MadSci Network: Physics |
Your question is an interesting one, and -- as with most interesting questions -- the answer is that "it all depends..." For something to truly explode, most people believe (correctly) that it takes about 10,000 joules of laser energy to be applied to the surface per cubic centimeter of volume. By explosion, this means to me that the thing which absorbs the laser energy essentially instantly turns into a hot plasma (a gas of ions and electrons) and disassembles into an unrecognizable flash in something on the order of a millionth of a second. Let's now think a bit about the laser... To burn skin a little bit, you might start with a laser with pulsed energy output of 0.1 joules in a 0.635 cm (that's 1/4 inch, if you're thinking English units) beam. This laser will hurt a little bit when it hits your hand, but it won't leave a visible mark -- although it will blow the paint off the dial of your watch, which I know for a fact based on an experience I had with a very nice Omega Submariner which my wife gave me a few years ago. If you scale up the laser energy a bit to 2 joules in a 1 cm beam, the results are quite different: it causes flames (actually plasma) to blow off your skin and leaves a white mark of charred (but not penetrated) skin after a single pulse -- pretty ugly and hurts like the dickens, also based on personal experience. For a first estimate, let's just say that something like 3 joules in a laser pulse can cause some sort of burn. Now let's look at the tube you considered. I'll guess that the wall thickness of the tube is about 0.020" -- which would be considered thinwall if it were stainless steel tubing. 0.020" is equal to about 0.020 X 2.54 ~ .05 cm -- since I can only do sensible calculations in metric measurements, although I confess to thinking in English units sometimes. I'll also guess that the tube might be about 1/4 inch in diameter -- which is about 0.6 cm -- pretty big for a capsule that you'd swallow, so I'll back off my guess and say that maybe it's 0.5 cm in diameter. If the tube is 3/4" long -- that's about 1.8 cm or so -- the volume of the tubular section is equal to the cross sectional area of the tube multiplied by the length. The cross sectional area of such a thin tube is exactly given by the expression (Pi) X ( Router*Router - Rinner*Rinner); Pi = 3.14159 (a constant), Router and Rinner refer to the inner and outer radii of the tube. But I'm pretty lazy and, rather than do all this multiplication in a case where we don't need perfect accuracy, I use the fact that for a very thin-walled tube, the area is almost exactly equal to the circumference (Pi X Diameter X Wall Thickness), and for rough purposes this is just about 3 X 0.5 cm X 0.05 cm which we can do in our head to determine that the cross sectional area of the tube is about 0.075 square cm. [Just for fun, I did the exact calculation, using 0.5 cm as the outside diameter (which is twice the radius) of the tube and got the following: 3.14159 X(.50/2 X .50/2 -.45/2 X .45/2) = 0.0746 square cm, which is very close to the answer using the much easier way of estimating.] Multiplying this by the length of the tube to get the volume we find that this is 0.075 X 1.8 = 0.135 cubic centimeters -- and this is just for the cylindrical section. Assuming that the ends of the tube are flat and of diameter 0.5 cm, the area of each end is calculated as -- using rough calculations again, since we don't have to be exact -- just Pi X Radius X Radius ~ 3 X .25 X .25 ~ 0.4 square centimeters. Since the ends are 0.05 cm thick, the volume of each is 0.4 X 0.05 = 0.02 cubic centimeters. So the total volume of both ends is 0.04 cubic centimeters. Adding the volumes of the tube and the ends we get 0.175 cubic centimeters -- and since we're making rough estimates and I'm very lazy and prefer to deal with calculations I can do in my head, we'll estimate this as 0.2 cubic centimeters. If we take the 2 joules of laser energy we guessed above and put it into the capsule, the total energy deposition density is 2 Joules / 0.2 cubic centimeters or 10 joules per cubic centimeter... Comparing this with the 10,000 joules needed to turn something instantly into a flaming ball of plasma, it's pretty clear that we're a little shy in laser energy to create an explosion. But what if you REALLY meant that the laser would be powerful enough to cause these light burns over your entire body -- and we'll consider my body to be a thin pancake that's 2 m high and 0.5m wide (I'm not particularly thin, but I am about that high and wide). My surface area would then be 2 square meters and if I had 2 Joules per square centimeter distributed over my entire body, that would mean that our laser had 2 X 2 X 10,000 Joules of total output, or 40,000 joules total. If we stuff that through the small hole in the capsule, we'd be putting 40,000 joules onto a mass of .2 cubic centimeters -- so we'd have 200,000 joules of laser energy on a target that's just 0.2 cubic centimeters, resulting in an energy density of 1,000,000 joules per cubic centimeter. This is well above our explosion limit, so the capsule would be expected to burst instantly into a plasma fireball and disassemble. You may be concerned that I ignored the reflecting surface on the inside of the capsule. It turns out that any reflector, even a pretty good one, leaks a little light through -- maybe a tenth of a percent or so of the enregy that hits it. And any capsule or reflector material will absorb a little bit -- glass will absorb a tenth of a percent or so per centimeter of thickness, steel will absorb essentially all of it in a fraction of a centimeter. Also, slight imperfections in the coatings and/or materials always exist which absorb a little more than the nominal values. All of these factors, coupled with the hideously huge energy density of a MILLION JOULES PER CUBIC CENTIMETER would invariably cause a teeny localized area to be vaporized into a small plasma by part of the beam. The vaporized volume -- since it's a gas of ions and electrons -- would absorb the beam much more heavily and propagate damage to adjacent areas of the tube, which would then vaporize and absorb more, and so on until the tube disassembles very rapidly. The reflector on the inside of the tube will help to keep the pulsed beam from leaking out of the tube. This would probably allow the input pulse energy to be decreased somewhat -- it's hard to calculate exactly how much, but I'd guess that the energy needed to cause the explosion would be reduced by somewhere between a factor of 10 and 100, to something like 400- 4000 Joules. This is pretty close to my personal experience, in which I put a big piece of exposed polaroid film in front of the world's biggest laser (at the time) and hit it with about 300 Joules of output energy. The paper didn't explode, exactly, but the top layers of the paper (maybe half the thickness of the capsule you postulate) were blasted off the surface in a fireball jet that deposited light ash over most of the laser lab. In this case, the surface the beam hit was black (so that most of the beam was absorbed without reflection) but I hit it with so much lower beam energy that the situation is probably a reasonable, but rough, analog. Last, but not least, comes the issue of whether any of this is practical or important... From the standpoint of blowing up cylinders, it's pretty clear from the above that a lot of laser energy is needed -- of order thousands of Joule. Since lasers nowadays cost something like $100,000 for a 0.5 Joule lab laser, it's pretty apparent that things are likely to get pretty expensive pretty quickly. Just the laser would cost a ton of money, and that doesn't consider anything that you might have to add to point the laser at what you wanted to shoot it at or into -- it takes a pretty good optical system to repeated shoot into a tiny hole, and the optics can cost as much or more than the laser. You may also wonder why I keep talking about a pulsed laser. It turns out that if you tried to achieve the same function with a laser that was not pulsed, but put out continuous power over a longer period of time, things would change. If you used a low power laser and exposed the capsule for a long period of time (in this sense, any period greater than a few tens of microseconds probably qualifies as a long period of time) to deposit the energy slowly, a variety of things could happen. If the time was long enough, the tube might just heat up as the heat absorbed was carried away by radiation or convection. If the time was a little shorter, the tube might melt or burn. Or, if the time wasn't too short, it could still explode. What actually occurs depends on the laser power, the time, the hole size, the capsule size and material, and the reflectivity and surface quality of the inside of the capsule. In other words, it all depends...
Try the links in the MadSci Library for more information on Physics.