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1 UCRL-ID B - High Energy Gull Generator (Owl Note #24) W.Stephens DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof. 1 w(date unknown) This is an informal report intended primarily for internal or limited external distribution. The opinions and conclusions stated are those of the author and may or may not be those of the Laboratory. Work performed mdez the auspices of tbe U.S.Department of Energy by the Lawrence Livemore National Laboratory under Contract W-7405-ENG-48..,:,._.:4,:.:,
2 DISCLAIMER Portions of this document may be illegible in electronic image products. hag= are produced from the best available original document.
3 I. I' Owl Note Number 24 William H. Stephens DECLASSIFICATION STAMP ON REVERSE- Acrpoee The pw'yose of this experiment was to demonstrate that a G u l l type generator could be msde which would produce currents greater than 2 X lo8 amperes in inductances sufficiently large to posaess an electrical energy on the order of 108 joules. current of 2.5 X 108 amgems. The 'melectrical energy associated with this current was on the order of 4 X 107 joules. The generator produced a Analysis of Results The experiment consisted of a 9Og generator, a 5 foot coax extension and a 20 inch cone section. (See setup photo) ~ i g hexplosive was lighted at the 909 generator end and burned through the emeture into the cone. Inductance was wiped out as the burn Front progressed. The current produced was measured by three separate probes located i n the last of the cone section. The shot was fired a t Bunker 350 on Wednesday, 23 Wmmiber 1960 after considerable d e l a y s due t0 weather and engineering problems w i t h the joints. A l l disgnostlcs worked satisfactorily. Rraaing camera pictures showed the joints held without visible arcing. Predicted "I vs t" curve ~ I X lo6 w s h load. mot 914L The data from 9OgA indicated that a current of -5 * could be produced by t h e 909 generator i n a -.2 tisee showed that 8 coax type generator multiflied so I&= 3 2 at low level had produced a current of 7 X 107 amps in a foot coax section. The t curve "pkdicted current vs tine" wa8 our best estimate of the output of the 9ogB Shot generator based on the above date. We thought the current m l g h t turn over near the end due t o high field limitations and energy loas in the walls.
4
5 Experimental "I VB t" curve The "I v8 ti' curve was p l o t t e d from oscilloscope traces. The d a t a was plotted and the best curve was &an through the data points by eye "Ais "smoth curve" I s the one shown. The data from t h e three separate probes agreed quite well and there waa no large diviations from the smooth curve. Inductance vs tine curve The inductance a8 a f h c t i o n of pasition u i t h i n the been open t o question f o r somi? time. (cone angle 5 : 1&the B B I I ~8s ~~ attached t o an armature and wa8-909 generator has "o settle this question a metal cone the observed unpertubed cone angle) was made rnechmically pulled through the generator. distance" i n the 909 generator was measured in this manner. This data was used in calculating the energy. The lneasured value of L is the part of the "L vs t" c m from 380 psec to 480 vsec. ~ r o m480 psec to 628 psec the cone is i n the 5 foot coax and the v d u e s i n this region were hand calculated. The inductance f+rcxn628 psec on were calculated by Jim FBulkner. Values of L beyond 660 psec s h a d not be considered reliable due to motion of the wall of the cavity which was under high magnetic pressure for a long period of tine. The lower or minimum energy extrapolation was ms&e huwever using these calculrttioas. The "L VB Enerm v1s time The *'E vs t" curve wa8 obtained usfng the ''1 vs t" and the "L vs t" data. There are several interesting facets t o the energy curve. The f i r s t i s the early peak snd lo58 of energy a t 412 wsec t o 430 psec. The cone a t the p e e had just entered the first turns (6 turns per inch f o r six inches) and the recovery i n the energy occurs at the t i n e the cone left the 6 t u r n s per inch section. h i s indicates possible arcing tum t o turn caused by overloading (to0 hi& I, - 2 X lo4 amps). W A had an Io of 1.4 X 104 amps and i t s "E Vs t" curve ahowed a very small plateau a t this sane point. After recovery t h e 9OgB epergy curre WBB very similar to that of goga. Extrapolation of the energy c d v e from the peak at 412 psec parallel to the recovery slope, gives the predicted edrrent c m e. Had less energy been put i n the gogb it appears it vould have p u t out twice the cun.ent and four tines the energy i n the coax section.!&e second i n t e r e s t i n g p o i n t i n the energy curve is that the current
6 multiplication in the 5 foot coax was very high (-75% theoretical) even though it to& 200 psec to wipe out. Ftnally the energy beyond 600 psec i t 3 difficult to determine w i t h any degree of accuracy due to the changing inductance caused by the motion of the w a l l s under t h e inf'luence of the high magnetic fields. As previously mentioned the L w i l l be larger than a 13b3tlc calculation would indicate. The extrapolation (marked) (Min 90 energy u n i t s ) ie the energy using the static case. The extrapolation (marked) ox-x(bfpx 400 energy units) is obtained by extrapolation using the high efficiency shown in the cone up to this time. Due to the perturbation of the mgnetic'field we believe the most probably value of the energy curve is near the maximum value shown. Had the 909 put in it's expected energy (4 tims the value obtained) the - 8 final energy could have easily have gone beyond10 joules. DIsTRfBuTION CyU F. Ford 2A J. Foster 3 c9-y 4A R. Kidder 5A I% BY 6A C. McDonald 711 J. hck0u.s 8A J. Shearer 9A J. lfll.son sa
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