sr theory of electrodynamics for relative moving charges by james keele, m.s.e.e. october 27, 2012

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SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

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Page 1: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

SR Theory of Electrodynamics for Relative Moving Charges

By James Keele, M.S.E.E.October 27, 2012

Page 2: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Special Theory of Relativity (SRT)

Basic Postulates1. Relativity Principle(RP): “all inertial frames

are totally equivalent for the performance of all physical experiments”

2. “light travels rectilinearly with constant speed c in vacuum in every inertial frame”

Page 3: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Logic applied to the 2nd Postulate: Constancy of the Speed of Light.

If Physicists accept the law, , and believe that and are constant in all inertia frames then must be constant in all inertial frames. Otherwise, if and/or are/is not constant in all inertial frames, because is not constant, then Postulated 1 is invalid because the electrodynamics laws of nature contain these constants.

o o

o

1c

o

oo oc

o

o

oc

Page 4: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Other Basic Considerations

1. The charge of an electron or proton is mathematically considered herein to be a point charge and does not have a finite size.

2. An uniform electric field exists about a stationary electric point charge, pervading the space equally in all directions and falling off in intensity at 1/r2.

3. Velocities are relative between interacting particles.

Page 5: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Other Basic Considerations Cont’d4. The electric field of a moving charge pervades all the space of its inertial frame, thus having instant reaction with a charge in contact with it. Acceleration of a charge creates a new velocity that changes the electric field that spreads out over the new inertial frame at the speed of light.5. The charge value, q, is invariant from one inertial frame to another.6. A positive sign on the overall magnetic force represents repulsion while a negative sign represents attraction. 7. A negative sign must be entered into the equations for negative charges such as electrons. A positive sign must be entered into the equations for positive charges such as protons. This makes the direction of the overall force appear correctly as in 6 above.

Page 6: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

SRT Formalism Employed

1. Lorentz Transformation2. Three Vectors: a(a1, a2, a3) (lower case)3. Four Vectors: V(V1.V2.V3,V4) (Upper case)Four vector force formula:

4. The four vector force is good for transforming force between inertial frames and creating force laws.

5.

F

2c

,vf

fF v

22 c/1/1 vv

Page 7: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Mathematical Setup for Analysis of Force Between Relative Moving Charge Particles

Page 8: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Lorentz Force Law—Starting Point for the Four-Force SRT Transformation

Relativist’s Starting Point Lorentz Force Law (Wrong)

(1)Keele’s Starting Point (Right)

(2)

f=3-force, q=charge, e=electric field, v=relative velocity, h=magnetic field, c=velocity of light

2c

qhv

ef

ef q

Page 9: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Why Relativist’s Starting Point is Wrong1. When we are just trying to derive the force between a stationary charge and a moving charge the Lorentz Force Law that contains the magnetic field is the wrong starting point. If we include the term that has the magnetic field and assume it comes from the moving charge itself, then we would be doing a transform from two different inertial frames which is a “no-no” in SRT. If the term involving the magnetic field arises from a separate source other than the moving charge, then the transform would work for the transform of magnetic field. But we are not doing that, so we can expect the magnetic force to fall out of the transform of just the moving charge’s electric field. This was found to be the case. The is the most important point of this whole presentation that shows where errors are made.

2. The regular Lorentz Force Law could be applicable in Cathode Ray Tube or accelerators where the source of the magnetic field is separate from the “magnetic field” created by the moving charge. You don’t start out in two different inertial frames.

3. An experiment performed by Keele with his results shows that his is the correct starting point.

4. The magnetic field h in (1) is derived from the Biot-Savart Law which was derived before the Old Ampere’s Law from current flowing in a wire. The magnetic field from a moving isolated charge is different from the magnetic field of a current element as will be shown in a later slide.

Page 10: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Transformation Results

Relativist’s Results

(3)

Keele’s Results(4)

evh c

1

3/222233 sinc/-1

q

vr

re

Page 11: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Length Contraction of e-field of Moving Electron as seen by a Stationary Particle

Page 12: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Magnetic Force Between Relative Moving Isolated Charges

Total electric field and magnetic forces between the relative slow moving charges (after mathematical manipulations of (4) using the Binomial Theorem and eliminating higher orders of ) :

(5)

Subtracting the stationary electric field force from (5) we have the magnetic force:

(6)

22 c/v

22

2

31221

12m cos5.15.0c

qkq

v

r

rf

2

2

2

31221

12 cos5.15.0c

1qkq v

r

rf

Page 13: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Current Element

Length contraction of the spacing between charges in the current element increases the charge line density of the current element as seen by a stationary observer (γσ).

Stationary Electrons

Stationary Protons

Moving Electrons --- showing length contraction of each charge’s field and the length contraction of the spacing between the charges in the current element

Page 14: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

The Magnetic Force Law Between a Stationary Charge and a Stationary Current Element

Include one more relativistic effect to (4) for a current element (current flowing in a short piece of a conductor): This effect is length contraction of the spacing between the current carrying electrons in the current element as seen by the stationary charge. This has the effect of increasing the charge density of the current carrying electrons in the current element. The result is:

(7)Where σ is the line charge density.Notice there is a small magnetic force on a stationary charge with respect to the current element.

22

2

31221

12m cos5.11c

dskq

v

r

rf

Page 15: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Eq. (7) is applied three times to the cross combinations of charges in the two current elements and then the resulting forces are added. The charges in (7) are replaced by resulting in the Old Ampere’s Law:

(8)A study of this law reveals that successive current elements with current in the same direction repel each other. This fact has been demonstrated by experiments of Peter Graneau. This is an effect the Biot-Savart Law does not allow. Eq. (8) obeys Newtons 3rd Law whereas most other similar laws do not. They generally have to be integrated around a closed loop to have any applicability.

The Magnetic Force Law Between Stationary Current Elements (Found to Be the Old Ampere’s Law)

sv'ds/ I

12212222121

1212mˆˆˆˆ3ˆˆ2

c

dsdsIkIˆ rsdrsdsdsdrf 111

r

Page 16: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Equivalent Mathematical Form of Old Ampere’s Law

Eq. (9) below is mathematically equivalent to Eq. (8) in the previous slide:

(9)

where = unit vector in the direction of r12 and r12 = magnitude of the vector r12 joining the two current elements. The constants are k = 1/40 (0 = permittivity of free space) and c = speed of light. The I1 and I2 are current magnitudes and ds1 and ds2 are current element lengths. The angles are: 1 = angle between ds1 and r12; 2 = angle between ds2 and r12; = angle between the plane of ds2 with r12 and the plane of ds1 with r12.

2121212

22121

1212m coscoscossinsin2c

dsdsIkIˆ

rrf

12r̂

Page 17: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Experiment With the Old Ampere’s Law

A simple experiment was performed on various shapes of one-turn coils. The inductance L of these coils was computer calculated using Ampere’s Law. Then the Inductance was measured by determining resonance of the inductor with a calibrated capacitor. The measured value of L is then compared with the computed value.

Page 18: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Method employed to measure inductance (Lm) of a coil

Calibrated Capacitor

Formulas: , Resonance

Sine Wave Generator

One-turn coil

Frequency Meter

Scope

2

LIE

2

Cf2

1L

2m

Page 19: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

One-turn solenoid set up for calculating its inductance using the old Ampere’s Law

Page 20: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Math showing how inductance may be calculated using a computer

The energy stored between two current elements

and is:

(3)

If both differential lengths and are imagined to move

outward with r to keep angle variables constant, then all the variables in the (…) function are constant and only r varies. The (…) function can then be moved outside the integral sign, and the result of the integration is then:

(4)

Page 21: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Math for one-turn solenoid inductance cont’d

Inserting Eq. (1) into (4), we get:

(5)

From Fig. 1 we know , ,

. To set up (4) for computer integration,

we further set 1 degree, so

(6)

For the present case, . Substituting (6) into (5), we

get:

(7)

where K is a constant.

Page 22: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Math for one-turn solenoid cont’d

Then the total energy stored in the solenoid is:

(8)

where the summation limits prevent counting of infinite self contributions.

Computing for our one-turn solenoid with radius of 0.254m:

(9)

The value of L computed from (9) compares favorably with the measured value; i.e. within 2% of 2.205 micro henries.

Page 23: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Coil Forms

Page 24: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Experimental Results

• Measured and Calculated Results (Wire dia. = 0.635)• Name ds (mm) Lm (microhenries) Lc (microhenries) Δ %• Triangle 2.4 1.914819 1.909496 -0.28• Circle 2.7 2.399168 2.396962 -0.09• Square 2.8 2.717203 2.717502 0.01• 3-D Square 3.2 3.222207 3.223535 0.04• 3-D Tetra 3.1 3.760989 3.765264 0.11

Since no self-inductance relationship of ds was employed in the calculation of Lc , it is deduced quite appropriately from the above table that for the measured and calculated values to agree so closely, the internal inductance of the current element ds must be zero. Varying the ds length on either side of the ones presented above will produce a calculated value of Lc that will be above or below the measured value of Lm.

Page 25: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Computer modeling of a current element to show zero energy stored in its inductance

The self-inductance of the current element wasnot added in the computer model for calculatingthe inductance of single-turn inductors of the various shapes, so the self-inductance needed to be verified to be zero.

End Views of current element

A square cross-section is used in the model to approximate the round cross-section area of the wire current element to make the math easier. Areas are made equal. The current element is divided up into many rectangular parallelpipeds.

Current Element

Page 26: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Current Element LengthA computer model of the current element using the inductance (energy storage) formulation of Ampere’s Law was created. It determined the length of the current element so that there would be no energy storage in it. (The energy stored in each current element was not added in the computer calculations of the previous slide.) The following table shows the comparison between the required length of ds for a match between the calculated values of L with the measured values of L.• Circle coil. Wire dia. a parameter.• Wire dia. (mm) Lm (microhenries) ds (mm) required ds (mm) calculated

• for Lc match for zero inductance in

• current element model • 0.254 2.747 1 1.08• 0.635 2.399 2.8 2.71• 2.134 1.944 12 9.1

Page 27: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Some Conclusions From Experiment

1. The old Ampere Law is the correct one.2. The other magnetic laws derived above: force

between relative moving charges, and the force between a charge and current element are correct since they preceded in derivation of the Old Ampere’s Law.

3. The SRT derivations of these laws are correct.

Page 28: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Some Applications

1. Arc Welding2. Radio Wave Propagation3. Study of Elementary Particles4. Gravity

Page 29: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Arc Welding

A study of the plasma current flow in the arc gap suggests the relative moving positive and negative ions will be pulled together greater than when stationary, and thus will emit energy. (This is analogous to an electron in a hydrogen atom falling from a higher orbit to a lower orbit.) It may be possible to “burn” the material of the plasma this way and thus emit more energy than is output from the welding machine.

Page 30: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Radio Wave PropagationEq. (7) appropriately modified appears to be a natural for the expression of the magnetic field of a propagated radio wave.

(7) Modified by:Remove q1 to go back to the magnetic e-field. Also the following:

, , ,

(10)

This magnetic field acts on a charge like an electric field. Further development is beyond the scope of my present intentions.

22

2

31221

12m cos5.11c

dskq

v

r

rf

223

1222

2max cos5.11c

c/sinI kL

r

rtw rem

v22

2

dsIds

2I

v /c)sin(wtII max22 r Lds2

me

Page 31: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

E-field of Dipole Antenna

E-field is like the e-field between capacitor plates.

DipoleAntenna

e-field

Page 32: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Study of Elementary Particles

Eq. (4) can be used in a Bohr Atom like model for elementary particles since the equations is good for up to the speed of light:

(4)

Page 33: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Gravity

If the gravity can be considered to be a field, and if the gravity field has similar characteristics to an electric field (but much smaller in amplitude), and if the heavenly bodies are treated as mathematical points, then the gravity field of a heavenly body will have the four-force Lorentz Transformation given by Eq. (11).

(11) 3/222233

22

sinc/-1

G

vr

mm

re

Page 34: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Gravity Cont’d

For slow relative moving heavenly bodies (earth in orbit about the sun for example) then Eq. (11) may be reduced to:

(12)This is a new law of gravity.

2

2

2

31221

12 cos5.11c

1G v

r

mm rf

Page 35: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Gravity Cont’d

Eq. (12) was tested in a computer program to see if the excess force (in addition to the Newton gravity law) would produce the Mercury Perihelion Advance.

(12)

2

2

2

31221 cos5.11

c

G v

r

mmexcess

rf

Page 36: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Gravity Cont’d

It did. Table below show the computed results:

Expressed in arc seconds per 100 Earth years. (If Mercury’s advance was measured relative to Earth’s then Mercury’s Advance would be 42.3 calculated according to the computer model.)

Planet Calculated Results Observed Results

Mercury 46.328 43.11

Venus 9.0634 8.624, 8.4

Earth 4.0230 3.38, 5.00

Page 37: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Uses of New Gravity Law

1) May explain why rockets launched vertically travel further than predicted by Newton’s gravity law.

2) Use in accelerating universe ongoing studies.3) Weight of a vertically rotating disc will be non-uniform: The

top and bottom will be heavier, and the sides will be lighter. A horizontal spinning disc should weigh more than the same disc spinning vertically.

Page 38: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Summary of Derived LawsMagnetic Force Between: Relative Moving Isolated Charges:

Stationary Charge and Current Element:

Two Current Elements (Old Ampere’s Law):

Total Gravity Force BetweenTwo Masses:

22

2

31221

12m cos5.15.0c

qkq

v

r

rf

22

2

31221

12m cos5.11c

dskq

v

r

rf

12212222121

1212mˆˆˆˆ3ˆˆ2

c

dsdsIkIˆ rsdrsdsdsdrf 111

r

2

2

2

31221

12 cos5.11c

1G v

r

mm rf

Page 39: SR Theory of Electrodynamics for Relative Moving Charges By James Keele, M.S.E.E. October 27, 2012

Reasons that these Laws are correct:

1) The old Ampere’s law was derived from SRT and found to be the correct one from the experiments performed.

2) The other two magnetic laws are fall-outs of the steps to derive the old Ampere’s, therefore they can be taken as correct.

3) The gravity law was derived by analogy with SRT applied to e-field of an isolated charge. The excess gravity force thus created was found by calculation to be responsible for the perihelion advances of the planets by computer computation. Therefore this law is correct.