GENERAL OBSERVATIONS ON THE PROPERTIES OF CELLS.

From the number of different properties possessed by my cells, it might

be anticipated that the different combinations of those properties would

result in cells having every variety of action. This is found to be the

case. As a general rule, the cells are noteworthy in one respect only.

Thus, if a cell is extremely sensitive to light, it may not be specially

remarkable in other respects. As a matter of fact, however, the cells

most sensitive to the light are also "U B cells."

The property of sensitiveness to light is independent of the power to

generate current by exposure to light--the best current-generating cells

being only very moderately sensitive to light, and some of the most

sensitive cells generate scarcely any current at all. Current-generating

cells are, almost without exception, "U B cells;" and the best

current-generating cells are strongly polarized, showing a considerable

change of resistance by reversing the direction of a current through

them; and they are also strong "anode cells," i.e., the surface next to

the gold offers a higher resistance to a battery current than the other

surface of the selenium does. The power to generate a current is

temporarily weakened by sending a battery current through the cell while

exposed to light, in either direction. The current generated by exposure

to light is also weakened by warming the cell, unless the cell is

arranged for producing current by exposure to heat.

The properties of sensitiveness to light and to change of battery power

are independent of each other, as I have cells which are sensitive to

change of current but absolutely insensitive to light--their resistance

remaining exactly the same whether the cells are in darkness or in

sunlight. I also have cells which are sensitive to light, but are

unaffected by change of battery power, or by reversing the direction of

the current through them.

The sensitiveness to change of battery power is also independent of the

sensitiveness to reversal of direction of the current. Among the best "L

B cells," some are "anode cells" and others are "cathode cells," while

still others are absolutely insensitive to reversal of current or to the

action of light.

_Constancy of the resistance_.--A noticeable point in my cells is the

remarkable constancy of the resistance in sunlight. Allowing for

differences in the temperature, the currents, and the light, at different

times, the resistance of a cell in sunlight will remain practically

constant during months of use and experiments, although during that time

the treatments received may have varied the resistance in dark hundreds

of thousands of ohms--sometimes carrying it up, and at others carrying it

down again, perhaps scores of times, until it is "matured," or reaches

the condition in which its resistance becomes constant.

As has already been stated, the sensitiveness of a cell to light is

increased by proper usage. This increased sensitiveness is shown, not by

a lowered resistance in light, but by an increased resistance in dark.

This change in the cells goes on, more or less rapidly, according as it

is retarded or favored by the treatment it receives, until a maximum is

reached, after which the resistance remains practically constant in both

light and dark, and the cell is then "matured," or finished. The

resistance in dark may now be 50 or even 100 times as high as when the

cell was first made, yet, whenever exposed to sunlight it promptly shows

the same resistance that it did in the beginning. The various treatments,

and even accidents, through which it has passed in the mean time, seem

not to have stirred its molecular arrangement under the action of light,

but to have expended their forces in modifying the positions which the

molecules must normally assume in darkness.

_Practical applications_.--There are many peculiarities of action

occasionally found, and the causes of such actions are not always

discernible. In practice, I have been accustomed to find the

peculiarities and weaknesses of each cell by trial, developing its

strongest properties and avoiding its weaknesses, until, when the cell is

finished, it has a definite and known character, and is fitted for

certain uses and a certain line of treatment, which should not be

departed from, as it will be at the risk of temporarily disabling it. In

consequence of the time and labor expended in making cells, in the small

way, testing, repairing damages done during experiments, etc., the cost

of the cells now is unavoidably rather high. But if made in a commercial

way, all this would be reduced to a system, and the cost would be small.

I may say here that I do not make cells for sale.

The applications or uses for these cells are almost innumerable,

embracing every branch of electrical science, especially telegraphy,

telephony, and electric lighting, but I refrain from naming them. I may

be permitted, however, to lay before you two applications, because they

are of such general scientific interest. The first is my

_Photometer_.--The light to be measured is caused to shine upon a

photo-electric current-generating cell, and the current thus produced

flows through a galvano-metric coil in circuit, whose index indicates

upon its scale the intensity of the light. The scale may be calibrated by

means of standard candles, and the deflections of the index will then

give absolute readings showing the candle power of the light being

tested. Or, the current produced by that light and that produced by the

standard candle may be compared, according to any of the known ways of

arranging and comparing different lights--the cell being lastly exposed

alternately to the two lights, to see if the index gives exactly the same

deflection with each light.

This arrangement leaves untouched the old difficulty in photometry, that

arising from the different _colors_ of different lights. I propose to

obviate that difficulty in the following manner. As is well known, gold

transmits the green rays, silver the blue rays, and so on; therefore, a

cell faced with gold will be acted upon by the green rays, one faced with

silver by the blue rays, etc. Now, if we construct three cells (or any

other number), so faced that the three, collectively, will be acted upon

by all the colors, and arrange them around the light to be tested, at

equal distances therefrom, each cell will produce a current corresponding

to the colored rays suited to it, and all together will produce a current

corresponding to all the rays emitted by the light, no matter what the

proportions of the different colors may be. The three currents may act

upon the same index, but each should have its own coil, not only for the

sake of being able to join or to isolate their influences upon the index,

but also to avoid the resistances of the other cells. If a solid

transparent conductor of electricity could be found which could be thick

enough for practical use and yet would transmit all the rays perfectly,

i.e., transmit white light unchanged, that would be still better. I have

not yet found a satisfactory conductor of that kind, but I think the plan

stated will answer the same purpose. This portion of my system I have not

practically tested, but it appears to me to give good promise of removing

the color stumbling-block, which has so long defied all efforts to remove

it, and I therefore offer it for your consideration.

_Photo-electric regulator_.--My regulator consists of a

current-generating cell arranged in front of a light, say an electric

lamp, whose light represents the varying strength of the current which

supports it. The current produced in the cell by this light flows through

an electro-magnetic apparatus by means of which mechanical movement is

produced, and this motion is utilized for changing resistances, actuating

a valve, rotating brushes, moving switches, levers, or other devices.

This has been constructed on a small scale, and operates well, and I

think it is destined to be largely used, as a most sensitive, simple, and

perfect regulator for currents, lights, dynamos, motors, etc., etc.,

whether large or small.

In conclusion, I would say that the investigation of the physical

properties of selenium still offers a rare opportunity for making very

important discoveries. But candor compels me to add that whoever

undertakes the work will find it neither an easy nor a short one. My own

experience would enable me to describe to you scores of curious

experiments and still more curious and suggestive results, but lack of

time prevents my giving more than this very incomplete outline of my

discoveries.

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Scientific American Supplement, No. 492, June 6, 1885 · 第 36 / 59 题