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#131
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KLM wrote:
On Thu, 18 Mar 2004 05:39:21 +0000, Tim Auton tim.auton@uton.[groupSexWithoutTheY] wrote: Do you all think that tangos are dumb enough to trigger the bomb with the ringer or would the detonator answer first and listen for a DTMF sequence. Hmmm? Achmed the bomb maker gets a wrong number just as he's connecting the thing. I very much doubt they bother with DTMF decoders. I mean, how often do you get a wrong number? I've had about 4 in my life. They'll just connect the ringer (or vibrate function) to the detonator (with whatever minimal circuitry in between is required - I've never used a detonator!) and then only turn the phone on at the last minute. It's not dumb to design a remote detonation system that requires the absolute minimum of specialist knowledge and equipment to construct. To use the unique cellphone ID to detonate a remote bomb is actually a very ingenious innovation. No timers to mess with. The terrorist has full and instant control of the time and place to set off the bomb. As Tim says its relatively easy to connect the ringer wires to a simple circuit to output enough juice to trigger the detonator. Frist year student project - like using a battery to keep a capacitor charged and the ringer closes the discharge switch. Boom. I'm pretty sure that it won't work that simple. There are other factors at play that make controlling things with a telephone a lot harder to achieve than you think... For everyone's safety I'm not going into the details. -- Reply to nico@nctdevpuntnl (punt=.) Bedrijven en winkels vindt U op www.adresboekje.nl |
#132
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If you think it is that hard, it's obvious the reason you won't go into the
details. You don't know. It is rather easily done. "Nico Coesel" wrote in message ... I'm pretty sure that it won't work that simple. There are other factors at play that make controlling things with a telephone a lot harder to achieve than you think... For everyone's safety I'm not going into the details. |
#134
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John Woodgate wrote in message ...
I read in sci.electronics.design that Bill Sloman wrote (in ) about 'CB Radios, Cellphones and Gasoline Vapor Ignition', on Sun, 21 Mar 2004: For the difference between Dewar benzene and Kekule benzene see http://www.chemsoc.org/exemplarchem/...enzenering.htm Dewar benzene can actually be made? Do you know when it was discovered? What about the prismatic form? I would have thought that was a lot easier to make, if I didn't have a suspicion that that is where simple bonding ideas break down. IIRR all three Dewar benzenes can be made - with difficulty. They've been available since before 1971 at least - which is when my project fell apart - but they were newish then. The three-carbon rings at either end of the prismatic version do have a lot of steric strain, but they can be made - I think pyrethroid insecticides include just such a cyclopropane ring. ---------- Bill Sloman, Nijmegen |
#135
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(John Michael Williams) wrote in message om...
(Bill Sloman) wrote in message . com... ... The controlling relationship is between the volume of the sphere in which the reaction is first initiated, and the surface area of that sphere - if the intial volume is too small, not enough energy is released to heat the surrounding shell of gas to the ignition temperature. ... ------- Bill Sloman, Nijmegen This makes sense. I think I can see a spark 0.1 mm in radius, at say 4000 K. That's about 4 cubic picometers in volume and about 0.1 square micron in surface area (assuming sparks have smooth surfaces). But, I'm not sure how to relate that to the threshold of flame propagation. If energy is a factor, rather than power, the duration of the spark would seem to be relevant, too. Sparks are much faster than flame fronts - when I was involved in instrinsic safety nobody paid any attention to spark duration, and for all practical purposes the energy stored in the capacitance of a spark gap is dumped into the gas much faster than it can be dissipated. ------ Bill Sloman, Nijmegen |
#136
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![]() CW says... "Nico Coesel" wrote... I'm pretty sure that it won't work that simple. There are other factors at play that make controlling things with a telephone a lot harder to achieve than you think... For everyone's safety I'm not going into the details. If you think it is that hard, it's obvious the reason you won't go into the details. You don't know. It is rather easily done. Any electronics engineer or technician can do it. (CW, please don't top post) -- Guy Macon, Electronics Engineer & Project Manager for hire. Remember Doc Brown from the _Back to the Future_ movies? Do you have an "impossible" engineering project that only someone like Doc Brown can solve? My resume is at http://www.guymacon.com/ |
#137
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In , Jeff Liebermann wrote
in part: Neon lamp needs about 60 volts to light and 40 volts to stay lit. The 4 watt flourescent tube wants at least 90 volts to start, and I think (i.e. guess) about 50 volts to stay lit. Lower voltage neon lamps do indeed light at 60 volts RMS and stay lit at 40 volts RMS. But these are lowish figures. 4-watt fluorescents need more, except they stay lit at only about 30 volts at full current, and part of that reason is thermionic emission from hot electrodes. I would not worry about RF from a cellphone igniting anything. If a cellphone is going to be found to ignite gasoline vapor, I think more likely ways a * Sparks in the vibration motor * Sparks from failing wires/connections * Sparks in speakers with voice coils with intermittent shorts * Sparks in switches (in whatever few models having switches that actually switch enough current to make a spark) I have already seen the Snopes item months ago when I first heard of cellphones supposedly causing gas station fires, and they make it sound as if cellphone ignition of gasoline vapors may never have actually occurred, evidence that this has indeed happened appears mainly anecdotal, and that this is rare if it does happen. When I refuel my car, I keep my cellphone either far or upwind from the gas inlet of my car. (My cellphone has vibration on.) I also ground myself by touching something far/upwind of the fuel inlet if I let go of the nozzle and have to touch the nozzle or anything near the fuel inlet again before leaving the gas station to avoid the greater danger of static electricity. - Don Klipstein ) |
#138
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In , Bill Sloman wrote
in part: I had to work through the equations many years ago for an experiment intended to monitor the process in which one of the "Dewar benzenes" converted itself to normal - Kekule's - benzene, which is an enormously energetic process, involving about an order of magnitude more energy per molecule than you get out of TNT and PETN. I really didn't want to blast my experimental apparatus to smithereens. When I went through the calculations with my supervisor, he pulled a very long face - the motivation for the experiment had been some unexpected flashes of light seen when a dumb organic chemist had released small drops of liquid "Dewar benzene" into a hot cell, and my calculations made it clear that the flashes of light were just thermal radiation from a hot plasma, rather than fluorsecence from from an electronically excited state of Kekule benezene, which is what my supervisor had been hoping for ... For the difference between Dewar benzene and Kekule benzene see http://www.chemsoc.org/exemplarchem/...enzenering.htm If this produces anything near 10x the energy per weight of TNT or PETN, then a version with controlled reaction rate would make one heck of a rocket propellant. I thought the ultimate energy per mass was magnesium and oxygen (or was it beryllium and oxygen?), just a few times as much energy per mass as TNT and not good like usual rocket propellants for producing gas to use as rocket exhaust. I am surely skeptical of changing one isomer of a molecule to another producing even comparable energy to, let alone more energy than decomposition of a similar or somewhat greater mass molecule of high explosive. - Don Klipstein ) |
#139
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In , Jeff Liebermann wrote:
On Sun, 21 Mar 2004 08:47:34 +0000, John Woodgate wrote: I read in sci.electronics.design that Jeff Liebermann wrote (in mppp50ho4dr08ahkb3dlbqkcfkp0ih ) about 'CB Radios, Cellphones and Gasoline Vapor Ignition', on Sun, 21 Mar 2004: The gap necessary to create an arc with 22 volts is: 22V / 20,000V/in = 0.001 inches Kinda small, but given a microscope, a 1 mil spark gap will arc. But it takes about 350 V to do so. The relationship between voltage and gap length is very non-linear below about 500 V. I didn't know that it wasn't linear. I just assumed that it takes the same amount of energy to peel electrons off of a single atom (ionize) regardless of gap seperation. It gets messy. You can see how messy it gets when you see what happens in the cathode area of a "glow discharge". A "glow discharge" is one of two common processes where positive ions of the gas/vapor are accelerated by the cathode-adjacent electric field into the cathode material, and where positive ions bombarding the cathode dislodge electrons from the cathode to maintain the supply of free electrons in the "discharge" (conductive path of glowing gas/vapor). (The other of the two common discharge mechanisms where cathode bombardment by positive ions dislodges electrons is the "cold cathode arc". There is still another cathode process for a discharge known as the "thermionic arc".) The glow discharge cathode process has 5 layers, 3 dim/dark and 2 bright. There is some sort of 'natural spacing' and 'natural thickness' of these layers, which varies with gas/vapor type and pressure and the cathode material. There is also a characteristic voltage drop of the cathode process known as the "cathode fall", and that is normally a few times or several times the ionization potential of the gas/vapor. There is such a thing as "normal glow", where the cathode process occurs at its natural current density (for the gas/vapor type and pressure and cathode material), and the first two dark layers and the two bright layers and some minimal portion of the third dark layer have a tendency to occupy some 'natural distance' (a function of gas/vapor type and pressure and cathode material) between cathode and anode. Then there is "abnormal glow", where the cathode process is forced into a smaller space between electrodes and/or is conducting a current density higher than 'natural' (for the gas/vapor type/pressure and cathode material) due to more current flowing than is "natural" for the available cross section of cathode process. When that happens, the "cathode fall" is even higher than that of "nowmal glow". There's also the minor detail of RF excitation versus DC. As I vaguely remember from my 35 years ago college welding classes, TIG welding uses RF to strike the arc because it takes less power/energy/whatever to start the arc. I don't know about that, but I have heard of RF glow discharges maybe having the cathode process eliminating one bright layer and one dark layer (for "electrodeless discharge" that occurs where insulation exists over the cathode for example), and that may reduce the cathode fall. We're allegedly talking about striking an arc across 0.001" with a 5 watt, 27MHz transmitter terminated with a 50 ohm load. If it's non-linear in the opposite direction, the calcs are gonna be no fun. ![]() I have everything it takes to test this. Microscope slide, with two sewing pins glued with hotmelt goo and seperated by 0.001". Apply RF and watch through the microscope. I'll see if I can throw something together and post photos (time permitting). Please do!!! - Don Klipstein ) |
#140
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"S" wrote in message et...
the show on discovery channel, mythbusters. debunked that myth, They also showed in the same episode that a good percentage of fueling fires come from static sparks around the gas tank. Someone mentioned it before, but ground yourself away from the tank before you start fueling. Apparently women are more likely not to ground themselves and have something 70% of all spark induced fires. It was pretty cool to watch the show and see a firefighter deliberately generate a static spark and light himself on fire at a gas pump. |
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