So, the effective area of a rotor S is as follows.
And also, because the number of rotor is n, the whole effective area of rotors(S) is as follows.
|
C = | 1 | ¡¿ |
n(r2 - r 1)
{¥ð(r2 +r
1)- 2E¥á } |
[F] |
|
|
| 9¡¿1011 |
4¥ðd |
2. The Rotation Movement of Rotor and Charge * Discharge
of Electric Energy
For the sake of convenience, after it was assumed that A and B
in Figure 3 do horizontal movements, the principle was explained. But, in fact, because they do rotation movements,
A and B are treated as stators, and a' and b' as rotors like Figure 7~11. And though slip rings are shown to be four
different-sized concentric circles, R1 is expressed to seem connected directly with a, b and R2 connected directly
with a', b' by omitting slip rings and brushes in Figure 8~11. And in case A and B are equal to a and b like Figure 7,
the capacity is expressed as Cab, and in case A and B are equal to a' and b' like Figure 9, the capacity is expressed
as Ca'b'. When (+) and (-) electricity are stored in A and B with D.C. high voltage generator, (-) and (+) electricity
are produced in a and b owing to the action of electrostatic induction. And because A and B are completely insulated,
it is assumed that (+) and (-) electricity once stored here are not changed and are preserved forever.
By means of the formula,
electric energy of
is stored in Figure 7.
In that case, in order to make the voltage of electric energy
V(Wab = 1/2 CabV2 [J]but the original voltage is V.), the voltage of D.C.
high voltage generator which is authorized by A and B must be made to be 2V because
Figure 3 is the same that two in Figure 1 are connected in series(Refer to series connection method of condenser)
.
Like in Figure 8, when a rotor is rotated to the direction of ¡æ , (-)
electricity is produced in a escaping from (+) electric attraction of A and (+) electricity is produced in b escaping from
(-) electric attraction of B. But these electricities flow into R1 by their own attraction as soon as they escape from (+) and
(-) electric attraction of A and B. And because the part which took (+) electric attraction of A appears in a', electrostatic
induction action takes place, and then (-) and (+) electricity are produced. And because the part which took (-) electric
attraction of B appears in b', electrostatic induction operation occurs, and then (+) and (-) electricity are produced. In that
case, (-) electric attraction of a' and (+) electric attraction of b' remain kept because they are attracted by (+) and (-)
electric attraction of A and B, while (+) electric attraction of a' and (-) electric attraction of b' flow into R2 by their own
attractions. Accordingly, like in Figure 9, the electric energy of

first stored during rotation until a' and b' are equal to A and B, and the electric energy of
not taken by the electric attraction of A and B among electric energy newly produced by electrostatic induction action are stored.
Therefore, the amount of electric energy flows to R1 and R2 while a rotor is half rotated is two times as much as the amount of electric
energy first stored.
&When a rotor is rotated like in Figure 10, contrary to Figure 8, (-) electricity appears in a' escaping from (+)
electric attraction of A and (+) electricity appears in b' escaping from (-) electric attraction of B.
But these electricities flow into R2 by their own
attraction as soon as they escape from (+) and (-) electric attraction of A and B. And because the part which took (+) electric
attraction of A appears in a, electrostatic induction action occurs, and then (-) and (+) electricity are produced. And because the
part which took (-) electric attraction of B appears in b, electrostatic induction action occurs, and then (+) and (-) electricity are
produced. In that case, (-) electric attraction of a and (+) electric attraction of b remain kept because they are attracted by (+)
and (-) electric attraction of A and B, while (+) electric attraction of a and (-) electric attraction of b flow into R1 by their own
attractions. But in that case, because the pole is changed like in Figure 8, a and b' are (-) poles and b and a' are (+) poles.
On the other hand, because a' and b are (-) poles, and b' and a are (+) poles like in Figure 10, the direction of electric current is
opposite to Figure 8. Accordingly, the electric current of electrostatic induction generator is an alternating current.
When a rotor reaches the state like in Figure 11, the electric energy of

in Figure 9 stored and the electric energy of
not taken by the electric attraction of A and B among electric energy produced newly by electrostatic induction action flow into R1
and R2, but the electric energy of
not taken by the electric attraction of A and B is stored. Therefore, the amount of electric energy which flows to R1 and R2 while
a rotor is once rotated is
2(Wab + Wa'b') = 2(1/2 CabV2
+1/2 Ca'b'V2 ) [J]
And for the sake of convenience, Cab and Ca'b' are distinguished, but because they are actually
the same capacity, if Cab and Ca'b' are C,
2(Wab + Wa'b') = 2(1/2 CabV2 +1/2 Ca'b'V2 )
= 2(1/2 CV2 +1/2 CV2 )
= 2CV2 [J]
And because the amount of electric energy flowing into R1 and R2 is proportioned to the number
of rotations, if the number of rotations per t second is N, the following expression becomes made.
W = 2 CV2 Nt [J]
Like this, whenever a rotor is half rotated, a half of the electric energy newly produced by the stored electric energy and electrostatic
induction action flows into external circuit, and the other half is repeatedly stored and at the same time electricity comes to flow, the direction
of electric current changing. In that case, the type of wave motion gets rectangular. In other words, electric current is proportioned to the
area of rotor, whenever a rotor is half rotated, the direction of electric current is changed. And also, because the area of rotor is linearly
constant whenever changed again, it gets developed into a rectangle-wave alternating current.
But this is not a good form of wave.
In order to get an applicable big output, the voltage should be strengthened to generate electricity. But it cannot be used as it is.
So the voltage should be moderately lowered by using a transformer, in that case sine wave is the most efficient. Electric current
is proportioned to the changing area of rotor. Like in Figure 12, either the pole of electric connector may be made rectangular(dotted line)
and the pole of rotor may be made a form of sine, or the polar number may be heightened to the maximum because the higher the polar
number gets, the closer it gets to sine wave.
Accordingly, because the polar number is heightened to the maximum to make output high, the pole of rotor necessarily need not be made
to be a form of sine.
3. Relation between Polar Number, Output and Electric Current
Polar
number would mean that of stator and the rate of stator to rotor is 1 to 2.
When a stator with one pole
like in Figure 5 is combined with a rotor with two poles like in Figure 6, a simple rotor like in Figure 13 is made.
Let`s suppose
that when a stator is rotated in the direction of ¡æ and for t second with a certain velocity, the changed areas become a[§²]
and a'[§²](The unit of [§²] will below be omitted.).
And then when a stator of two poles is combined with a rotor with four poles after they made like Figure
14 with the same sizes as Figure 5 and 6, a simple generator like in Figure 15 is made.
And when a rotor is rotated in the direction of ¡æ and for t second at the same velocity with Figure 13,
the changed areas become b, b', c and c'. Accordingly,
a=a'=b=b'=c=c'
2(a+a') = (b+b') + (c+c')

Like this, they are the same sizes, but when polar number becomes two, the changed area also becomes double and when polar number becomes three, the changed area also becomes three times .....
and when polar number becomes n, the changed area also becomes n. That is to say, the changing area of rotor becomes proportioned to polar number. Thus, because the electricity stored in the whole area of rotor does not flow into external circuit at a time, but whenever
a rotor is rotated, the electricity of changing area flows into external circuit, electric current becomes increased with a certain size, proportioned to polar number. In other words, when polar number is heightened two, three, ...... n times, the capacity is increased two,
three, ...... n times, or the velocity of rotation becomes two, three, ...... n times fast. Therefore, if the former formula of 
W = 2 CV2 Nt [J]
is multiplied by polar number(E),
the amount of electric energy flowing to outside while rotor is rotated for t second becomes
W = 2 CV2 NEt [J]
When this is expressed by electric power(P),
| p= |
2 CV2 NEt | = 2 CV2 NE [W] |
|
| t |
This is a basic formula to calculate the output of electrostatic induction generator.
And this formula
of output is broken down into electric voltage and electric current. Because
P=V¥¡ [W]
can be broken down into
P=V¥¡
[W]
So when
P = 2 CV2 NE [W]
is broken down into
P = V¤ý2 CVNE [W] ,
V is electric voltage and
¥¡ = 2 CVNE [A]
is electric current.
Like this, it can be found that while sizes are the same, output and electric current are proportioned to polar number.
This is already made public as No. 91-13655.
And because frequency (f) is the product of rotation no.(N) multiplied by polar no.(E),
it becomes
f = NE / sec [Hz]
So the frequency of electrostatic induction generator is much higher than that of common alternating current(50/60[HZ]) because the number
of rotations and that of poles are heightened to the maximum to heighten output.
But polar number should not be heightened without limit. Because
when polar number is heightened, the number of insulated line(11) proportioned to polar number is also increased, and it means that the effective
area is decreased as much. Thus, polar number should be fixed moderately.
Now, the making of stator and rotor, and the way
both of them are combined will be explained.
1.Stator
A stator makes a rotor produce
electrostatic induction, keeping a strong electric connection owing to the high voltage of D.C. high voltage generator. When electricity is generated
into just one of (+) and (-) poles in D.C high voltage like B in Figure 1, it is called a simple-system stator(Patent No. 8606). And when electricity is
generated into both of (+) and (-) poles like A and B of Figure 3, it is called a plural-system stator.
After many insulated plates with 2mm thick are made quadrilateral, they are cut in half and the
opposite angles of coupling holes(7, 8) are also cut to decompose and compose them freely. And after posting thin aluminum paper
on it and with razor blade drawing lines on electrode(1), coupling wires(3, 4) and another coupling wires(5, 6) connecting all electrodes with
coupling holes(7, 8) like a form of Figure 16, detach the aluminum paper from other parts except electrode(1), coupling wires(3, 4, 5, 6) and
coupling holes(7, 8). And electrode, coupling wire and coupling hole are made on the back side just like on the front side, but all electrodes(1)
on both front and back side should match each other and the same. And also, as high voltage is allowed in stator, insulation is very important.
So an insulated tape was attached four times and after cutting it, a strong adhesive was posted on the edge.
But I made this easily.
If a stator is practically made, this insulation alone is not enough. As long as there isn`t a perfect insulator,
electricity flows to places(2) other than electrode(1) under high voltage. So the result is that the voltage of electrode
becomes nearly the same as that of non-electrode and the output decreases much. So in order not to transmit electricity to non-electrode,
as illustrated in Figure 16, it should be detached(2; dotted line part) or it should be sunken in.
2. Rotor
A rotor makes electricity flow into outside, doing electrostatic induction action and rotation movement owing to a strong electric
force of a stator.
In order to make the electricity of a rotor flow into outside, the basic principle of Patent No. 8606(Figure 1)
was supplemented like Figure 3, but this alone is not enough. Because electric attraction arising from both sides of a rotor gets weak and electricity
does not flow well when the insulated material is thick and the dielectric constant is high. Thus, the thinner insulated material and the higher
dielectric constant are good.
Many epoxy plates 1[mm] thick and both sides coated with copper plate are made circular like Figure 17,
and then axis holes(17) are drilled to make the axis of a rotor go through in the middle of them and many bolt holes(18) are drilled to
make thin and long bolt go through. And then transparent tape is attached on them. After drawing lines with razor blade to make a form
of electrode(d, e, f, g, h, I, j, k) like Figure 17, detach tape from non-electrode and draw lines with black enamel on places to become
coupling wires(12, 13, 14a, 14a'), circular circuits(15, 16) and integrated electrodes(a, a').

And connect electrodes(d, f, h, j) with integrated electrode(a) and electrodes(e, g, l, k) with integrated electrode(a').
And use the same method on back side as front side. Then electrodes(d', f', h', j') are connected with integrated electrode(b) and electrodes
(e', g', l', k') with integrated electrode(b'). In that case, like a rotor, d and d', e and e' ..... k and k' should match each other and the same.
And small conducting holes(19a, 19a', 20b, 20b') are drilled in all integrated electrodes(a, a', b, b'), so it is easy to connect
them with conducting wires. And when these rotors are put in solvent with chloride of second iron, copper is left in place with
tape and enamel posted but the other copper are dissolved and the rotors like Figure 17 and 18 are made. And in order to prevent
short-circuit, the surface of a rotor is thinly painted with clear rocker.
After making many rotors in this way
and dividing them into two, One is marked with C and the other with D. And then integrated electrodes of Group C are marked with ac,
b'c, a'c, bc like Figure 19 and integrated electrodes of Group D are marked with aD, b'D, a'D, bD like Figure 20. After that, put small
circular plates(26) to adjust space between C and D like Figure 21, and pass the axises of rotor(27) and long bolts(30) through axis holes(17)
and many bolt holes(18) in order of C, D, ..... And at the same time after passing conducting wire through conducting holes(19a, 19a', 20b, 20b')
of the same integrated electrodes(ac-ac, a'c-a'c ..... b'D-b'D), solder integrated electrode and conducting wire. In that case, the number of
integrated electrodes, or conducting wires is eight(ac, b'c, a'c, bc, aD, b'D, a'D, bD) but they should be divided into two. As it is shown in the
development figure of stator and rotor in Figure 22, bD, ac, b'c and a'D are (-) poles and aD, bc, b'D and a'c are (+) poles(It is A.C but is
classified into (+) and (-) like D.C because it is changed into the same pole.). So when they are made into one, it leads to two. And finally after
drawing these two conducting wires out of the last small circular plates(26') and connecting them with two slip rings(33, 34), make the insulated
lines(11, 11') of rotor in a row
and fasten both sides of the axises of rotor(27) and long bolts(30) with nuts(28, 29, 31). Now, the assembling of a rotor like Figure 21 is completed.
3. The Combination of Stator and Rotor
After assembling a rotor and a stator in this way, when both of
them are combined, it becomes an electrostatic induction generator. Now, after assembling a stator, the way to combine it with a rotor will be
described.
First, divide stators made like Figure 16 into two(A and B) and mark the bottom stator of A as A1, the top stator of A as A2,
the bottom stator of B as B1, and the top stator of B as B2. And, as illustrated in Figure 23, fasten front and back supporters(39, 39') on prop(38)
with acryl sticks(41, 41') 3[mm] thick and then fasten stators with adhesive in order of A1, B1, A1,.... on acryl sticks.
the assembled stator and fasten the bearing
And then put the rotor on (43) of the axis of the rotor on supporters(39, 39') with nuts to make the rotor rotate well. And fasten acryl stick(42') standing on both sides with
adhesive, pushing A2 into the grooves(9,10) of A1 and B2 into B1. And fasten the stator with acryl sticks diagonally so as to be crushed(Treat back
side with the same way as front side). And as illustrated in Figure 24, pass conducting wire(44A1) through the coupling hole(8) of A1, conducting
wire(44A2) through the coupling hole(7) of A2, conducting wire(44B1) through the coupling hole(8) of B1 and conducting wire(44B2) through
the coupling hole(7) of B2, and connect 44A1 with 44A2 and 44B1 with 44B2. If so, all stators are connected with two conducting wires.
When generating electricity, connect these two conducting wires with (+) and (-) poles of D.C. high voltage generating device.(A simple-system
stator is one that connects all of the stators with one conducting wire and then connects the conducting wire with either of (+) and (-) poles of D.C.
high voltage generating device.). And finally after contacting brush(40) with slip rings(33, 34), fasten it with supporter(39). Now, an electrostatic
induction generator like Figure 23 is completed.
As mentioned above,
I explained the making of an electrostatic induction generator.
But this is not practical but is made for the purpose of experimenting. So in order to put it into practice, the selection of materials and the
method of making need doing differently.