U.S. Patent 6,377,436

Microwave Transmission Using a Laser-Generated Plasma Beam Waveguide

Issued April 23, 2002 to Jed Margolin


ABSTRACT

      A directed energy beam system uses an ultra-fast laser system, such as one using a titanium-sapphire infrared laser, to produce a thin ionizing beam through the atmosphere. The beam is moved in either a circular or rectangular fashion to produce a conductive shell to act as a waveguide for microwave energy. Because the waveguide is produced by a plasma it is called a plasma beam waveguide. The directed energy beam system can be used as a weapon, to provide power to an unmanned aerial vehicle (UAV) such as for providing communications in a cellular telephone system, or as an ultra-precise radar system.



Full Patent     1,403 KB (PDF)
 Specification Only      44 KB (HTML)
 Drawings Only       613 KB (PDF)
Reference: U.S. Patent  5,726,855  (Mourou)  763 KB (PDF)
Other References  746 KB (PDF)



By an interesting coincidence there is an article in the May 2002 issue of Scientific American (page 81) about ultrafast lasers. The article is coauthored by Dr. Gerard Mourou, one of the inventors of the chirped-pulse ultrafast laser.


In the event you are planning on building the device, I strongly urge you to contact me and secure my services in order to bring the device up in a controlled and orderly fashion. Otherwise, unless you build the device exactly as outlined in the Patent Specification, there is a possibility, however small, that it will produce a bang that is much larger than the one you may be expecting.

I believe there is a possibility that, with a few modifications, my invention can be used to produce a fusion reaction. Think linear tokamak.

You didn't think I stopped working on it after I filed the Patent Application, did you?  :-)

Jed Margolin
San Jose, CA
June 7, 2002




Microwave Transmission Using a Laser-Generated Plasma Beam Waveguide

Possibilities to Investigate
 

Jed Margolin



These possibilities are highly speculative, but because of their potential benefits (or consequences) they must be considered.

Possibility #1

Part 1:

If the frequency of the microwave energy is the same frequency as that used by microwave ovens (2.45GHz.), the water molecules in the waveguide will heat up, turning first into steam, and then into a plasma. We can inject water if the humidity is not high enough.

I believe there is a good chance this plasma will be contained by the waveguide due to the intense magnetic field produced by the ultrafast laser.

From the article in Scientific American (May 2002, page 82) written by Gérard Mourou and Donald Umstadter:

"  These compact lasers can fire a hundred million shots per day and can concentrate their power onto a spot the size of a micron, producing the highest light intensities on earth. Associated with these gargantuan power densities are the largest electric fields ever produced, in the range of a trillion volts per centimeter. Such intense laser light interacting with matter re-creates the extreme physical conditions that can be found only in the cores of stars or in the vicinity of a black hole: the highest temperatures, 1010 kelvins; the largest magnetic fields, 109 gauss; and the largest acceleration of particles, 1025 times the earth's gravity."
Part 2:

If this plasma is contained by the waveguide, we would like the plasma to come shooting out the end of the waveguide. This may occur naturally, especially if the beam is tilted above the horizontal. If not, by modulating the microwave energy (amplitude and/or frequency) we may be able to produce systolic action. Think of a standing wave pattern traveling along the length of the waveguide.
 

Part 3:

Being able to produce a blast of plasma through a cross-section of a few inches at long distances (10 KM. or so) would produce a weapon more destructive than I had planned, but would probably be acceptable. (Dead is Dead.)

However, there is a much better use for what I will call the plasma projector.

Since the plasma has mass, it has momentum.

We can use it to power the first stage of a launch vehicle. Since all the fuel for the first stage would come from the ground (and would be water) the launch vehicle would have an extremely high mass ratio. (A high percentage of the mass of the launch vehicle would make it into orbit. Most of the mass of current launch vehicles is in the first stage.)  The launch vehicle would only have to carry its own fuel to continue past the atmosphere (and for maneuvering and de-orbiting).

We can do this with a number of plasma projectors arranged in a circle aimed at the bottom of the launch vehicle which would be in the shape of a large disc.

When it is time to fire the second stage, the disc can be dropped. Alternatively, the disc can be comprised of vanes which can be opened. This has the advantage of giving the launch vehicle some amount of control of the launch, especially for dynamic stability.

The use of water as the primary fuel makes it much more environmentally friendly than the toxic rocket fuels currently used.

If NASA is too embarrassed to develop a launch vehicle that looks something like a flying saucer we will just have to find someone else to do it.


Possibility #2

If the laser-generated plasma beam waveguide, instead of being cylindrical, is conical and comes to a point (gradually, over a long distance, lets say 10KM.) the plasma will also be focused to a point. If the magnetic containment is sufficient, it may produce a fusion reaction at the point of the waveguide. It would be like a linear Tokamak.

There is a potential problem, since the critical dimension of a waveguide must be more than one-half the lowest frequency to be transmitted. As the waveguide narrows it will become less than this, so this is something to look into further.

The reason for using the 10KM. figure is that the ideal shape of this waveguide is an exponential horn, such as used in horn loudspeakers. A cross sectional area that changes exponentially is the optimum shape for matching the impedances of two different pressure areas, but having the cross sectional area change linearly over a long enough distance might be good enough.

If this works, it is possible that such a fusion reaction would propagate back through the waveguide to its source, so I suggest short bursts.

Since a conical waveguide may be produced accidentally simply by making a non-ideal mirror ring, any system must be very carefully designed and tested under controlled conditions.

In any event, this is much more of a weapon than I would like. It would instantly and completely destroy anything it hits, and then some.

One saving grace would be to use it to generate electricity, presumably at a distance considerably shorter than 10 KM., preferably like 2M. I would like that. Perhaps an external magnetic field can be used to shape the waveguide into an approximation of an exponential horn.

Another saving grace would be to use it in a rocket engine. In this case a pressurized cylinder (presumably metal) would be used to contain the atmosphere for ionization by the ultrafast laser and to provide water vapor for the fusion reaction. The idea is to have the energy released by the fusion reaction propel the plasma out the tail end at a very high velocity, thus producing thrust. Since the engine is obviously a mission-critical component, there should be at least two or three of them on the spacecraft.

While we're on the subject of atmospheres, both the Mourou patent and the Scientific American article seem to assume the use of a standard atmosphere for the ultrafast laser. I wonder what the ultrafast laser would do in a pure atmosphere of nitrogen, or hydrogen, or maybe just water vapor, since water vapor is a necessary component anyway. I also wonder what kind of trail the beam of an ultrafast laser would leave if it were aimed into a tank of salt water.


Possibility #3

Lately, I've been wondering about the effects of standing waves in the plasma projector discussed in Possibility #1.  Standing waves are produced in a transmission line when the line is terminated in other than its characteristic impedance. The energy is reflected at the impedance discontinuity; the percentage of energy reflected is a function of the impedance mismatch.

The highest impedance discontinuity occurs when the end of the transmission line is either open or shorted. A conducting plate would qualify as a short and would also provide a handy place for injecting water into the waveguide.

The microwave transmitter can be modulated (frequency and/or amplitude) to control the standing wave pattern.

The question is whether the standing waves would produce alternating areas of plasma compression and rarefaction and whether the compression in the areas of high compression would be high enough to be interesting.


Possibility #4

If you build a device using my patent (after obtaining a license, of course), I would like you to do the following:

1. Measure the frequency of the microwave energy at the end of the waveguide and compare it to the frequency of the microwave transmitter. While there is no reason to believe that the frequency will be different, we are venturing into unknown territory and should be alert for any anomalies.

2. For the same reason you should measure gravity both inside and immediately outside the waveguide. If anything can affect gravity anomalistically at less than galactic distances it would be the intense magnetic field and relativistic electrons produced by an ultrafast laser.

3. Just for grins, measure time inside the waveguide.


Jed Margolin
San Jose, CA
July 4, 2002 
 


Copyright 2002 Jed Margolin


Power Calculations for Directed Energy Weapon
 
Microwave Transmission Using a Laser Generated Plasma Beam Waveguide
Jed Margolin  9/13/2006, posted 8/7/2009
 
Assumptions
 
Circular Waveguide
Frequency       1/2 wavelength diameter           Area                            Area
 2 GHz             2.952   inches                          6.84  sq inches           44.16   sq cm
 4 GHz             1.476   inches                          1.71  sq inches           11.04   sq cm
 6 GHz             0.984   inches                          0.76  sq inches           4.91     sq cm
 
The best commercially available circular metal waveguide is wc281 which has an attenuation of 0.3 db/100 feet.
 
 I expect the plasma beam waveguide to be more efficient than that so I have used attenuation factors of 0.1 db/100 feet and 0.05 db/100 feet.
 
My reason for believing this is:
 
1.  With a metal waveguide, I2R losses heat the metal without materially affecting its conductivity unless it melts the waveguide.
 
2.  With the plasma beam waveguide the I2R losses will heat the plasma, making it more conductive.
 
All calculations are at sea level.
                                                           
1 sq inch =      6.4516 sq cm
 
 
Generic Calculations
 
Pulsed Power
Microwave Transmitter Power = 1 MW
Attenuation (db) =  0.05 db/100 feet
Frequency = 2 GHz.
 
Distance (feet)   Attenuation (db) Power (MW) Power (W) Power Density
   at Target
(W/Sq Inch)
Power Density
   at Target
  (W/Sq cm)
100 0.05 0.9885531 988,553 144,437 22,388
500 0.25 0.9440609 944,061 137,936 21,380
1,000 0.50 0.8912509 891,251 130,220 20,184
5,000 2.50 0.5623413 562,341 82,163 12,735
10,000 5.00 0.3162278 316,228 46,204 7,162
20,000 10.00 0.1000000 100,000 14,611 2,265
50,000 25.00 0.0031623 3,162 462 72
100,000 50.00 0.0000100 10.0 1.46 0.23
 
                                                                                                                                     
 
Pulsed Power
Microwave Transmitter Power = 1 MW
Attenuation (db) = 0.05 db/100 feet
Frequency = 4 GHz.
                                                                                                                                               
Distance (feet)   Attenuation (db)  Power (MW) Power (W) Power Density
    at Target
  (W/Sq Inch)
Power Density
   at Target
  (W/Sq cm)
100 0.05 0.9885531 988,553 577,747 89,551
500 0.25 0.9440609 944,061 551,744 85,521
1,000 0.50 0.8912509 891,251 520,880 80,737
5,000 2.50 0.5623413 562,341 328,653 50,941
10,000 5.00 0.3162278 316,228 184,815 28,646
20,000 10.00 0.1000000 100,000 58,444 9,059
50,000 25.00 0.0031623 3,162 1,848 286
100,000 50.00 0.0000100 10.0 5.84 0.91



Pulsed Power
Microwave Transmitter Power = 1 MW
Attenuation (db) = 0.05 db/100 feet
Frequency = 6 GHz.
 
Distance (feet)   Attenuation (db) Power (MW) Power (W) Power Density
   at Target
 (W/Sq Inch)
Power Density
   at Target
  (W/Sq cm)
100 0.05 0.9885531 988,553 1,299,931 201,490
500 0.25 0.9440609 944,061 1,241,424 192,421
1,000 0.50 0.8912509 891,251 1,171,980 181,657
5,000 2.50 0.5623413 562,341 739,470 114,618
10,000 5.00 0.3162278 316,228 415,834 64,454
20,000 10.00 0.1000000 100,000 131,498 20,382
50,000 25.00 0.0031623 3,162 4,158 645
100,000 50.00 0.0000100 10.0 13.15 2.04
 
_______________________

Pulsed Power
Microwave Transmitter Power = 1 MW
Attenuation (db) = 0.1 db/100 feet
Frequency = 2 GHz.
 
Distance (feet)   Attenuation (db) Power (MW) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.10 0.9772372 977,237 142,783 22,131
500 0.50 0.8912509 891,251 130,220 20,184
1,000 1.00 0.7943282 794,328 116,059 17,989
5,000 5.00 0.3162278 316,228 46,204 7,162
10,000 10.00 0.1000000 100,000 14,611 2,265
20,000 20.00 0.0100000 10,000 1,461 226
50,000 50.00 0.0000100 10 1.5 0.2
100,000 100.00 0.0000000001 0.00010 0.000015 0.000002
 
 
 
Pulsed Power
Microwave Transmitter Power = 1 MW
Attenuation (db) = 0.1 db/100 feet
Frequency = 4 GHz
 
Distance (feet)   Attenuation (db) Power (MW) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.10 0.9772372 977,237 571,134 88,526
500 0.50 0.8912509 891,251 520,880 80,737
1,000 1.00 0.7943282 794,328 464,235 71,957
5,000 5.00 0.3162278 316,228 184,815 28,646
10,000 10.00 0.1000000 100,000 58,444 9,059
20,000 20.00 0.0100000 10,000 5,844 906
50,000 50.00 0.0000100 10 5.8 0.9
100,000 100.00 0.0000000001 0.00010 0.000058 0.000009
 
 
Pulsed Power
Microwave Transmitter Power = 1 MW
Attenuation (db) = 0.1 db/100 feet
Frequency = 6 GHz
 
Distance (feet)   Attenuation (db) Power (MW) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.10 0.9772372 977,237 1,285,051 199,183
500 0.50 0.8912509 891,251 1,171,980 181,657
1,000 1.00 0.7943282 794,328 1,044,528 161,902
5,000 5.00 0.3162278 316,228 415,834 64,454
10,000 10.00 0.1000000 100,000 131,498 20,382
20,000 20.00 0.0100000 10,000 13,150 2,038
50,000 50.00 0.0000100 10 13.1 2.0
100,000 100.00 0.0000000001 0.00010 0.000131 0.000020
 
_______________________
 
Average Power (Equivalent Heating Power)
Microwave Transmitter Power = 100 KW
Attenuation (db) = 0.05 db/100 feet
Frequency = 2 GHz.
 
Distance (feet)            Attenuation (db) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.05 98,855 14,444 2,239
500 0.25 94,406 13,794 2,138
1,000 0.50 89,125 13,022 2,018
5,000 2.50 56,234 8,216 1,274
10,000 5.00 31,623 4,620 716
20,000 10.00 10,000 1,461 226
50,000 25.00 316 46 7
100,000 50.00 1.0 0.15 0.02
 
 
Average Power (Equivalent Heating Power)                                                                                                
Microwave Transmitter Power = 100 KW
Attenuation (db) = 0.05 db/100 feet
Frequency = 4 GHz.
 
Distance (feet)            Attenuation (db) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.05 98,855 57,775 8,955  
500 0.25 94,406 55,174 8,552
1,000 0.50 89,125 52,088 8,074
5,000 2.50 56,234 32,865 5,094
10,000 5.00 31,623 18,482 2,865
20,000 10.00 10,000 5,844 906
50,000 25.00 316 185 29
100,000 50.00 1.0 0.58 0.09



Average Power (Equivalent Heating Power)                                                                                                
Microwave Transmitter Power = 100 KW
Attenuation (db) =  0.05 db/100 feet
Frequency = 6 GHz.
 
Distance (feet)            Attenuation (db) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.05 98,855 129,993 20,149
500 0.25 94,406 124,142 19,242
1,000 0.50 89,125 117,198 18,166
5,000 2.50 56,234 73,947 11,462
10,000 5.00 31,623 41,583 6,445
20,000 10.00 10,000 13,150 2,038
50,000 25.00 316 416 64
100,000 50.00 1.0 1.31 0.20
 
_______________________
  
Average Power (Equivalent Heating Power)                                                                                                
Microwave Transmitter Power = 100 KW
Attenuation (db) = 0.1 db/100 feet
Frequency = 2 GHz.
 
Distance (feet)            Attenuation (db) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.1       97,724 14,278 2,213
500 0.5 89,125 13,022 2,018
1,000 1.0 79,433 11,606 1,799
5,000 5.0 31,623 4,620 716
10,000 10.0 10,000 1,461 226
20,000 20.0 1,000 146 23
50,000 50.0 1 0.15 0.02
100,000 100.0 0.00001 0.0000015 0.0000002
 
 
 
Average Power (Equivalent Heating Power)                                                                                                
Microwave Transmitter Power = 100 KW                                                                 
Attenuation (db) = 0.1 db/100 feet
Frequency = 4 GHz.  
 
Distance (feet)            Attenuation (db) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.1 97,724 57,113 8,853
500 0.5 89,125 52,088 8,074
1,000 1.0 79,433 46,423 7,196
5,000 5.0 31,623 18,482 2,865
10,000 10.0 10,000 5,844 906
20,000 20.0 1,000 584 91
50,000 50.0 1 0.58 0.09
100,000 100.0 0.00001 0.0000058 0.0000009
 
 

Average Power (Equivalent Heating Power)                                                                        
Microwave Transmitter Power = 100 KW
Attenuation (db) = 0.1 db/100 feet
Frequency = 6 GHz.
 
Distance (feet)            Attenuation (db) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.1 97,724 128,505 19,918
500 0.5 89,125 117,198 18,166
1,000 1.0 79,433 104,453 16,190
5,000 5.0 31,623 41,583 6,445
10,000 10.0 10,000 13,150 2,038
20,000 20.0 1,000 1,315 204
50,000 50.0 1 1.31 0.20
100,000 100.0 0.00001 0.0000131 0.0000020
 
 
Specific Calculations
                                                                                                           
Continuous Wave Klystron
            Toshiba                       http://www.toshiba-tetd.co.jp/tetd/eng/electron/e_kly.htm
            Type                                        E3724
            Frequency (MHz)                   2,450
            Output Power (KW)               100
            Efficiency (%)                          60
            Gain (db)                                45
            Beam (KV)                             42
            Beam Current (A)                   4.0
            Weight (KG)                           150
            Length (M)                             1.75
 
            Input Power    167 KW
                                    220 VAC @ 758 A
 
Average Power (Equivalent Heating Power)
Microwave Transmitter Power = 100 KW
Attenuation (db) = 0.05 db/100 feet
Frequency = 2 GHz.
 
Distance (feet)            Attenuation (db) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.05 98,855 14,444 2,239
500 0.25 94,406 13,794 2,138
1,000 0.50 89,125 13,022 2,018
5,000 2.50 56,234 8,216 1,274
10,000 5.00 31,623 4,620 716
20,000 10.00 10,000 1,461 226
50,000 25.00 316 46 7
100,000 50.00 1.0 0.146 0.023
 
 

Average Power (Equivalent Heating Power) (Toshiba E3724)
Microwave Transmitter Power = 100 KW
Attenuation (db) = 0.1 db/100 feet
Frequency = 2 GHz.
 
Distance (feet)            Attenuation (db) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.1 97,724 14,278 2,213
500 0.5 89,125 13,022 2,018
1,000 1.0 79,433 11,606 1,799
5,000 5.0 31,623 4,620 716
10,000 10.0 10,000 1,461 226
20,000 20.0 1,000 146 23
50,000 50.0 1.00 0.15 0.02
100,000 100.0 0.000010 0.0000015 0.0000002
 
 

Pulsed Klystron
            Toshiba           http://www.toshiba-tetd.co.jp/tetd/eng/electron/e_kly.htm
            Type                                        E3746A
            Frequency (MHz)                   5,712
            Output Power (MW)              50
            Efficiency (%)                         47
            Gain (db)                                52
            Pulse Length (us)                   2.5
            Pulse Rate (pps)                     50
            Beam Volt. (KV)                    354
            Beam Curr. (A)                       315
            Weight (KG)                           300
            Length (M)                             1.4
 
            Duty Cycle                              0.000125 = 0.0125 %
            Average Output Power           6.25 KW
            Input Power                            13.30 KW
 
 
Pulsed Power                          (Toshiba E3746A)
Microwave Transmitter Power = 50 MW
Attenuation (db)                     0.05 db/100 feet
Frequency = 6 GHz.
 
Distance (feet)   Attenuation (db) Power (MW) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.05 49.43 49,427,655 64,996,548 10,074,485
500 0.25 47.20 47,203,044 62,071,222 9,621,059
1,000 0.50 44.56 44,562,547 58,599,012 9,082,865
5,000 2.50 28.12 28,117,066 36,973,477 5,730,900
10,000 5.00 15.81 15,811,388 20,791,714 3,222,722
20,000 10.00 5.00 5,000,000 6,574,917 1,019,114
50,000 25.00 0.158 158,114 207,917 32,227
100,000 50.00 0.00050 500 657 102
 
 
 
Pulsed Power                                                                                                 
Microwave Transmitter Power = 50 MW
Attenuation (db) = 0.1 db/100 feet
Frequency = 6 GHz.
 
Distance (feet)   Attenuation (db) Power (MW) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.10 48.86   48,861,861 64,252,539 9,959,163
500 0.50 44.56 44,562,547 58,599,012 9,082,865
1,000 1.00 39.72 39,716,412 52,226,424 8,095,112
5,000 5.00 15.81 15,811,388 20,791,714 3,222,722
10,000 10.00 5.00 5,000,000 6,574,917 1,019,114
20,000 20.00   0.50 500,000 657,492 101,911
50,000 50.00 0.00050 500 657 102
100,000 100.00 0.000000005 0.0050 0.007   0.001
 
 
 
Pulsed Klystron
            Toshiba           http://www.toshiba-tetd.co.jp/tetd/eng/electron/e_kly.htm
            Type                                        E3787
            Frequency (MHz)                   2,700-2,900
            Output Power (MW)              1.6
            Efficiency (%)                         46
            Gain (db)                                53
            Pulse Length (us)                      4
            Pulse Rate (pps)                     200
            Beam Volt. (KV)                    79
            Beam Curr. (A)                       44
            Weight (KG)                           39
            Length (M)                             0.9
                                                                                                           
            Duty Cycle                              0.0008 = 0.08 %
            Average Output Power           1.28 KW
            Input Power                            2.78 KW                                            
                                                                                                           
                                                                                                           
Pulsed Power
Microwave Transmitter Power = 1.6 MW
Attenuation (db) = 0.05 db/100 feet
Frequency = 2 GHz.
 
Distance (feet)   Attenuation (db) Power (MW) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.05 1.58 1,581,685 231,099 35,820
500 0.25 1.51 1,510,497 220,698 34,208
1,000 0.50 1.43 1,426,002 208,352 32,295
5,000 2.50 0.90 899,746 131,461 20,377
10,000 5.00 0.51 505,964 73,926 11,459
20,000 10.00 0.16 160,000 23,377 3,624
50,000 20.00 0.016 16,000 2,338 362
100,000 50.00 0.000016 16.0 2.3 0.36
 
 
 
Pulsed Power              (Toshiba E3787)
Microwave Transmitter Power = 1.6 MW
Attenuation (db) = 0.1 db/100 feet
Frequency = 2 GHz.
 
Distance (feet)   Attenuation (db) Power (MW) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.10 1.56 1,563,580 228,453 35,410
500 0.50 1.43 1,426,002 208,352 32,295
1,000 1.00 1.27 1,270,925 185,694 28,783
5,000 5.00 0.51 505,964 73,926 11,459
10,000 10.00 0.16 160,000 23,377 3,624
20,000 20.00 0.016 16,000 2,338 362
50,000 50.00 0.00002 16.0 2.3 0.4
100,000 100.00 0.00000000016 0.00016 0.000023 0.000004
 
 
 
 
Recommendations
                                                                                                           
Although a pulsed klystron has a low average power, the high intensity pulses will fry electronics and may detonate ordnance by triggering the detonators.
                       
The continuous wave klystron will produce heating.
 
I recommend pairing a pulsed klystron (Toshiba E3787) with a continuous wave klystron (Toshiba E3724).
 
Note: The power calculations do not include the power required by the ultrafast lasers.
                                                                                                           
                                                                                                           
Summary
                                                                                               
E3724              Input Power    167 W
Continuous Wave Klystron    220 AC @ 758 A
 
Average Power (Equivalent Heating Power)
Microwave Transmitter Power = 100 KW
Attenuation (db) = 0.05 db/100 feet
Frequency = 2 GHz.
 
 
Distance (feet)            Attenuation (db) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.05 98,855 14,444 2,239
500 0.25 94,406 13,794 2,138
1,000 0.50 89,125 13,022 2,018
5,000 2.50 56,234 8,216 1,274
10,000 5.00 31,623 4,620 716
20,000 10.00 10,000 1,461 226
50,000 25.00 316 46 7.2
100,000 50.00 1.00 0.15 0.023
 
 

E3787
Pulsed Klystron  
            Duty Cycle                  0.0008 = 0.08  %
            Average Output Power 1.28 KW
            Input Power                 2.78 KW
 
Pulsed Power
Microwave Transmitter Power = 1.6 MW
Attenuation (db) = 0.05 db/100 feet
Frequency = 2 GHz.
 
 
Distance (feet)   Attenuation (db) Power (MW) Power (W) Power Density
   at Target
  (W/Sq Inch) 
Power Density
  at Target
 (W/Sq cm)
100 0.05 1.58 1,581,685 231,099 35,820
500 0.25 1.51 1,510,497 220,698 34,208
1,000 0.50 1.43 1,426,002 208,352 32,295
5,000 2.50 0.90 899,746 131,461 20,377
10,000 5.00 0.51 505,964 73,926 11,459
20,000 10.00 0.16 160,000 23,377 3,624
50,000 20.00 0.005 5,060 739 115
100,000 50.00 0.000016 16.0 2.3 0.36
 
 
 
The effects of this directed energy on various targets
 
1.  Aircraft - The pulsed segment will disable the aircraft’s electronics. The CW segment will cause local heating and weakening of the aircraft structures. Aerodynamic forces will cause the aircraft to break up in flight.
 
2.  Missiles - As with aircraft, the pulsed segment will disable the missile’s electronics. The CW segment will cause local heating and weakening of the missile structures. Aerodynamic forces will cause the missile to break up in flight. Additionally, the missile fuel may detonate, especially with missiles using solid rocket motors.
 
3.  Humans - The most effective shot is the head shot. The brain will absorb the microwave energy and quickly boil, causing the brain to explode out through the ears, nose, mouth, and eye sockets.
 
 
This directed energy is a lethal weapon and may not, under any circumstances, be characterized as a non-lethal or less-than-lethal weapon. These are morally bankrupt terms when used with weapons which have the ability to be lethal or cause permanent damage to humans.
 

 


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