[Illustration: DIAGRAM OF T-H ARC LIGHTING SYSTEM.]

The “T-H” (Thompson-Houston) lamp employed the shunt feed principle.

The carbons were normally separated, being in most types drawn apart

by a spring. A high resistance magnet, shunted around the arc, served

to draw the carbons together. This occurred on starting the lamp and

thereafter the voltage of the arc was held constant by the balance

between the spring and the shunt magnet. As the carbon burned away the

mechanism advanced to a point where a clutch was tripped, the carbons

brought together, and the cycle repeated. Both the T-H and Brush

systems were extensively used in street lighting, for which they were

the standard when the open arc was superseded by the enclosed.

OTHER AMERICAN ARC LIGHT SYSTEMS

[Illustration: THOMSON-HOUSTON ARC LAMP, 1878.

This is an early model with a single pair of carbons.]

[Illustration: THOMSON DOUBLE CARBON ARC LAMP.

This later model, having two pairs of carbons, was commercially used

for many years. This lamp is in the collection of the Smithsonian

Institution.]

Beginning with about 1880, several arc light systems were developed.

Among these were the Vanderpoele, Hochausen, Waterhouse, Maxim,

Schuyler and Wood. The direct current carbon arc is inherently more

efficient than the alternating current lamp, owing to the fact that the

continuous flow of current in one direction maintains on the positive

carbon a larger crater at the vaporizing point of carbon. This source

furnishes the largest proportion of light, the smaller crater in the

negative carbon much less. With the alternating current arc, the large

crater is formed first on the upper and then on the lower carbon. On

account of the cooling between alternations, the mean temperature falls

below the vaporizing point of carbon, thus accounting for the lower

efficiency of the alternating current arc.

[Illustration: MAXIM DYNAMO.

This dynamo is in the collection of the Smithsonian Institution.]

For this reason all these systems used direct current and the 10 ampere

ultimately displaced the 20 ampere system. The 10 ampere circuit

was later standardized at 9.6 amperes, 50 volts per lamp. The lamp

therefore consumed 480 watts giving an efficiency of about 15 lumens

per watt. This lamp gave an average of 575 candlepower (spherical) in

all directions, though it was called the 2000 cp (candlepower) arc as

under the best possible conditions it could give this candlepower in

one direction. Later a 6.6 ampere arc was developed. This was called

the “1200 cp” lamp and was not quite as efficient as the 9.6 ampere

lamp.

“SUB-DIVIDING THE ELECTRIC LIGHT”

While the arc lamp was being commercially established, it was at once

seen that it was too large a unit for household use. Many inventors

attacked the problem of making a smaller unit, or, as it was called,

“sub-dividing the electric light.” In the United States there were four

men prominent in this work: William E. Sawyer, Moses G. Farmer, Hiram

S. Maxim and Thomas A. Edison. These men did not make smaller arc lamps

but all attempted to make an incandescent lamp that would operate on

the arc circuits.

[Illustration: SAWYER’S INCANDESCENT LAMP, 1878.

This had a graphite burner operating in nitrogen gas.]

[Illustration: FARMER’S INCANDESCENT LAMP, 1878.

The graphite burner operated in nitrogen gas. This lamp is in the

collection of the Smithsonian Institution.]

Sawyer made several lamps in the years 1878–79 along the lines of the

Russian scientists. All his lamps had a thick carbon burner operating

in nitrogen gas. They had a long glass tube closed at one end and the

other cemented to a brass base through which the gas was put in. Heavy

fluted wires connected the burner with the base to radiate the heat,

in order to keep the joint in the base cool. The burner was renewable

by opening the cemented joint. Farmer’s lamp consisted of a pair of

heavy copper rods mounted on a rubber cork, between which a graphite

rod was mounted. This was inserted in a glass bulb and operated in

nitrogen gas. Maxim made a lamp having a carbon burner operating in a

rarefied hydrocarbon vapor. He also made a lamp consisting of a sheet

of platinum operating in air.

EDISON’S INVENTION OF A PRACTICAL INCANDESCENT LAMP

Edison began the study of the problem in the spring of 1878. He had a

well-equipped laboratory at Menlo Park, New Jersey, with several able

assistants and a number of workmen, about a hundred people all told.

He had made a number of well-known inventions, among which were the

quadruplex telegraph whereby four messages could be sent simultaneously

over one wire, the carbon telephone transmitter without which Bell’s

telephone receiver would have been impracticable, and the phonograph.

All of these are in use today, so Edison was eminently fitted to attack

the problem.

[Illustration: MAXIM’S INCANDESCENT LAMP, 1878.

The carbon burner operated in a rarefied hydrocarbon vapor. This lamp

is in the collection of the Smithsonian Institution.]

Edison’s first experiments were to confirm the failures of other

experimenters. Convinced of the seeming impossibility of carbon, he

turned his attention to platinum as a light giving element. Realizing

the importance of operating platinum close to its melting temperature,

he designed a lamp which had a thermostatic arrangement so that

the burner would be automatically short circuited the moment its

temperature became dangerously close to melting. The burner consisted

of a double helix of platinum wire within which was a rod. When the

temperature of the platinum became too high, the rod in expanding

would short circuit the platinum. The platinum cooled at once, the

rod contracted opening the short circuit and allowing current to flow

through the burner again. His first incandescent lamp patent covered

this lamp. His next patent covered a similar lamp with an improved

thermostat consisting of an expanding diaphragm. Both of these lamps

were designed for use on series circuits.

[Illustration: EDISON’S FIRST EXPERIMENTAL LAMP, 1878.

The burner was a coil of platinum wire which was protected from

operating at too high a temperature by a thermostat.]

The only system of distributing electricity, known at that time, was

the series system. In this system current generated in the dynamo

armature flowed through the field coils, out to one lamp after another

over a wire, and then back to the dynamo. There were no means by which

one lamp could be turned on and off without doing the same with all the

others on the circuit. Edison realized that while this was satisfactory

for street lighting where arcs were generally used, it never would

be commercial for household lighting. He therefore decided that a

practical incandescent electric lighting system must be patterned

after gas lighting with which it would compete. He therefore made

an intensive study of gas distribution and reasoned that a constant

pressure electrical system could be made similar to that of gas.

The first problem was therefore to design a dynamo that would give a

constant pressure instead of constant current. He therefore reasoned

that the internal resistance of the armature must be very low or the

voltage would fall as current was taken from the dynamo. Scientists

had shown that the most economical use of electricity from a primary

battery was where the external resistance of the load was the same as

the internal resistance of the battery, or in other words, 50 per cent

was the maximum possible efficiency.

[Illustration: DIAGRAM OF CONSTANT CURRENT SERIES SYSTEM.

This, in 1878, was the only method of distributing electric current.]

[Illustration: DIAGRAM OF EDISON’S MULTIPLE SYSTEM, 1879.

Edison invented the multiple system of distributing electric current,

now universally used.]

When Edison proposed a very low resistance armature so that the dynamo

would have an efficiency of 90 per cent at full load, he was ridiculed.

Nevertheless he went ahead and made one which attained this. The

armature consisted of drum-wound insulated copper rods, the armature

core having circular sheets of iron with paper between to reduce the

eddy currents. There were two vertical fields above and connected in

shunt with the armature. It generated electricity at about a hundred

volts constant pressure and could supply current up to about 60

amperes at this pressure. It therefore had a capacity, in the present

terminology, of about 6 kilowatts (or 8 horsepower).

[Illustration: EDISON DYNAMO, 1879.

Edison made a dynamo that was 90 per cent efficient which scientists

said was impossible. This dynamo is in the collection of the

Smithsonian Institution and was one of the machines on the steamship

Columbia, the first commercial installation of the Edison lamp.]

A multiple system of distribution would make each lamp independent of

every other and with a dynamo made for such a system, the next thing

was to design a lamp for it. Having a pressure of about a hundred volts

to contend with, the lamp, in order to take a small amount of current,

must, to comply with Ohm’s law, have a high resistance. He therefore

wound many feet of fine platinum wire on a spool of pipe clay and

made his first high resistance lamp. He used his diaphragm thermostat

to protect the platinum from melting, and, as now seems obvious but

was not to all so-called electricians at that time, the thermostat

was arranged to open circuit instead of short circuit the burner when

it became too hot. This lamp apparently solved the problem, and, in

order to protect the platinum from the oxygen of the air, he coated

it with oxide of zirconium. Unfortunately zirconia, while an insulator

at ordinary temperatures, becomes, as is now known, a conductor of

electricity when heated, so that the lamp short circuited itself when

it was lighted.

[Illustration: EDISON’S HIGH RESISTANCE PLATINUM LAMP, 1879.

This lamp had a high resistance burner, necessary for the multiple

system.]

[Illustration: EDISON’S HIGH RESISTANCE PLATINUM IN VACUUM LAMP, 1879.

This experimental lamp led to the invention of the successful carbon

filament lamp.]

During his experiments he had found that platinum became exceedingly

hard after it had been heated several times to incandescence by current

flowing through it. This apparently raised its melting temperature so

he was able to increase the operating temperature and therefore greatly

increase the candlepower of his lamps after they had been heated a few

times. Examination of the platinum under a microscope showed it to be

much less porous after heating, so he reasoned that gases were occluded

throughout the platinum and were driven out by the heat. This led him

to make a lamp with a platinum wire to operate in vacuum, as he thought

that more of the occluded gases would come out under such circumstances.

[Illustration: EDISON’S CARBON LAMP OF OCTOBER 21, 1879.

This experimental lamp, having a high resistance carbon filament

operating in a high vacuum maintained by an all-glass globe, was the

keystone of Edison’s successful incandescent lighting system. All

incandescent lamps made today embody the basic features of this lamp.

This replica is in the Smithsonian Institution exhibit of Edison lamps.

The original was destroyed.]

These lamps were expensive to make, and, knowing that he could get the

requisite high resistance at much less cost from a long and slender

piece of carbon, he thought he might be able to make the carbon last

in the high vacuum he had been able to obtain from the newly invented

Geissler and Sprengel mercury air pumps. After several trials he

finally was able to carbonize a piece of ordinary sewing thread. This

he mounted in a one-piece all glass globe, all joints fused by melting

the glass together, which he considered was essential in order to

maintain the high vacuum. Platinum wires were fused in the glass to

connect the carbonized thread inside the bulb with the circuit outside

as platinum has the same coefficient of expansion as glass and hence

maintains an airtight joint. He reasoned that there would be occluded

gases in the carbonized thread which would immediately burn up if the

slightest trace of oxygen were present, so he heated the lamp while it

was still on the exhaust pump after a high degree of vacuum had been

obtained. This was accomplished by passing a small amount of current

through the “filament,” as he called it, gently heating it. Immediately

the gases started coming out, and it took eight hours more on the pump

before they stopped. The lamp was then sealed and ready for trial.

[Illustration: DEMONSTRATION OF EDISON’S INCANDESCENT LIGHTING SYSTEM.

Showing view of Menlo Park Laboratory Buildings, 1880.]

On October 21, 1879, current was turned into the lamp and it lasted

forty-five hours before it failed. A patent was applied for on November

4th of that year and granted January 27, 1880. All incandescent lamps

made today embody the basic features of this lamp. Edison immediately

began a searching investigation of the best material for a filament and

soon found that carbonized paper gave several hundred hours life. This

made it commercially possible, so in December, 1879, it was decided

that a public demonstration of his incandescent lighting system should

be made. Wires were run to several houses in Menlo Park, N. J., and

lamps were also mounted on poles, lighting the country roads in the

neighborhood. An article appeared in the New York Herald on Sunday,

December 21, 1879, describing Edison’s invention and telling of the

public demonstration to be given during the Christmas holidays. This

occupied the entire first page of the paper, and created such a furor

that the Pennsylvania Railroad had to run special trains to Menlo

Park to accommodate the crowds. The first commercially successful

installation of the Edison incandescent lamps and lighting system was

made on the steamship Columbia, which started May 2, 1880, on a voyage

around Cape Horn to San Francisco, Calif.

The carbonized paper filament of the first commercial incandescent lamp

was quite fragile. Early in 1880 carbonized bamboo was found to be not

only sturdy but made an even better filament than paper. The shape of

the bulb was also changed from round to pear shape, being blown from

one inch tubing. Later the bulbs were blown directly from molten glass.

[Illustration: DYNAMO ROOM, S. S. COLUMBIA.

The first commercial installation of the Edison Lamp, started May 2,

1880. One of these original dynamos is on exhibit at the Smithsonian

Institution.]

As it was inconvenient to connect the wires to the binding posts of

a new lamp every time a burned out lamp had to be replaced, a base

and socket for it were developed. The earliest form of base consisted

simply of bending the two wires of the lamp back on the neck of the

bulb and holding them in place by wrapping string around the neck. The

socket consisted of two pieces of sheet copper in a hollow piece of

wood. The lamp was inserted in this, the two-wire terminals of the lamp

making contact with the two-sheet copper terminals of the socket, the

lamp being rigidly held in the socket by a thumb screw which forced

the socket terminals tight against the neck of the bulb.

[Illustration: ORIGINAL SOCKET FOR INCANDESCENT LAMPS, 1880.]

[Illustration: WIRE TERMINAL BASE LAMP, 1880.

This crude form of lamp base fitted the original form of lamp socket

pictured above. This lamp is in the exhibit of Edison lamps in the

Smithsonian Institution.]

This crude arrangement was changed in the latter part of 1880 to a

screw shell and a ring for the base terminals, wood being used for

insulation. The socket was correspondingly changed. This was a very

bulky affair, so the base was changed to a cone-shaped ring and a

screw shell for terminals. Wood was used for insulation, which a short

time after was changed to plaster of Paris as this was also used to

fasten the base to the bulb. It was soon found that the tension created

between the two terminals of the base when the lamp was firmly screwed

in the socket often caused the plaster base to pull apart, so the shape

of the base was again changed early in 1881, to the form in use today.

An improved method of connecting the ends of the filament to the

leading-in wires was adopted early in 1881. Formerly this was

accomplished by a delicate clamp having a bolt and nut. The improvement

consisted of copper plating the filament to the leading-in wire.

[Illustration: ORIGINAL SCREW BASE LAMP, 1880.

This first screw base, consisting of a screw shell and ring for

terminals with wood for insulation, was a very bulky affair. This lamp

is in the exhibit of Edison lamps in the Smithsonian Institution.]

[Illustration: IMPROVED SCREW BASE LAMP, 1881.

The terminals of this base consisted of a cone shaped ring and a screw

shell. At first wood was used for insulation, later plaster of paris

which was also used to fasten the base to the bulb. This lamp is in the

exhibit of Edison lamps in the Smithsonian Institution.]

In the early part of the year 1881 the lamps were made “eight to

the horsepower.” Each lamp, therefore, consumed a little less than

100 watts, and was designed to give 16 candlepower in a horizontal

direction. The average candlepower (spherical) in all directions was

about 77 per cent of this, hence as the modern term “lumen” is 12.57

spherical candlepower, these lamps had an initial efficiency of about

1.7 lumens per watt. The lamps blackened considerably during their life

so that just before they burned out their candlepower was less than

half that when new. Thus their mean efficiency throughout life was

about 1.1 l-p-w (lumens per watt). These figures are interesting in

comparison with the modern 100-watt gas-filled tungsten-filament lamp

which has an initial efficiency of 12.9, and a mean efficiency of 11.8,

l-p-w. In other words the equivalent (wattage) size of modern lamp

gives over seven times when new, and eleven times on the average, as

much light for the same energy consumption as Edison’s first commercial

lamp. In the latter part of 1881 the efficiency was changed to “ten

lamps per horsepower,” equivalent to 2¼ l-p-w initially. Two sizes of

lamps were made: 16 cp for use on 110-volt circuits and 8 cp for use

either direct on 55 volts or two in series on 110-volt circuits.

[Illustration: FINAL FORM OF SCREW BASE, 1881.

With plaster of paris, the previous form of base was apt to pull apart

when the lamp was firmly screwed into the socket. The form of the base

was therefore changed to that shown, which overcame these difficulties,

and which has been used ever since. The lamp shown was standard for

three years and is in the exhibit of Edison lamps in the Smithsonian

Institution.]

EDISON’S THREE-WIRE SYSTEM

The distance at which current can be economically delivered at 110

volts pressure is limited, as will be seen from a study of Ohm’s law.

The loss of power in the distributing wires is proportional to the

square of the current flowing. If the voltage be doubled, the amount

of current is halved, for a given amount of electric power delivered,

so that the size of the distributing wires can then be reduced to

one-quarter for a given loss in them. At that time (1881) it was

impossible to make 220-volt lamps, and though they are now available,

their use is uneconomical, as their efficiency is much poorer than that

of 110-volt incandescent lamps.

Edison invented a distributing system that had two 110-volt circuits,

with one wire called the neutral, common to both circuits so that the

pressure on the two outside wires was 220 volts. The neutral wire had

only to be large enough to carry the difference between the currents

flowing in the two circuits. As the load could be so arranged that it

would be approximately equal at all times on both circuits, the neutral

wire could be relatively small in size. Thus the three-wire system

resulted in a saving of 60 per cent in copper over the two-wire system

or, for the same amount of copper, the distance that current could be

delivered was more than doubled.

[Illustration: DIAGRAM OF EDISON’S THREE-WIRE SYSTEM, 1881.

This system reduced the cost of copper in the multiple distributing

system 60 per cent.]

DEVELOPMENT OF THE ALTERNATING CURRENT CONSTANT POTENTIAL SYSTEM

The distance that current can be economically distributed, as has

been shown, depends upon the voltage used. If, therefore, current

could be sent out at a high voltage and the pressure brought down to

that desired at the various points to which it is distributed, such

distribution could cover a much greater area. Lucien Gaulard was a

French inventor and was backed by an Englishman named John D. Gibbs.

About 1882 they patented a series alternating-current system of

distribution. They had invented what is now called a transformer which

consisted of two separate coils of wire mounted on an iron core. All

the primary coils were connected in series, which, when current went

through them, induced a current in the secondary coils. Lamps were

connected in multiple on each of the secondary coils. An American

patent was applied for on the transformer, but was refused on the basis

that “more current cannot be taken from it than is put in.” While

this is true if the word energy were used, the transformer can supply

a greater current at a lower voltage (or vice versa) than is put in,

the ratio being in proportion to the relative number of turns in the

primary and secondary coils. The transformer was treated with ridicule

and Gaulard died under distressing circumstances.

[Illustration: DIAGRAM OF STANLEY’S ALTERNATING CURRENT MULTIPLE

SYSTEM, 1885.

This system is now universally used for distributing electric current

long distances.]

Information regarding the transformer came to the attention of

William Stanley, an American, in the latter part of 1885. He made an

intensive study of the scheme, and developed a transformer in which

the primary coil was connected in multiple on a constant potential

alternating-current high-voltage system. From the secondary coil a

lower constant voltage was obtained. An experimental installation

was made at Great Barrington, Mass., in the early part of 1886, the

first commercial installation being made in Buffalo, New York, in the

latter part of the year. This scheme enabled current to be economically

distributed to much greater distances. The voltage of the high-tension

circuit has been gradually increased as the art has progressed from

about a thousand volts to over two hundred thousand volts pressure in a

recent installation in California, where electric power is transmitted

over two hundred miles.

INCANDESCENT LAMP DEVELOPMENTS, 1884–1894

In 1884 the ring of plaster around the top of the base was omitted; in

1886 an improvement was made by pasting the filament to the leading-in

wires with a carbon paste instead of the electro-plating method; and

in 1888 the length of the base was increased so that it had more

threads. Several concerns started making incandescent lamps, the

filaments being made by carbonizing various substances. “Parchmentized”

thread consisted of ordinary thread passed through sulphuric acid.

“Tamadine” was cellulose in the sheet form, punched out in the shape

of the filament. Squirted cellulose in the form of a thread was also

used. This was made by dissolving absorbent cotton in zinc chloride,

the resulting syrup being squirted through a die into alcohol which

hardened the thread thus formed. This thread was washed in water, dried

in the air and then cut to proper length and carbonized.

[Illustration: STANDARD EDISON LAMP, 1884.

The ring of plaster around the neck of previous lamps was omitted. This

lamp is in the exhibit of Edison lamps in the Smithsonian Institution.]

[Illustration: STANDARD EDISON LAMP, 1888.

The length of the base was increased so it had more threads. This lamp

is in the exhibit of Edison lamps in the Smithsonian Institution.]

History of electric light · 第 3 / 6 段