From: jameshartman@tsrcom.com Date: Aug 26 1996 AUDIO1.ASC -------------------------------------------------------------------- The following appeared in the prestigious Electric Spacecraft Journal - Issue #8, Published May 3, 1993. Page 40. ÚÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄ¿ ³ Information from ³ ³ Charles A. Yost ³ ³Dynamic Systems Inc³ ³ 73 Sunlight Drive ³ ³Leicester, NC 28748³ ÀÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÙ After James Hartman described making a loud- speaker levitate (ESJ#6, page 43), I decided to see if a loudspeaker could produce a net thrust. Apparently it can. I used a ten-inch diameter, eleven- pound Altec woofer suspended in pendular fashion by a pair of 38-inch long strings. (See Figure 1.) A constant 20 to 40 Hz high amplitude sine wave input didn't cause the slightest movement. However, quick pulsing of the sound in this frequency range was able to cause the woofer to swing in pendular fashion. The amplitude of the swing could be progressively ______________ 3 ^ | 8 | <-- | --> 1/2"| | /| air flow \ / | / | --- ÛÛ | ÄÄÄÄÄ> \ | 11 lb.\| Figure1. Speaker suspension increased if the sound pulses were timed to occur as the speaker was swinging through center. The maximum amplitude was about 1/2 inch. The voice coil chamber of the speaker was about three inches in diameter and two inches deep with a 3/4-inch central hole through which the air pulsed. A fine thread on a small stick allowed the airflow to be distinguished. (See Figure 2.) It is my thought that a very transient sound pulse sets up a brief unbalanced air flow and projects the equivalent of a smoke ring away from its face. Is there an equivalent electrostatic pulse phenomenon?* | | /| | / / Inward | / / Pulsed ÛÛßßN / air flow Ûß___. . . . . ÛÛ S . ---> .---> .---> ----> ÛÛ S . .. .. Outward Ûß___. pulsed ÛÛ N\ air flow ÛÛÜÜ \ \ \ \ \ \| internal construction Figure 2. Speaker Design