12
1 重力と電磁気力 The Gravitational Force and the Electromagnetic Force* Yoshio TAKEMOTO**, Seishu SHIMAMOTO*** Department of Mechanical and Electrical Engineering, School of Engineering, Nippon Bunri University Abstract This paper provides the matrix which contains the gravitation and the electromagnetic field. We explain that the similarity or difference between the gravitation forces and electromagnetic force. 1. Introduction 1.1. Definition of the imaginary charge and its derivatives The magnetic charge m is a pure imaginary part of the complex charge as i e m , then its potential (1), magnetic field (2), Maxwell equation (3) and the Coulomb-Lorentz force (4) are . 1 i i i ic ( ) r r A 0 0 0 0 m m (1) i c i ic ic E B r A t B t . i i c c c i i c c A A grad rot A div t t (2) . i c i ic 0 r E B t m t B (3)

The Gravitational Force and the Electromagnetic Force

  • Upload
    others

  • View
    9

  • Download
    0

Embed Size (px)

Citation preview

Page 1: The Gravitational Force and the Electromagnetic Force

1

重力と電磁気力

The Gravitational Force and the Electromagnetic Force*

Yoshio TAKEMOTO**, Seishu SHIMAMOTO***

Department of Mechanical and Electrical Engineering, School of Engineering,

Nippon Bunri University

Abstract

This paper provides the matrix which contains the gravitation and the electromagnetic field. We

explain that the similarity or difference between the gravitation forces and electromagnetic force.

1. Introduction

1.1. Definition of the imaginary charge and its derivatives

The magnetic charge m is a pure imaginary part of the complex charge as ie m , then its

potential (1), magnetic field (2), Maxwell equation (3) and the Coulomb-Lorentz force (4) are

.

1ii i

ic ( )

r rA 0 0

0 0

mm

(1)

i c i

ic ic

E B r A

tB t

.

i i cc

ci i c

c

A

Agrad rot A

divt

t

(2)

.

i c i

ic

0 r E B

tm t B (3)

Page 2: The Gravitational Force and the Electromagnetic Force

2

,

i i

ic

F E B 0

t tF E e m (4)

where i i e m e m means a complex conjugate.

1.2. The matrix expression of the mass and its fields like the magnetic charge

It is the same as that of the magnetic charge m . We put the mass M as iM which is a pure

imaginary number, because the two masses has the power of absorption. Then its potential (5),

(magnetic) field (6), Maxwell equation (7) and the Coulomb-Lorentz force (8) are

.

1ii i

i ( )

r rA 0 0

0 0

g

g

MM

G G (5)

i ic

ic ic

E B Ar

gt g

g g g

B t

.

i i cc

ci i c

c

A

Agrad rot A

g

g

g

g g

divt

t

(6)

.

ii c

ic

E B0 r

gt

g g

BM t (7)

,

i i

ic

E BF 0

gtt

g g

BF M this is not

,

i

0

M (8)

where i iM M means a complex conjugate.

2. The matrix which contained the electric charge and the mass simultaneously

2.1 The electric charge and the mass in the same matrix

We put the electric charge e and the magnetic charge m as ( i )1 te m which is the time

component and the mass (1 ,1 ,1 )x y zM which is the space component, which means that the

magnetic charge is on the complex conjugate and the mass is on the space conjugate as follows:

Page 3: The Gravitational Force and the Electromagnetic Force

3

0 ( i )1( i )

(1 ,1 ,1 )

e m Mt

x y z

k e m

GM

0

.

1 0 0 0

0 1 0 0( i )

0 0 1 0

0 0 0 1

0 1 0 0 0 0 1 0 0 0 0 1

1 0 0 0 0 0 0 i 0 0 i 0, ,

0 0 0 i 1 0 0 0 0 i 0 0

0 0 i 0 0 i 0 0 1 0 0 0

k e m

GM

Then we can use the same standard for each unit of the charge ie m and the mass M .

For simplicity, we take the complex charge as i q e m and “the charge and mass” as q M

0 1

(1 ,1 ,1 )

t

x y z

k q

GM. And its potential (9), field (10), the Maxwell equation (11) are

0

11

c (1 ,1 ,1 )

rA

0

ge t

ge x y z

k q

GM

0

.

1

(1 ,1 ,1 )

r

r

t

x y z

k e

GM

(9)

c

ic c

E B Ar

get ge

ge ge ge

E t

.

cc

ci c

c

A

Agrad rot A

ge

ge

ge

ge ge

divt

t

(10)

0 0

.

1 c

(1 ,1 ,1 ) ic

q M

E Br

t get

x y z ge ge

q Et

M (11)

Page 4: The Gravitational Force and the Electromagnetic Force

4

2.2. Maxwell Equation and the temporary unit

(i) The temporary unit of the electron

By the Coulomb force 0

2

k eqF

r , we temporarily define the charge which has the capability to

generate an electric potential as [ ]w Cwe , [ ]w Cwq instead of e , q and 0

2 2

w wk eq e qF

r r .

By the equation of motion

2

2

d

de e

rF m m

t (Newton), we temporarily define the mass of the

charge which has the difficulty [ ]e kgim m of moving to the electromagnetic field.

More specifically, the symbol [ ]w Cwe is the physical meaning that the quantity [ ]w kgwe can

accelerate the mass [ ]e kgim by the value

2

2

d

d

r

t. In this case the units kgi and kg are same and by

the relation 3 2 2

2

220[ /( )]

2 2[ / ]1 1

kgi m C sw

kgi m s

k eeF , we get 1 3 3 2 2

2 20 [ ][ /( )]

[ / ]w Ckgi m C s

Cw kgi m s

e k e

.

(ii) The temporary unit of the mass

By the Universal gravitation of Newton2

GMm

Fr

, We temporarily define the mass which

has the capability to generate a gravitational potential as [ ]w kgwM , [ ]w kgwm instead of M , m and

2 2 w wM mGMm

Fr r

.

By the equation of motion

2

2

d

d

rF m m

t (Newton) and more we temporarily define the

mass of the particle which has the difficulty [ ]i kgim m of moving to the gravitational field.

More specifically, the symbol [ ]w kgwm is the physical meaning that the quantity [ ]w kgwm can

accelerate the mass [ ]i kgim by the value

2

2

d

d

r

t. In this case the units kgi and kg are same, and

by the relation 3 2 2

2

22[ /( )]

2 2[ / ]1 1

kgi m kg sw

kgi m s

G mmF , we get 1 3

2 2[ / ] w

kgw kgi m s

m

Page 5: The Gravitational Force and the Electromagnetic Force

5

3 2 2 [ ][ /( )] kgkgi m kg s

G m .

2.3. The Coulomb and the Gravitational Force of “the charge and the mass”.

We defined a source 1

(1 ,1 ,1 )

w t

ww

w x y z

q

M

q M ,potential

c

ge

ge

A

,fieldic

get

ge ge

E

E Band particle

0 ' 1

' (1 ,1 ,1 )

ge w t

ge w x y z

u q

M

uare as

above 2.1.

Furthermore, we expect the Coulomb and the Gravitational force as

.

' 1

ic ' (1 ,1 ,1 )

E BF

get w tt

ge ge w x y z

E qF

M (12)

But this is not the same size matrix. Therefore we take the variation method as follows1)

:

We put0

cc c

cc

P p A

wge

wge

qEE

Min the previous paper, then

0

.

'c d c

( ) 0 cicdc

'c

E Br uP

ge

wget

ge ge ge

w

uE q

EtTr

M

(13)

Concretely when the particle is not move, the potential (9) and field (10) are

1( , ) q M

r

.

1 0 0 0

0 1 0 0

0 0 1 0

0 0 0 1

0 1 0 0 0 0 1 0 0 0 0 1

1 0 0 0 0 0 0 i 0 0 i 0, ,

0 0 0 i 1 0 0 0 0 i 0 0

0 0 i 0 0 i 0 0 1 0 0 0

w

w

q

M

(14)

Page 6: The Gravitational Force and the Electromagnetic Force

6

3

1( , ) E q M

r

0

0 i i

i 0 i

i i 0

0 0 i i1 0 0 0 1 0 0 0 0 i 0 i 1

0 1 0 0 0 1 0 0 i 0 00 0, ,

0 0 1 0 0 0 1 0 0 0i 0 0

0 0 0 1 0 0 0 1 i 0 0i 0 0

w

w w w w w

x y z

x z yM

y z x

z y x

z y z x

z xy zq x M q y M q z

x zz y

x zy z.

0 i i 00 0 0

0 1 0 0 i 0 0

0 0 1 0 i 0 0

0 0 0 1 0 0

w

y x

y xM

x y

x y

(15)

Additionally, we calculate the above trace (13).

(i) When 0 r (time component)

0d

c( ) ({ ' ( ic ) ' }) 0dc c c

u

E Bge ge

get w ge ge w

Eu

Tr Tr E q M .

(ii) When c 0 t (space component)

0d( ) ( ' ( ic ) ' i( ic ) ' )dc c c c

ge ge ge

get w ge ge w ge ge w

uTr Tr E M q M

u uPE B E B .

For simplicity we limit the x -direction.

The charge and the mass is 1

(1 ,1 ,1 )

q M

w t

w w

w x y z

q

M

.

1 0 0 0

0 1 0 0

0 0 1 0

0 0 0 1

0 1 0 0 0 0 1 0 0 0 0 1

1 0 0 0 0 0 0 i 0 0 i 0, ,

0 0 0 i 1 0 0 0 0 i 0 0

0 0 i 0 0 i 0 0 1 0 0 0

w

w

q

M

Page 7: The Gravitational Force and the Electromagnetic Force

7

And the electric and the gravitational field is ( , )E q M

3

.

0 0 0

0 0 0

0 0 0 i

0 0 i 01

0 0 0 0 0 0 i 0 0 i 0

0 0 0 0 0 0 0 0 0, ,

0 0 0 0 0 0 i 0 0 0

0 0 0 i 0 0 0 0 0 0

w

w w w

x

xM

x

x

r x x x

x x xq M M

x x x

x x x

Therefore we calculate the trace

0'

c c( )

ic'

c

0E Br u

ge

wget

ge ge ge

w

uq

EtTr

M

.

(The time component)

0d

c( ) ( ' ( ic ) ' ) 0dc c c

ge ge

t get w ge ge w

Eu

F Tr Tr E q M

u

E B .

(The space component)

0d( ) ( ' ( ic ) ' i( ic ) ' )dc c c c

ge ge ge

get w ge ge w ge ge w

uTr Tr E M q M

u uPF E B E B ,

where

0 0 0 0 1 0 0

0 0 0 1 0 0 0' '( ' ) ( ) 4

0 0 0 i 0 0 0 ic c c

0 0 i 0 0 0 i 0

ugex w w w wget w

x

xM M M MTr E M Tr x

x

x

,

0

0 0 0 1 0 0 0

0 0 0 0 1 0 0' '(( ic ) ' ) ( ) 4

0 0 0 0 0 1 0c c c

0 0 0 0 0 0 1

E Bge w w w w

ge ge x w

x

u xq q q qTr q Tr x

x

x

,

Page 8: The Gravitational Force and the Electromagnetic Force

8

( i( ic ) ' )c

u

E Bge

ge ge wTr M

0 0 0 i 0 0 0 1 0 0 i 0 0 0 1 0

0 0 0 0 0 i 0 0 0 0 0 0 0 i' '(i i )

0 0 0 0 i 0 0 i 0 0 0 1 0 0 0c c

i 0 0 0 1 0 0 0 0 0 0 0 i 0 0

w w w w

x x

x xM M M MTr

x x

x x

' '4 4

c c w w w wM M M M

x x .

Therefore the space component

0

.

' 'd( ) ( ' ( ic ) ' i( ic ) ' ) 4( 3 )dc c c c c c

u uP

F E B E Bge ge ge w w w w

get w ge ge w ge ge w

u q q M MTr Tr E M q M

As a result, this shows that the universal gravitation has 3 times as the much relation as

electromagnetic power; we think that this reason is that the time is one-direction and the space is a

three-direction.

3. The planet and atom

3.1. Angular momentum

The hypothesis about electron arrangement (orbit).

"The electron which is not excited is arranged one by one so that it may become a fixed angular

momentum (the amount of resonance)."

Example 1 (Hydrogen nucleus H ) the ionization energy is 13.598 VHE e

We put the circular orbit radius 1r of the electron which is not excited. Then the speed is

2

0 01

2

1 1

( )c ce

R k ev

r m r by the balance equation

22 01

1 0( ) ( )c e

k evr R

m . Therefore the momentum

is 2

1 1 1 0 1 0c ( )2

e e e

hm rv m r R m rk e

where 2

34

[ / ]1.05457 10

kg m s

.

Example 2 (Helium nucleus He) the ionization energy is 54.416 V( 4) HHe

E e E

We put the circular orbit radius 11 '

2

rr , 0 0' 2R R of the electron which is not excited. Then

Page 9: The Gravitational Force and the Electromagnetic Force

9

the speed is 10 01

1 1

2''2

c ' c

vR Rv

r r by the balance equation

22 01

1 0

2''( ) '( )

c e

k evr R

m

02R .

Therefore the momentum is 11 1 1 1 1' ' (2 ) ( )

2e e e

rm r v m v m rv .

Example 3 (Lithium atom core2Li

) the ionization energy is 2 122.451 V( 9) HLiE e E

We put the circular orbit radius 11 ''

3

rr , 0 0'' 3R R of the electron which is not excited. Then

the speed is 10 01

1 1

3''''3

c '' c

vR Rv

r r by the balance equation

22 01

1 0

3''''( ) ''( )

c e

k evr R

m

03R .

Therefore the momentum is 11 1 1 1 1'' '' (3 ) ( )

3e e e

rm r v m v m rv .

Moreover, it can be concluded that the point 1r

n of resonating according to the strength of an

electric field is near in inverse proportion to the number n of the protons in a core. Thereby, a

hypothesis can be prepared, saying, "The angular momentum of non-excited electron is constant

which was not depended on the number n of the protons in a core."

3.1.1. The electron around the atomic nucleus

Here, we define the resonance value 2 2

161 1

[ /( )][ ] [ ]

6.58205 101

e

kg m C sC C

m rvk

e as the point of

the resonance instead of angular momentum 1 1 em rv in the hydrogen atom, moreover this

resembles the resonance of the whistle, and the resonating point becomes near in proportion to the

value of a central electric charge q.

3.1.2. The planet and the satellite for solar system

In the case of the planet which goes around the Sun, the resonating point becomes far in

proportion to the mass M of a central star, therefore we define the resonance value

2

1 1

[ /( )]

is

m kg s

m rvK

m M

(where m is the mass and im is the inertial mass), as the point of the

resonance instead of angular momentum, moreover this resembles the relation of the size and pitch

Page 10: The Gravitational Force and the Electromagnetic Force

10

of a drum.

3.1.3. The calculation for the resonance value K

It takes into consideration that universal gravitation has 3 times as much relation as

electromagnetic power in the last of the section 2. We take a standard value of the resonance

2 2 2

15

[ / ] [ /( )]3 1.97461 10

s C kg m kg s

K k in the planet and each point of the resonance is

measured as follows:

Example 4 The resonance value 0 rv

KM

of the planet around the Sun

We calculate the resonance values of the Venus, the Earth and the Mars as follows;

(i) The orbital speed of the Venus is 4

[ / ]3.5020 10 m sv and the distance between the Venus

and the Sun is 11

[ ]1.08204 10 mr .

Then we get the value 2

15

0 [ /( )][ ]

1.90516 10m kg s

kg

rvK

M

.

(ii) The orbital speed of the Earth is 4

[ / ]2.9783 10 m sv and the distance between the Earth and

the Sun is 11

[ ]1.49598 10 mr . Then we get the value 2

15

0 [ /( )][ ]

2.24013 10m kg s

kg

rvK

M

.

(iii) The orbital speed of the Mars is 4

[ / ]2.4128 10 m sv and the distance between the Mars and

the Sun is 11

[ ]2.27942 10 mr . Then we get the value 2

15

0 [ /( )][ ]

2.76518 10m kg s

kg

rvK

M

.

By (1), (2) and (3), the standard value of the resonance 2

15

[ /( )]1.97461 10

s m kg s

K is

between the Venus and the Earth.

In order to take out a better point, although there is no basis in particular. But we take the value

2

15

[ /( )]

2( ) 2.42 102

m m kg s

Venus EarthMars

K mean

(no reason), 2

1 m

Mr K

G ,

Page 11: The Gravitational Force and the Electromagnetic Force

11

1

m

Gv

K as a point of the resonance.

This formula is no reason, but this is near the value 2

15

[ /( )]2.23 10

m kg s

by a method of least

squares to resonance among Jupiter to Pluto. Therefore we get the next table 1.

Table 1

Ratio of the resonance point for the planet.

Mercury (mean) Jupiter Saturn Uranus Neptune Pluto

Orbital radius[m] 5.79E+10 (1.75E+11) 7.78E+11 1.43E+12 2.88E+12 4.50E+12 5.92E+12

Orbital speed [m/s] 4.79E+04 (2.76E+04) 1.31E+04 9.64E+03 6.79E+03 5.43E+03 4.74E+03

Resonance[m2/(kg・s)] 1.39E-15 2.42E-15 5.11E-15 6.92E-15 9.82E-15 1.23E-14 1.41E-14

Ratio of resonance 0.58 1 2.11 2.86 4.06 5.08 5.82

The value of the set (Venus, Earth, Mars) is 1, then the value of Jupiter , Saturn, Uranus,

Neptune ,Pluto is about 2, 3, 4, 5, 6 respectively.

We compare two resonance value the mean value and the standard value, and its ratio is

15

[ ]15

2.42 10( ) 1.225

1.97 10i s

m meanR

m K

.

This is equivalent to having estimated the weight of the central star R times greatly. And the

mercury is very closed to the Sun, therefore its orbit is elliptic and its rotation is affected in

revolution.

Example 5 The resonance value 0 rv

KM

of the satellite around the planet

We calculate the resonance values of a satellite around the planet as follows;

By two formula 1 1rvK

M (resonance) and

2

1 1rv GM (balance equation in the circle orbit), we

get the expected the minimum orbital radius of the satellite 4 2 2

3

[ ]2

1[ ] [ /( )]

[ /( )]

kg

m m kg s

m kg s

Mr K

G

.

For example, the case of the Earth and the moon, the orbital radius of the moon is 3.84×108 m,

the orbital speed is 1.018×103 m/s and the Earth mass is 5.977×10

24 kg. Therefore the position of the

satellite expected is 2 5

1 4.27614 10R M

r K mG

≒ , where the mass of the central star is being

corrected in R double here. This value 5

1 4.27614 10≒r m means that it's inside the equatorial

radius 6378000 m of the Earth. At other planets, the expected radius 1r is inside the equatorial

Page 12: The Gravitational Force and the Electromagnetic Force

12

radius except for Jupiter only.

The ratio of the resonance point can change by the square root of the radius, because

1 1 1 1

1

rv r rGGR MK

R M R M r R M

. Therefore we get the next table 2.

Table 2

Square root of ratio of the radius for the planet.

Earth Jupiter Saturn Uranus Neptune Pluto

Mass[10^24kg] 5.977 1899 568.8 86.67 103 0.012

Expected r1[m] 4.28E+05 1.36E+08 4.07E+07 6.20E+06 7.37E+06 8.59E+02

Equatorial

radius[m] 6.38E+06 7.15E+07 6.03E+07 2.56E+07 2.48E+07 1.14E+06

Stationary

orbit[m] 4.22E+07 1.59E+08 1.09E+08 8.47E+07 9.37E+07 1.84E+07

Proximity

radius r0[m] 3.84E+08

(Moon)

1.28E+08

(Metis~)

1.34E+08

(Pan~)

4.98E+07

(Cordelia~)

4.82E+07

(Naiad~)

1.96E+08

(Charon~) 0

1r

r

29.97 0.97-14.92 1.81-24.54 2.83-58.06 2.56(?)-81.03 150.94-274.61

4. Conclusion

The gravity force is very similar to the electronic force but has 3 times power. The planet

arrangement is similar to the electron arrangement but is little influenced by its inner planet.

References

[1] Y. Takemoto, A Gauge Theory on the Anti-de Sitter Space, Bull. of NBU, Vol. 34, No.1

(1993-Feb.) pp.99-115.

[2] Y. Takemoto, New Notation and Relativistic Form of the 4-dimensional Vector in Time-Space,

Bull. of NBU, Vol. 34, No.1 (2006-Mar.) pp. 32-38.

[3] Y. Takemoto, A New Form of Equation of Motion for a Moving Charge and the Lagrangian, Bull.

of NBU, Vol. 35, No.1 (2007-Mar.) pp. 1-9.

[4] Y. Takemoto, S. Shimamoto, The Electric Charge and the Imaginary Charge, Bull. of NBU, Vol.

42, No.2 (2014- Oct.) pp.1-12.