Charles S. Osborne’s wesbite.  As implied and admitted by Coupling’s article, even at the time of the device’s invention there was ambivalence about its long-term economic and technical viability, despite its functionality and innovative design. 

     An image of a Selectron Tube, from Giorgio Basile’s Lamps & Tubes, is shown below.  (Scroll down to end of post for a photograph showing a Selectron Tube in the hands of its inventor, illustrating its relative size.)

      Eventually, the initial, 4,096-bit storage capacity Selectron Tube proved to be more difficult to manufacture than anticipated, and the concept was re-designed for a 256-bit storage capacity Tube.  To no avail.  Both tube designs were superseded by magnetic core memory in the early 1950s. 

     As for J.J. Coupling?  Well…(!)…this was actually the nom de plume of Dr. John R. Pierce, a CalTech educated engineer, who had a long and rich literary career, writing for Astounding, Analog, and other publications.  His lengthy oeuvre is listed at The Internet Speculative Fiction Database.

     Today, Dr. Pierce’s “The Little Blue Cells” opens a window onto the world of information technology and scientific literature – for the general public – from over six decades gone by.  His article, with accompanying illustrations, is presented below.

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THE LITTLE BLUE CELLS
By J.J. COUPLING

The most acute problem in the design of a robot, a thinking machine, or any of the self-serving devices of science-fiction is memory.  We can make the robot’s body, its sensory equipment, its muscles and limbs.  But thinking requires association of remembered data; memory is the essential key.  So we present the Little Blue Cells!

Most of the robots I have met have been either man-sized androids with positronic brains to match, or huge block-square piles of assorted electrical junk.  The small, self-portable models I admire from a distance, but I feel no temptation to speculate about their inner secrets.  The workings of the big thinking machines have intrigued me, however.  It used to be that I didn’t know whether to believe in them or not.  Now, the Bell Laboratories relay computer, the various IBM machines and the Eniac are actually grinding through computations in a manner at once superhuman and subhuman.  With the other readers of Astounding I’ve had a sort of inducted tour through the brain cases of these monsters in “Modern Computing Devices” by E.L. Locke.  I’m pretty much convinced.  It’s beginning to look as if we’ll know the first robot well long before he’s born.

Perhaps some readers of science fiction can look back to the old, unenlightened days and remember a prophetic story called, I believe, “The Thinking Machine.”  The inventor of that epoch had first to devise an “electronic language” before he could build his electrical cogitator.  The modern thinking machine of the digital computer type comes equipped with a special electronic alphabet and vocabulary if not with a complete language.  The alphabet has the characters off and on, or 0 and 1, the digits of the binary system of enumeration, and words must certainly be of the form 1001-110—and so on.  We may take it from Mr. Locke that somewhere in the works of our thinking machine information will be transformed into such a series of binary digits, whether it be fed in on paper tape or picked up by an electronic eye or ear.  The machine’s most abstruse thought, or its fondest recollection – if such machines eventually come to have emotions – will be stored away as off’s and on’s in the multitudinous blue cells of the device’s memory.

I’m sure that I’m right in describing the memory cells of the machine as multitudinous and little – that is, if it’s a machine of any capabilities at all.  To describe them as blue is perhaps guessing against considerable odds, but there are reasons even for this seemingly unlikely prognostication.

The multitudinous part is, I think, obvious.  The more memory cells the machine has, the more the machine can store away – learn – the more tables and material it can have on hand, and the more complicated routines it can remember and follow.  The human brain, for instance, has around ten billion nerve cells.  It may be that each of these can do more than store a single binary digit – a single off or on, or 0 or 1.  Even if each nerve cell stored only one digit, that would still make the brain a lot bigger than any computing machine contemplated at present.  Present plans for machines actually to be built call for one hundred thousand or so binary digits, or, for only a hundred-thousandth as many storage cells as the brain has nerve cells.  Mathematicians like to talk about machines to store one to ten million binary digits, which would still fall short of the least estimated size of the brain by a factor of one thousand to ten thousand.  But, if one hundred thousand and ten million both small numbers as far as the human brain is concerned, they’re big numbers when it comes to building a machine, as we can readily see.  It is because of the size of such numbers that we know that the memory cells of our thinking machine will have to be small, and, we might add, cheap.

For instance, some present-day computers use relays as memory cells.  Now, a good and reliable relay, one good enough to avoid frequent failure even when many thousands of relays are used, costs perhaps two dollars.  If we wanted a million cells, the cost of the relays would thus be two million dollars, and this is an unpleasant thought to start with.  Further, one would probably mount about a thousand relays on one relay rack, and so there would be a thousand relay racks.  These could perhaps be packed into a space of about six thousand square feet – around eighty by eighty feet.  Then, there would have to be quite a lot of associated equipment, for more relays would be needed to make a connection to a given memory cell and to utilize the information in it.  This would increase the cost and the space occupied a good deal.  The thing isn’t physically possible, but it seems an unpromising start if we wish to advance further toward the at least ten sand-fold greater complexity of the human brain.

Fortunately, at just the time it as needed, something better than the relay has come along.  That something, the possessor of the little blue cells, is the selectron.  It is a vacuum tube which can serve in the place of several thousand relays.  It promises to be reliable, small and, dually, at least, cheaper than relays, and in addition it is very much faster – perhaps a thousand-fold.  The selectron was invented by an engineer, Dr. Jan A. Rajchman – pronounced Rikeman – for the purpose of making an improved computer and so its appearance at the right time is, after all, no accident.  Instead, it is a tribute to Dr. Rajchman’s great inventive ability.  Lots of people who worked on computers knew what the problem was, but only he thought of the selectron.

You might wonder how to go about inventing just what is needed, and if Dr. Rajchman’s career can cast any light on this, it’s certainly worth looking into.  Did he, for instance, think about computers from his earliest technical infancy?  The answer is that he certainly didn’t.  I have a copy of his doctoral thesis, “Le Courant Résiduel dans Les Multiplicateurs D’Electrons Electrostatiques,” which tells me that he was born in London in 1911, that he took his degree at Le Ecole Polytechnique Federale, at Zurich and thereafter did research on a radically new type of electrically focused photo-multiplier – see “Universes to Order,” in Astounding for February, 1944.  I am not sure how many different problems he has worked on since, but during the war he did do some very high-powered theoretical work on the betatron, as well as some experimental work on the same device.  It would seem that the best preparation for inventing is just to become thoroughly competent in things allied to the field in which something new is needed.

What was needed in connects with computers was, as we have said, a memory cell, or, rather, lot, of them.  What do these cells have to do?  First of all, one must be able to locate a given cell in the memory so as to put information into it or take information out.  Then, one must be able to put into the cell the equivalent of a 0 or a 1.  One must have this stay there indefinitely, until it is deliberately changed.  Finally, one must be able to read off what is stored in the cell; one must be able to tell whether it signifies 0 or 1 without altering what is in the cell.  The selectron has these features.

You might be interested in some of the earlier suggestions for using an electron tube as a memory in a computing machine.  The electron beam of a cathode ray tube sounds like just the thing for locating a piece of information, for instance.  One has merely to deflect it the right amount horizontally and vertically to reach a given spot on the screen of the tube.  One wishes, however, to store a particular piece of information in a particular place and then to find that same place again and retrieve that same piece of information.  This would mean producing the exact voltages on the deflecting plates when the formation was stored, and that is by no means easy.  Further, if the accelerating voltage applied to the tube changes, the deflecting voltage needed to deflect the beam to a given place changes, and this adds difficulty.  When we realize further that our memory simply must not make mistakes, we see that there are real objections -to locating and relocating a given spot by simply deflecting an electron beam to it.  The selectron has a radically different means for getting electrons to a selected spot – the selectron grid.

The features of the selectron which Dr. Rajchman holds in his hand – page 163 – are illustrated simply in Figure 1.  There is a central cathode and around it a concentric accelerating grid.  When this grid is made positive with respect to the cathode, a stream of electrons floods the entire selectron grid, the next element beyond the accelerating grid.  The selectron grid, is made up of a number of thin bars located in a circular array, pointing radially outward, and a number of thin rings, spaced the same distance apart as are the bars.  Figure 2 shows a portion of the selectron grid formed by the rings and bars.  The rings and bars together form a number of little rectangular openings or windows.

Now, in operation each bar and ring of the selectron grid is held either several hundred volts positive with respect to the cathode, or else a little negative with respect to the cathode.  After a definite pattern of ages has been established on the selectron grid, the accelerating grid is made positive and the selectron grid is flooded with electrons.  What happens?  Let us consider first the bars of the selectron grid.  Figure 3 tells the story.  If two neighboring bars are negative, the approaching electrons are simply repelled and turned back.  If an electron enters the space between a positive bar and a negative bar, it is so strongly attracted toward the positive bar that it strikes it and is lost.  Only if the bars on both sides of the space which the electron enters are positive does the electron get through.  At the rings, the story is the same; an electron can pass between two rings only if both are positive; it is stopped if either one or both are negative.  Thus we conclude that electrons can pass through a little window formed by two bars and two rings only if both bars and both rings are positive.  If both bars and both rings forming a window are held positive, the window is open; if one or more of the bars or rings are negative, the window is closed.  Thus, we have a means for letting electrons through one window at a time.

In the early model selectrons there were sixty-four apertures between bars around the tube, and sixty-four apertures lengthwise, giving four thousand ninety-six windows in all, and any one of these could be selected for the passage of electrons by applying proper voltages to the bars and rings.  Does this mean that we must have one hundred twenty-eight leads into the tube for this alone, one for each bar and one for each ring?  The tube would certainly work if it had one hundred twenty-eight leads to the selectron grid, but Dr. Rajchman’s ingenuity has cut this down instead to thirty-two, a saving by a factor of four.  How is this done?  The table of Figure 4 tells the story.  Here we have in the top row the numbers of the bars, in order, sixty-four in all.  These bars are connected to two sets of eight leads.  The second and third rows show to which lead of a given set a bar is connected.  Thus, Bar 1 is connected to Lead 1 of Set I.  Bar 2 is connected to Lead 1 of Set II, while Bar 64 is connected to Lead 8 of Set II.  To save space, some of the bars have been omitted from the table.

You will observe that if we make Lead 7 of Set I positive, and all the rest of the leads of Set I negative, Bars 13, 29, 45 and 61 will be positive.  Then, if we make Lead 2 of Set II positive and all the other leads of Set II negative Bars 4, 8, 12 and 16 will be positive.  All the bars which do not appear in either of the above listings will be negative.  Now, the only adjacent bars listed are 12 and 13, which have been written in italics.  Hence, when Lead 7 of Set I and Lead 2 of Set II are made positive and all the other leads negative, electrons can pass between the two adjacent positive bars 12 and 13, but not between any other bars.  Thus, by selecting one lead from Set I and one lead from Set II, we can select any of the sixty-four spaces between bars.

The thoughtful reader will have noticed, by the way, that there are only sixty-three spaces between sixty-four bars.  This, however, omits the space out to infinity from Bar 1 and back from infinity to Bar 64.  We can in effect shorten this space by adding an extra bar beyond the sixty-fourth and connecting it to Bar 1.

The same sort of connection used with the bars is made to the ring so that by selecting and making positive one lead each in two sets of eight leads we can select any of the sixty-four spaces between rings.  Thus, in the end we have four sets of eight leads each, two sets the bars and two for the rings.  We make positive one wire in each set at a time.  The number of possible combinations we can get this way is four thousand ninety-six, and each allows electrons to go through just one window out of the four thousand ninety-six formed by the bars and rings of the selectron grid.  The action is entirely positive.  A given window is physically located in a given place.  Small fluctuations in the voltages applied to the bars and rings will not interfere with the desired operation.  This is a lot different from trying to locate a given spot by waving an electron beam around.

The selectron grid and its action are- of course, only a part of the mysteries of the selectron.  They provide a means for directing a stream of electrons through one of several thousand little apertures at will.  But, how can this stream of electrons be used in storing a signal and then in reading it off again?  Part of the answer is not new.  For some time electronic experts have n thinking of storing a signal on an insulating surface as an electric charge deposited on the surface by means of an electron stream.  Thus, by putting electrons on a sheet of mica, for instance, we can make the surface negative, and by taking them off we can make it positive.  It is easy enough to do either of these things, as we shall see in a moment.

There are two very serious difficulties with, such a scheme, however.  First, how shall we keep the positive or negative charge on the insulating surface indefinitely?  It will inevitably tend to leak off.  Second, how can we determine whether the surface is charged positively or negatively without disturbing the charge?  The logical exploring tool is an electron beam, but won’t the beam drain the charge off in the charge off in the very act of exploration?  Both of these difficulties are overcome in the selectron.  To understand how, we must know a little about secondary emission.

Beyond the accelerating and selectron grids of the selectron, as shown in Figure 1, there is a sheet of mica indicated as “storage surface.”  This has a conducting backing.  We are interested in what happens when electrons pass through an open window in the selectron grid – one made up of four positive bars and rings – and strike the mica.  The essential ingredients of the situation are illustrated in the simplified drawing of Figure 5.  Here the accelerating grid and the selectron grid are lumped together and shown as positive with respect to the cathode.  Electrons are accelerated from the cathode, pass through the accelerating grid and the open window of the selectron grid, and shoot toward the mica storage surface.  What happens?  That depends on the potential of the storage surface with respect to the cathode.

In Figure 6 the current reaching the part of the storage surface behind an open window is plotted vs. the potential of that part of the storage surface with respect to the cathode.  Potential is negative with respect to the cathode to the left of the vertical axis and positive with respect to the cathode to the right of the vertical axis.  Current to the storage surface is negative – electrons reaching the surface and sticking below the horizontal axis and positive – more electrons leaving the surface than reaching it – above the horizontal axis.  The curve shows how current to the surface varies as the potential of the surface is varied.

If the surface is negative with respect to the cathode, the electrons shot toward it are turned back before they reach it and the current to the surface is zero.  If the surface is just a little positive, the electrons shot toward it are slowed down by the retarding field between the very positive selectron grid and the much less positive storage surface, and they strike the surface feebly and stick, constituting a negative-current flow to the surface, and tending to make the surface more negative.  If the potential of the storage surface is a little more positive with respect to the cathode, the electrons reach it with enough energy to knock a few electrons out of it.  These are whisked away to the more positive selectron grid.  These negative electrons leaving the surface are equivalent to a positive current to the surface.  There are now as many electrons striking as before, but there are also some leaving, and there is less net negative current to the surface.  Finally, at some potential labeled V0 in Figure 6, one secondary electron is driven from the surface for each primary electron which strikes it, and the net current to the surface is zero.  If the potential of the storage surface is higher than V0, each primary electron releases more than one secondary and there is a net flow of electrons away from the surface, equivalent to a positive current to the surface.  This tends to make the storage surface more positive.

As the potential of the storage surface rises further above V0, current for a time becomes more and more positive.  Then, abruptly the neighborhood of the potential VS of the selectron grid itself, the current becomes negative again and stays negative.  Why is this?  The the primary electrons still strike the storage surface energetically and drive out more than one electron each.  The fact is that these secondary electrons leave the surface with very little speed.  When the storage surface is more positive than the selectron grid, there is a retarding field at the storage surface which tends to turn the secondaries back toward the storage surface.  Hence, there, is still a flow of primaries – a negative current – to the surface, but the secondaries are turned back before reaching the selectron grid and fall on the storage surface again.  Thus, the current to the storage surface is again negative.

Our mechanism for holding the storage surface positive or negative is immediately apparent from Figure 6.  If the surface is more positive than Vs, the current to it is negative and its potential will tend to fall.  If the surface has a potential between V0 and Vs, the current to it is positive and its potential will tend to rise.  Hence, if the storage surface initially has any potential higher than V0, current will flow to it in such a way as to tend to make its potential VB, the potential of the selectron grid.  If, on the other hand, the potential is between O and V0, the current to the surface will be negative and the potential of the surface will tend to fall to O.  If the potential of the surface is negative with respect to the cathode – less than O – there is no current to it from the electron stream and hence no tendency for the potential to rise and fall.  Actually, some leakage would probably result in 3 very slight tendency for the potential to rise.

We see, then, that when it is bombarded by electrons, a part of the storage surface tends naturally to assume one of two potentials, or VS O.  If it has initially any other potential, it tends to come back to one of these.  Which potential it assumes is determined by whether the initial potential is greater or less than V0.  Thus, if we store information on the part of the storage surface behind a particular window by making this area have a potential Vs with respect to the cathode – meaning, say, 1 – or O – meaning, O – and if this potential changes a little through electrical leakage, perhaps adjacent portions at a different potential, we can recover or regenerate the original potential merely by opening the window of the selectron grid and flooding the area with electrons.  In fact, we can periodically regenerate the potentials behind all windows by opening all windows at once and flooding the whole surface with electrons.  This is what is done in the operation of the selectron, and this regenerative feature, which makes it possible to retain the stored information indefinitely despite electrical leakage, is one of the most ingenious and important features of the selectron.

How do we get the information on the portions of the storage surface beind the various windows?  That is, how do we initially bring some portions of the surface to the potential Vs and others to the potential V0?  In this process of writing inflation into the tube, we first open the particular one of the four thousand ninety-six windows behind which we wish to store a particular piece of information, thus flooding a little portion of the surface with electrons.  Then, to the terminals T of Figure 5, between the cathode and the conducting backstage of the storage surface, we apply a very sharply rising positive pulse, shown as the dashed line of Figure 7.  Because of the capacitance between this backing plate and the front of the storage surface, where the electrons fall, this drives the front of the storage surface positive.  Then the pulse applied to the conducting backing falls slowly to zero, as shown.  However, the action of the electrons falling on the surface tends to make it assume the potential Vs, and so if the pulse falls off slowly enough the portion of the surface on which electrons fall is left at the potential Vs, as shown by the solid line of Figure 7.  Application of the pulse will leave the portion of the storage surface behind the open window at the potential Vs regardless of whether its initial potential is Vs or O, and the pulse will not affect portions of the surface behind closed windows, because no electrons reach them.

This tells us how we can bring any selected area of the storage surface to the potential Vs which, we can say, corresponds to writing 1 in a particular cell of this memory tube.  By flooding a given area or cell with electrons and applying a sharply falling, negative pulse, which rises again gradually toward O – the dashed pulse of Figure 7 upside down – we can bring any selected area of the storage surface to O potential, and thus write O in any selected cell of the memory.

Thus, each little area of the storage surface behind each window of the selectron grid is a cell of our memory.  By opening a particular window – through making one lead of each of the four sets of eight selectron grid leads positive – and pulsing the conducting backing positive or negative, we can make the little area of the storage surface behind that window assume a potential Vs or a potential O, and so can, in effect, write 1 or 0 in that particular memory cell.  By opening all windows periodically and flooding all areas with electrons, we can periodically bring all little areas back to their proper potentials, either VS or O, despite leakage of electrons to or away from the little areas.  We can, that is, put thousands of pieces of information into the selectron and keep them there.  What about reading?  How can we get this information out?

Imagine that the entire inner storage surface is covered with a phosphor or fluorescent material like that used on cathode-ray tube screens or inside of fluorescent lights.  Now, suppose we open one window of the selectron, shooting electrons at a particular area of the surface.  If that area has a potential O, the electrons will be repelled from it.  But, if that area has a potential Vs, corresponding to 1, the electrons will strike the fluorescent surface vigorously, emitting a glow of blue light.  Suppose we let this light fall on a photo-multiplier, of the type Dr. Rajchman worked on earlier in his career.  Then, when we open a given window of the selectron, if the potential of the surface behind the window is O, we get nothing out of the multiplier.  But, if the potential is Vs, there is a flash of light, and a pulse of current from the multiplier.  And so, we can not only write a O or a 1 in each little memory cell of the selectron, we can not only keep this information there indefinitely, but we can also read it off at will.

Dr. Rajchman has devised other ways for reading the stored information in the selectron, but the use of a phosphor-coated storage surface together with a photo-multiplier has been one of the preferred method.  I have spoken of the phosphor as one giving blue light.  This is because the photo-multiplier is more sensitive to blue light than to other colors.  And so, I predicted that the memory cells of the thinking machines will be not only multitudinous and small, but also blue.

Of course the selectron provides only a part of the thinking machine – that is, the memory.  Associated with it there must be circuits in tubes to seek out stored in tubes to seek out stored information, to make use of it to obtain new formation, to write in that new information, and to make use of the new information in turn.  All is a field apart.  Still, there is one wrinkle which is so intimately connected with the use of the selectron that it deserves mention here.  I have referred to the O or 1 a cell of the selectron which can tore a binary digit or, alternately, as a letter of the electronic alphabet which the machine understands.  Now, usually we don’t want to store isolated digits or letters: we want to store complete numbers or words – combinations of 1 and O, as, 10011.  This is 19 in binary notation, and might in some instance stand for the nineteenth word in a dictionary.  When we look up a number or a word, we want it all at once, not piecemeal.

When we want to write many multi-digit numbers in a book, as, in a table of logarithms, for instance, we usually assign a vertical column for each digit to be stored, and write each digit of a given number in a different column, along the same row.  Thus, entries in a log table appear as in Figure 8.  Suppose that in using the selectron we assign a different tube to each binary digit of the numbers to be stored.  If we wish to store twenty-digit numbers, we will need twenty tubes.  Each tube will, in effect, be a given column of our storage space.  The different cells in a tube will represent different rows.  Thus, Cell 1 of Tube 1 will be Row 1 Column 1, Cell 1 of Tube 2 will be Row 1 Column 2, while Cell 10 of Tube 1 will be Row 10 Column 1, et cetera.

We want to look up all the digits in a given row at once.  This means that we want to open corresponding windows in all the tubes at once, and so we can connect the corresponding selectron grid leads of all twenty tubes together.   Thus, if want to store a number in Row 1, we apply voltages to the selectron grid leads which will open Window 1 in all tubes.  We are then ready to read the number in Row 1 or to write a new number in.   The twenty photo-multipliers which read the twenty selectrons are not connected in parallel, but are connected separately to carry off the twenty digits of the number in Row 1 to their proper destinations.  Perhaps these twenty leads from the twenty photo-multipliers may go to the twenty backing plates of another twenty selectrons to which it is desired to transfer the number.  We see, thus, how a whole table of numbers can be stored in twenty selectrons.  The windows 1, 2, 3 et cetera, can represent, for instance, the angle of which we want the sine.  The first selectron can store the first digits of all the sines, the second selectron can store all the second digits, et cetera.  The twenty digits of the sine of any angle – any window number – can be read off simultaneously from the photo-multipliers of the twenty selectrons.

The selectron isn’t perfect by any means.  Perhaps it’s not even the final answer.  At the moment, in its early form, it may be almost expensive as relays, but that’s partly because it’s new.  It’s certainly great deal more compact than relays, a very great deal faster, and probably more reliable as well.  It represents a first huge stride in the electronics of the thinking machine.  Just how far it takes us is up to a lot of mathematicians, a lot of circuit gadgeteers, and, especially, to Dr. Jan A. Rajchman and RCA, to whom we must look for smaller, cheaper and better selectrons.

– J.J. Coupling, 1949 –

______________________________

References

Dr. Jan A. Rajchman

Jan A. Rajchman (at Wikipedia)

Jan. A. Rajchman (at I.E.E.E. History)

J.J. Coupling (Dr. John R. Pierce)

J.J. Coupling (at Wikipedia)

J.J. Coupling (at Speculative Fiction Database)

Machine Hearing and the Legacy of John R. Pierce (at Cal Tech) (at CalTech.edu)

Creative Thinking, by John R. Pierce (at Tom Schneider’s “Molecular Information Theory and The Theory of Molecular Machines”)

Selectron Tube

Pierce, John R. (as J.J. Coupling), “The Little Blue Cells”, Astounding Science Fiction, 1949, Vol. 42, No. 6, February, 1949, pp. 85-99

Lamps & Tubes / Lampen & Röhren (Giorgio Basile’s website)

Selectron Tube (at Wikipedia)

RCA Selectron (at Charles Osborne’s “RCA Selectron.com” – superb and comprehensive website)

Почему фон Нейман верил в SELECTRON (“Pochemu fon Neyman Veril v Selectron”) (Why Von Neumann believed in the Selectron) (In Cyrillic)

Astounding Science Fiction

Analog Science Fiction and Fact (at Wikipedia)

Imagining the Integrated Circuit: Astounding Science Fiction – July, 1948

Sometimes, fiction can foresee fact.

Sometimes, entertainment can anticipate reality.

This has long been so in the realm of science fiction, a striking example of which – perhaps arising from equal measures and intuition and imagination – appearing in Astounding Science Fiction in mid-1949.  That year, Eric Frank Russell’s three-part serial “Dreadful Sanctuary” was serialized in the June, July, and August issues of the magazine.

(Astounding Science Fiction, June, 1948; cover by William F. Timmins.  Note Timmins’ name on the “puzzle piece” in the lower left corner!)

(Astounding Science Fiction, July, 1948; cover by Chesley Bonestell)

With interior illustrations by William F. Timmins, the story, set in 1972, is centered upon the efforts of protagonist John J. Armstrong – an iconoclastic combination of entrepreneur, inventor, and unintended detective – to accomplish the first successful manned lunar landing (as his entirely private venture) in the face the inexplicable mid-flight destruction of each of his organization’s spacecraft.  Armstrong doesn’t fit the cultural stereotype of inventor or scientist.  As characterized by Russell, “Armstrong was a big, tweedy man, burly, broad-shouldered and a heavy punisher of thick-soled shoes.  His thinking had a deliberate, ponderous quality.  He got places with the same unracy, deceptive speed as a railroad locomotive, but was less noisy.”

While Russell’s story commences as a solid – and solidly intriguing – mystery, effectively conveying a sense wonder; with characters who portend to be more than two-dimensional; the events, plot, and underlying tone gradually change.  With the installments in the magazine’s July and and August issues, what had been a story with an eerie undertone of Fortean inexplicability, technical conjecture (such as the “ipsophone”, a video-telephone imbued with aspects of artificial intelligence – cool! – we’re talking 1948!), and a well-crafted mood of impending threat, gradually and steadily falls flat.  A pity, because to the extent that the story succeeds – and in parts it does succeed, and creatively at that – it does so far more as a hard-boiled (and very ham-fisted) detective tale than science-fiction.

Regardless of the story’s literary quality (I don’t think it’s ever been anthologized) the physical and psychological presence of the aptly named Armstrong (“arm”?! “strong”?!) remain consistent throughout.  Iconoclastic and independent, he’s extremely intelligent, and if need be, a man capable of brute intimidation, self-defense, and violence.  He is also canny, cunning, and psychologically astute.

It is these latter qualities that lead to Armstrong’s discovery – after meeting with a police captain – of a most intriguing device, at his residence in the suburbs of New York City. 

Correctly suspicious of surveillance by adversaries, on reaching his residence, …Armstrong cautiously locked himself in, gave the place the once-over.

“Knowing the microphone was there, it didn’t take him long to find it though its discovery proved far more difficult than he’d expected.

“Its hiding place was ingenious enough – a one hundred watt bulb had been extracted from his reading lamp, another and more peculiar bulb fitted in its place.

“It was not until he removed the lamp’s parchment shade that the substitution became apparent.

“Twisting the bulb out of its socket, he examined it keenly.

“It had a dual coiled-coil filament which lit up in normal manner, but its glass envelope was only half the usual size and its plastic base twice the accepted length.

“He smashed the bulb in the fireplace, cracked open the plastic base with the heel of his shoe.

“Splitting wide, the base revealed a closely packed mass of components so extremely tiny that their construction and assembling must have been done under magnification – a highly-skilled watchmaker’s job!  The main wires feeding the camouflaging filament ran past either side of this midget apparatus, making no direct connection therewith, but a shiny, spider-thread inductance not as long as a pin was coiled around one wire and derived power from it.

Illustration by William Timmins (July, 1948, p. 101)

“Since there was no external wiring connecting this strange junk with a distant earpiece, and since its Lilliputian output could hardly be impressed upon and extracted from the power mains, there was nothing for it than to presume that it was some sort of screwy converter which turned audio-frequencies into radio or other unimaginable frequencies picked up by listening apparatus fairly close to hand.

“Without subjecting it to laboratory tests, its extreme range was sheer guesswork, but Armstrong was willing to concede it two hundred yards.

“So microscopic was the lay-out that he could examine it only with difficulty, but he could discern enough to decide that this was no tiny but simple transmitter recognizable in terms of Earthly practice.

“The little there was of it appeared outlandish, for its thermionic control was a splinter of flame-specked crystal, resembling pin-fire opal, around which the midget components were clustered.” (July, 1948, pp.116-117)

I’ll not explain the origin of this device (it’d spoil the story should you read it!), but suffice to say that in the world of the “Dreadful Sanctuary”, things and people are not as they seem, in terms of origin, nature, and purpose. 

In our world, however, it seems that Eric Frank Russell created a literary illustration – at least in terms of its diminutive size and the delicacy of its fabrication – of what would in only a few years be known as the integrated circuit.

Sometimes, imagination can anticipate the future.

References

Chesley Bonestell (at Wikipedia)

Eric Frank Russell (at Wikipedia)

William F. Timmins (at Pulp Artists)

Astounding (Analog Science Fiction and Fact)

Integrated Circuit (at Wikipedia)