Scalar Electromagnetic Transceiver Antennas,

Torroidal Transformer Version,

Scalar Electromagnetic Vector Algebra,

References.

Introduction

There was some information about a Tesla scalar wave also called scalar electromagnetic waves in writings from Thomas Beardon. The scalar wave if it exits is an electrogravitational wave produced by combining two opposing electromagnetic waves. The electromagnetic energy or potential is send into the local gravity field instead because the electromagnetic fields polarities cancel, and is transmitted as an electrogravitational wave.

Scalar Electromagnetic Transceiver Antennas

Electromagnetic waves can be combined so that they are in superposition. Superposition means that the electromagnetic waves occupy the same position in space. When at superposition two electromagnetic waves or wave particles occupy the same position in space. The magnetic polarities of these two sinusoidal shaped waves are opposite in polarity. This cancels the electromagnetic field polarities. The resultant electromagnetic

signals becomes a weak conventional electromagnetic signal; the electromagnetic signals or waves cancel each other. We can make a superposition of electromagnetic waves by transmitting two radio signals from two separate loop antennas. The loop or coil radio antennas are placed in close proximity to each other as shown in figure 1. The antennas are nearly identical in shape and they are identified in the figure 1 as loop antennas a and b.

In the figure 1 we see the electromagnetic signal amplitude 4 from antenna a and electromagnetic signal 5 from from transmitter antenna loop b. These transmitter loops a and b form a scalar electromagnetic wave transmitter.

Transmitter Antennas

Figure 1.

The electromagnetic signals 4 and 5 from the coils cancel each other or nearly cancel reach other and produce the weaker resultant wave form 6. This very weak signal 6 can be detected by a conventional loop antenna r. The scalared radio wave amplitudes 4 and 6 cannot be detect completely by such a single loop coil r. A scalar electromagnetic wave receiver antenna system can detect such scalar waves

like 4 and 5. The l

Scalar Electromagnetic Wave receiver Antennas

Figure 1b.

The scalar wave receiver antenna could detect the scalared waves but the conventional

single loop antenna like r could not detect much electromagnetic signal.

To scalar the original electromagnetic waves the transmitter antenna system a and b needed an electric phase shifter circuit made of inductance L and capacitance C. Figure 2 shows the electronic schematic drawings of the antennas and their corresponding electric circuits and signal currents I

Antenna Circuits and Currents

Figure 2.

The phase shifter circuit values L and C insure that the electric sinusoidal wave form or sine wave current I

this phase angle Ø between the peak values of currents I

The values to calculate phase angle Ø are the distance d between the loop antennas a and b, the electric sine wave frequency f, and the speed of light c of the electromagnetic waves. The equations are: w=c/f, (1); Ø=[360 º×(d÷w)] ±180º=x±q, (2).

With these equations we first shift currents I

x=360 º×(d÷w) in equation (2) is used to calculate and estimate the required values for L and C. The electric phase shifter inductance L and capacitance C are determined by the distance h between transmitter antennas a and b and the electric signal current frequency f.

Demonstration Video 1. Scalared Electromagnetic Waves Transceiver:

http://www.machines-x.info/scalarwaves/ .WMV, file size: kilobytes.

This type of scalar electromagnetic wave may perhaps be a virtual photon wave. A virtual photon a component of a virtual photon wave may be a five dimensional particle that is about to become a real conventional photon. A virtual photon wave may perhaps produce virtual electrons of virtual electronic current I

Scalar Electromagnetic Vector Algebra

At The Transmitter Antennas

Input current magnitudes: I

I

Virtual electronic current in transmitter antennas a and b is:

I

with fourth dimensional component I

Input current vectors into antenna seperatly:

I

I

where current vector component I

The speculative linear transformation of electrical currents from n=3-space to n=5-space in transmitter antennas a and b is:

T:R

for examples: vector components I

Scalar wave or virtual photon field intensity or number of virtual electrons is:

k

Electromagnetic permeability of the local three dimensional vacuum space-time is u

At The Receiver Antennas

Electrical current magnitydes from receiver antennas c and d alone respectively are:

I

I

Virtual photon field intensity in receiver antennas c and d is:

k

where d is the physical distance betwen the scalar wave transmitter and receiver antennas sets. Number of irtual photons at receiver antennas c and d is:

k

Virtual electronic current in receiver antennas c and d is:

I

Output current vectors from antennas c and d separately:

I

Then the speculative linear transformation of electrical currents from n=5-space to n=3-space at receiver antennas c and d is:

T:R

where I

for examples: vector components I

I

Virtual photon wave pseudo energy in 5-space is:

c

with real energy E≈10

k

Conclusion

References

November 21, 2003.