The Role Of 3 Objective Lenses on a Compound Light ... - where is the objective lens on a microscope
Actually a black leather glove she was wearing. Remember kids, don't get your hand in the beam -- that glove started smoking instantly. It seems when you are wearing #12 arc welding lenses, you can't see much short of the sun and whatever is in the lens' focus. (Like your hand on fire.) The side of someone's head. I don't even remember who's head it was. Or maybe I won't say to save that person embarrassment. But it was far enough from the focal point to do too much damage. Or at least that is the claim. A canadian penny. Like coupons, I think the redemption value of these is $.01 per 20, so why not destroy it? Actually we never managed to completely destroy it, as whatever we placed it on would perish long before the penny would. (Which brings me to the next entry . . .) We did completely oxidize the surface, however. A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
Fiber optic borescopes, popularly known as fiberscopes, are a traditional type of device still used in many industries in Canada. Usually a fiberscope ...
There are probably many more otherwise useful and productive things which have met an untimely demise through our devious misuse of science. The memories are hazy (probably because of the fumes from all the burning plastic) but as they come back I will add them here.
The Random Destructive Acts FAQ Updated March 19, 2003: It has been about 8 years since I wrote this page (before 2002 the last modification date was June 30, 1995) and I still get emails about it every few days. The most frequently asked question is, "Where can I buy one?" Edmund Scientific quit making this rectangular lens a few years ago and the company split, but Edmund Industrial Optics now makes a round 35 inch diameter lens (and many smaller sizes). Last I checked it was on this page but that's likely to change. It was part number NT43-921: FRESNEL LENS 35.0" DIA and cost $224.10. Jacob Dickinson informed me that Alltronics.com sells a rectangular lens similar in size to the infamous lens we had, and a few weeks ago I got one (see below). It's thinner than the Edmund's lens we used to have and needed a frame, but it's big and about half the price of Edmund's lens. You can find it at http://www.alltronics.com/lenses.htm and it was $99 plus shipping when I looked. If you're looking for something smaller and a lot cheaper, you can often find cheap surplus (used) 12" Fresnel lenses at American Science and Surplus and Scientifics (the new owner of the Edmund Scientific Catalog) for as little as $3. And to answer another only slightly less frequently asked question, no the beloved Dershem Memorial Lens is not for sale. We decided it would go to the first of us to get a Ph.D. (in other words, to first order we left it up to fate) and Chris Chaput was the proud winner. Thus Dr. Chris now owns the lens and (for obvious reasons) it is kept at least 1000 miles away from him at all times. People also ask, "What was the area of the focus?" The best we ever got was about a centimeter across. The lens was somewhat flexible so the corners didn't tend to contribute much. A professor at U of M who had one of these said he built a frame with cross supports and was able to get more of the lens to contribute to the focus. A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
A 3D Morphable Model learnt from 10,000 faces J. Booth, A. Roussos, S. Zafeiriou, A. Ponniah, D. Dunaway. Proceedings of IEEE Int’l Conf. on Computer Vision and Pattern Recognition (CVPR), June 2016
LSFMmeaning
Ande's hand. Actually a black leather glove she was wearing. Remember kids, don't get your hand in the beam -- that glove started smoking instantly. It seems when you are wearing #12 arc welding lenses, you can't see much short of the sun and whatever is in the lens' focus. (Like your hand on fire.) The side of someone's head. I don't even remember who's head it was. Or maybe I won't say to save that person embarrassment. But it was far enough from the focal point to do too much damage. Or at least that is the claim. A canadian penny. Like coupons, I think the redemption value of these is $.01 per 20, so why not destroy it? Actually we never managed to completely destroy it, as whatever we placed it on would perish long before the penny would. (Which brings me to the next entry . . .) We did completely oxidize the surface, however. A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
by NT Shaked · 2007 · Cited by 68 — The solution to this problem can be obtained using the proposed optical system by representing each unblocked edge by a numerical 1 (light) and each blocked ...
It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
These can be freestanding, propped against a wall or cheval style, which allows you to adjust to different angles. If you'd rather not take up floor space, an ...
LSFM2024
This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
This lens takes nearly a square meter of sunlight and concentrates it into about a square centimeter. We did not have the lens for too long before we were all seeing spots and heading to the nearest welding supply shop. "Are you doing arc welding or gas welding?" "Neither, actually we are destroying random inanimate objects with a giant Fresnel lens." Ande's hand. Actually a black leather glove she was wearing. Remember kids, don't get your hand in the beam -- that glove started smoking instantly. It seems when you are wearing #12 arc welding lenses, you can't see much short of the sun and whatever is in the lens' focus. (Like your hand on fire.) The side of someone's head. I don't even remember who's head it was. Or maybe I won't say to save that person embarrassment. But it was far enough from the focal point to do too much damage. Or at least that is the claim. A canadian penny. Like coupons, I think the redemption value of these is $.01 per 20, so why not destroy it? Actually we never managed to completely destroy it, as whatever we placed it on would perish long before the penny would. (Which brings me to the next entry . . .) We did completely oxidize the surface, however. A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
Light sheet microscopy
Light sheet fluorescence microscopy
Unfortunately since I am now in California and the beloved Dershem Memorial Lens is still in Michigan, as is most of the, er, evidence, I can not at this time provide any images.
Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
Updated 2003.03.19 slashdotted 2004.05.21 This is a copy of the original page at http://www-personal.umich.edu/~bclee/lens.html The University of Michigan will be deleting all www-personal web pages in 2012.
DET10A/M -Ask a technical question Ask a technical question. Package Weight: 0.34 lbs / Each ...
The side of someone's head. I don't even remember who's head it was. Or maybe I won't say to save that person embarrassment. But it was far enough from the focal point to do too much damage. Or at least that is the claim. A canadian penny. Like coupons, I think the redemption value of these is $.01 per 20, so why not destroy it? Actually we never managed to completely destroy it, as whatever we placed it on would perish long before the penny would. (Which brings me to the next entry . . .) We did completely oxidize the surface, however. A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
LSFM
It has been about 8 years since I wrote this page (before 2002 the last modification date was June 30, 1995) and I still get emails about it every few days. The most frequently asked question is, "Where can I buy one?" Edmund Scientific quit making this rectangular lens a few years ago and the company split, but Edmund Industrial Optics now makes a round 35 inch diameter lens (and many smaller sizes). Last I checked it was on this page but that's likely to change. It was part number NT43-921: FRESNEL LENS 35.0" DIA and cost $224.10. Jacob Dickinson informed me that Alltronics.com sells a rectangular lens similar in size to the infamous lens we had, and a few weeks ago I got one (see below). It's thinner than the Edmund's lens we used to have and needed a frame, but it's big and about half the price of Edmund's lens. You can find it at http://www.alltronics.com/lenses.htm and it was $99 plus shipping when I looked. If you're looking for something smaller and a lot cheaper, you can often find cheap surplus (used) 12" Fresnel lenses at American Science and Surplus and Scientifics (the new owner of the Edmund Scientific Catalog) for as little as $3. And to answer another only slightly less frequently asked question, no the beloved Dershem Memorial Lens is not for sale. We decided it would go to the first of us to get a Ph.D. (in other words, to first order we left it up to fate) and Chris Chaput was the proud winner. Thus Dr. Chris now owns the lens and (for obvious reasons) it is kept at least 1000 miles away from him at all times. People also ask, "What was the area of the focus?" The best we ever got was about a centimeter across. The lens was somewhat flexible so the corners didn't tend to contribute much. A professor at U of M who had one of these said he built a frame with cross supports and was able to get more of the lens to contribute to the focus. A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
ZEISS Lightsheet
Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
The best depth of field for portraits is a shallow depth of field when you want your subject to stand out from the background. Fast lenses with f-stops below f/ ...
People also ask, "What was the area of the focus?" The best we ever got was about a centimeter across. The lens was somewhat flexible so the corners didn't tend to contribute much. A professor at U of M who had one of these said he built a frame with cross supports and was able to get more of the lens to contribute to the focus. A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
Like coupons, I think the redemption value of these is $.01 per 20, so why not destroy it? Actually we never managed to completely destroy it, as whatever we placed it on would perish long before the penny would. (Which brings me to the next entry . . .) We did completely oxidize the surface, however. A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
light sheet microscopy中文
Fale Conosco! Whatsapp: (11) 4426-4445 · Telefone: (11) 4426-4445 · E-mail: sac@ultralightoptics.com · ULTRALIGHT OPTICS.
The LSFM models were produced by using this software pipeline on the (proprietary) MeIn3D dataset. For full terms and conditions, and to request access to the models, please visit the LSFM website. For technical details on the models we provide, see MODELS.md.
Line pairs per millimeter (lp/mm) is a measurement used to describe the spatial resolution of imaging systems, indicating how many pairs of contrasting ...
Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
Apr 17, 2020 — Depth of field" refers to the range of distances from the lens in which objects filmed will be in focus. Thus the correct option is D.
When I was a kid, I always wanted Edmund Scientific's Giant Fresnel Lens. "Melts asphalt in seconds!" the ad said. When I went to graduate school I met several other people with the same enthusiasm for aimless destruction through bizarre means, and just enough combined cash to make it happen. Thus the reign of terror began. Unfortunately since I am now in California and the beloved Dershem Memorial Lens is still in Michigan, as is most of the, er, evidence, I can not at this time provide any images.
The code used to produce the LSFM models is contained within this repository and is completely open source under a BSD license. You are free to follow the code's documentation, which explains how to install this tool and run it yourself on a set of facial meshes to automatically build a 3D Morphable Model.
A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
Page contents: Historic (1995) Giant Fresnel Lens Page FAQ (including where you can get your giant fresnel lens!) The New Lens Random Destructive Acts via Focused Solar Radiation When I was a kid, I always wanted Edmund Scientific's Giant Fresnel Lens. "Melts asphalt in seconds!" the ad said. When I went to graduate school I met several other people with the same enthusiasm for aimless destruction through bizarre means, and just enough combined cash to make it happen. Thus the reign of terror began. Unfortunately since I am now in California and the beloved Dershem Memorial Lens is still in Michigan, as is most of the, er, evidence, I can not at this time provide any images. Things we have destroyed with the giant Fresnel lens: Our retinas. This lens takes nearly a square meter of sunlight and concentrates it into about a square centimeter. We did not have the lens for too long before we were all seeing spots and heading to the nearest welding supply shop. "Are you doing arc welding or gas welding?" "Neither, actually we are destroying random inanimate objects with a giant Fresnel lens." Ande's hand. Actually a black leather glove she was wearing. Remember kids, don't get your hand in the beam -- that glove started smoking instantly. It seems when you are wearing #12 arc welding lenses, you can't see much short of the sun and whatever is in the lens' focus. (Like your hand on fire.) The side of someone's head. I don't even remember who's head it was. Or maybe I won't say to save that person embarrassment. But it was far enough from the focal point to do too much damage. Or at least that is the claim. A canadian penny. Like coupons, I think the redemption value of these is $.01 per 20, so why not destroy it? Actually we never managed to completely destroy it, as whatever we placed it on would perish long before the penny would. (Which brings me to the next entry . . .) We did completely oxidize the surface, however. A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame. As you can see, the purchase of such a dangerous item is mostly a self-destructive act. Be warned. There are probably many more otherwise useful and productive things which have met an untimely demise through our devious misuse of science. The memories are hazy (probably because of the fumes from all the burning plastic) but as they come back I will add them here. The Random Destructive Acts FAQ Updated March 19, 2003: It has been about 8 years since I wrote this page (before 2002 the last modification date was June 30, 1995) and I still get emails about it every few days. The most frequently asked question is, "Where can I buy one?" Edmund Scientific quit making this rectangular lens a few years ago and the company split, but Edmund Industrial Optics now makes a round 35 inch diameter lens (and many smaller sizes). Last I checked it was on this page but that's likely to change. It was part number NT43-921: FRESNEL LENS 35.0" DIA and cost $224.10. Jacob Dickinson informed me that Alltronics.com sells a rectangular lens similar in size to the infamous lens we had, and a few weeks ago I got one (see below). It's thinner than the Edmund's lens we used to have and needed a frame, but it's big and about half the price of Edmund's lens. You can find it at http://www.alltronics.com/lenses.htm and it was $99 plus shipping when I looked. If you're looking for something smaller and a lot cheaper, you can often find cheap surplus (used) 12" Fresnel lenses at American Science and Surplus and Scientifics (the new owner of the Edmund Scientific Catalog) for as little as $3. And to answer another only slightly less frequently asked question, no the beloved Dershem Memorial Lens is not for sale. We decided it would go to the first of us to get a Ph.D. (in other words, to first order we left it up to fate) and Chris Chaput was the proud winner. Thus Dr. Chris now owns the lens and (for obvious reasons) it is kept at least 1000 miles away from him at all times. People also ask, "What was the area of the focus?" The best we ever got was about a centimeter across. The lens was somewhat flexible so the corners didn't tend to contribute much. A professor at U of M who had one of these said he built a frame with cross supports and was able to get more of the lens to contribute to the focus. A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
If you're looking for something smaller and a lot cheaper, you can often find cheap surplus (used) 12" Fresnel lenses at American Science and Surplus and Scientifics (the new owner of the Edmund Scientific Catalog) for as little as $3. And to answer another only slightly less frequently asked question, no the beloved Dershem Memorial Lens is not for sale. We decided it would go to the first of us to get a Ph.D. (in other words, to first order we left it up to fate) and Chris Chaput was the proud winner. Thus Dr. Chris now owns the lens and (for obvious reasons) it is kept at least 1000 miles away from him at all times. People also ask, "What was the area of the focus?" The best we ever got was about a centimeter across. The lens was somewhat flexible so the corners didn't tend to contribute much. A professor at U of M who had one of these said he built a frame with cross supports and was able to get more of the lens to contribute to the focus. A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
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Jacob Dickinson informed me that Alltronics.com sells a rectangular lens similar in size to the infamous lens we had, and a few weeks ago I got one (see below). It's thinner than the Edmund's lens we used to have and needed a frame, but it's big and about half the price of Edmund's lens. You can find it at http://www.alltronics.com/lenses.htm and it was $99 plus shipping when I looked. If you're looking for something smaller and a lot cheaper, you can often find cheap surplus (used) 12" Fresnel lenses at American Science and Surplus and Scientifics (the new owner of the Edmund Scientific Catalog) for as little as $3. And to answer another only slightly less frequently asked question, no the beloved Dershem Memorial Lens is not for sale. We decided it would go to the first of us to get a Ph.D. (in other words, to first order we left it up to fate) and Chris Chaput was the proud winner. Thus Dr. Chris now owns the lens and (for obvious reasons) it is kept at least 1000 miles away from him at all times. People also ask, "What was the area of the focus?" The best we ever got was about a centimeter across. The lens was somewhat flexible so the corners didn't tend to contribute much. A professor at U of M who had one of these said he built a frame with cross supports and was able to get more of the lens to contribute to the focus. A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
Updated March 19, 2003: It has been about 8 years since I wrote this page (before 2002 the last modification date was June 30, 1995) and I still get emails about it every few days. The most frequently asked question is, "Where can I buy one?" Edmund Scientific quit making this rectangular lens a few years ago and the company split, but Edmund Industrial Optics now makes a round 35 inch diameter lens (and many smaller sizes). Last I checked it was on this page but that's likely to change. It was part number NT43-921: FRESNEL LENS 35.0" DIA and cost $224.10. Jacob Dickinson informed me that Alltronics.com sells a rectangular lens similar in size to the infamous lens we had, and a few weeks ago I got one (see below). It's thinner than the Edmund's lens we used to have and needed a frame, but it's big and about half the price of Edmund's lens. You can find it at http://www.alltronics.com/lenses.htm and it was $99 plus shipping when I looked. If you're looking for something smaller and a lot cheaper, you can often find cheap surplus (used) 12" Fresnel lenses at American Science and Surplus and Scientifics (the new owner of the Edmund Scientific Catalog) for as little as $3. And to answer another only slightly less frequently asked question, no the beloved Dershem Memorial Lens is not for sale. We decided it would go to the first of us to get a Ph.D. (in other words, to first order we left it up to fate) and Chris Chaput was the proud winner. Thus Dr. Chris now owns the lens and (for obvious reasons) it is kept at least 1000 miles away from him at all times. People also ask, "What was the area of the focus?" The best we ever got was about a centimeter across. The lens was somewhat flexible so the corners didn't tend to contribute much. A professor at U of M who had one of these said he built a frame with cross supports and was able to get more of the lens to contribute to the focus. A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
Random Destructive Acts via Focused Solar Radiation When I was a kid, I always wanted Edmund Scientific's Giant Fresnel Lens. "Melts asphalt in seconds!" the ad said. When I went to graduate school I met several other people with the same enthusiasm for aimless destruction through bizarre means, and just enough combined cash to make it happen. Thus the reign of terror began. Unfortunately since I am now in California and the beloved Dershem Memorial Lens is still in Michigan, as is most of the, er, evidence, I can not at this time provide any images. Things we have destroyed with the giant Fresnel lens: Our retinas. This lens takes nearly a square meter of sunlight and concentrates it into about a square centimeter. We did not have the lens for too long before we were all seeing spots and heading to the nearest welding supply shop. "Are you doing arc welding or gas welding?" "Neither, actually we are destroying random inanimate objects with a giant Fresnel lens." Ande's hand. Actually a black leather glove she was wearing. Remember kids, don't get your hand in the beam -- that glove started smoking instantly. It seems when you are wearing #12 arc welding lenses, you can't see much short of the sun and whatever is in the lens' focus. (Like your hand on fire.) The side of someone's head. I don't even remember who's head it was. Or maybe I won't say to save that person embarrassment. But it was far enough from the focal point to do too much damage. Or at least that is the claim. A canadian penny. Like coupons, I think the redemption value of these is $.01 per 20, so why not destroy it? Actually we never managed to completely destroy it, as whatever we placed it on would perish long before the penny would. (Which brings me to the next entry . . .) We did completely oxidize the surface, however. A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame. As you can see, the purchase of such a dangerous item is mostly a self-destructive act. Be warned. There are probably many more otherwise useful and productive things which have met an untimely demise through our devious misuse of science. The memories are hazy (probably because of the fumes from all the burning plastic) but as they come back I will add them here. The Random Destructive Acts FAQ Updated March 19, 2003: It has been about 8 years since I wrote this page (before 2002 the last modification date was June 30, 1995) and I still get emails about it every few days. The most frequently asked question is, "Where can I buy one?" Edmund Scientific quit making this rectangular lens a few years ago and the company split, but Edmund Industrial Optics now makes a round 35 inch diameter lens (and many smaller sizes). Last I checked it was on this page but that's likely to change. It was part number NT43-921: FRESNEL LENS 35.0" DIA and cost $224.10. Jacob Dickinson informed me that Alltronics.com sells a rectangular lens similar in size to the infamous lens we had, and a few weeks ago I got one (see below). It's thinner than the Edmund's lens we used to have and needed a frame, but it's big and about half the price of Edmund's lens. You can find it at http://www.alltronics.com/lenses.htm and it was $99 plus shipping when I looked. If you're looking for something smaller and a lot cheaper, you can often find cheap surplus (used) 12" Fresnel lenses at American Science and Surplus and Scientifics (the new owner of the Edmund Scientific Catalog) for as little as $3. And to answer another only slightly less frequently asked question, no the beloved Dershem Memorial Lens is not for sale. We decided it would go to the first of us to get a Ph.D. (in other words, to first order we left it up to fate) and Chris Chaput was the proud winner. Thus Dr. Chris now owns the lens and (for obvious reasons) it is kept at least 1000 miles away from him at all times. People also ask, "What was the area of the focus?" The best we ever got was about a centimeter across. The lens was somewhat flexible so the corners didn't tend to contribute much. A professor at U of M who had one of these said he built a frame with cross supports and was able to get more of the lens to contribute to the focus. A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
Random Destructive Acts via Focused Solar Radiation When I was a kid, I always wanted Edmund Scientific's Giant Fresnel Lens. "Melts asphalt in seconds!" the ad said. When I went to graduate school I met several other people with the same enthusiasm for aimless destruction through bizarre means, and just enough combined cash to make it happen. Thus the reign of terror began. Unfortunately since I am now in California and the beloved Dershem Memorial Lens is still in Michigan, as is most of the, er, evidence, I can not at this time provide any images. Things we have destroyed with the giant Fresnel lens: Our retinas. This lens takes nearly a square meter of sunlight and concentrates it into about a square centimeter. We did not have the lens for too long before we were all seeing spots and heading to the nearest welding supply shop. "Are you doing arc welding or gas welding?" "Neither, actually we are destroying random inanimate objects with a giant Fresnel lens." Ande's hand. Actually a black leather glove she was wearing. Remember kids, don't get your hand in the beam -- that glove started smoking instantly. It seems when you are wearing #12 arc welding lenses, you can't see much short of the sun and whatever is in the lens' focus. (Like your hand on fire.) The side of someone's head. I don't even remember who's head it was. Or maybe I won't say to save that person embarrassment. But it was far enough from the focal point to do too much damage. Or at least that is the claim. A canadian penny. Like coupons, I think the redemption value of these is $.01 per 20, so why not destroy it? Actually we never managed to completely destroy it, as whatever we placed it on would perish long before the penny would. (Which brings me to the next entry . . .) We did completely oxidize the surface, however. A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame. As you can see, the purchase of such a dangerous item is mostly a self-destructive act. Be warned. There are probably many more otherwise useful and productive things which have met an untimely demise through our devious misuse of science. The memories are hazy (probably because of the fumes from all the burning plastic) but as they come back I will add them here. The Random Destructive Acts FAQ Updated March 19, 2003: It has been about 8 years since I wrote this page (before 2002 the last modification date was June 30, 1995) and I still get emails about it every few days. The most frequently asked question is, "Where can I buy one?" Edmund Scientific quit making this rectangular lens a few years ago and the company split, but Edmund Industrial Optics now makes a round 35 inch diameter lens (and many smaller sizes). Last I checked it was on this page but that's likely to change. It was part number NT43-921: FRESNEL LENS 35.0" DIA and cost $224.10. Jacob Dickinson informed me that Alltronics.com sells a rectangular lens similar in size to the infamous lens we had, and a few weeks ago I got one (see below). It's thinner than the Edmund's lens we used to have and needed a frame, but it's big and about half the price of Edmund's lens. You can find it at http://www.alltronics.com/lenses.htm and it was $99 plus shipping when I looked. If you're looking for something smaller and a lot cheaper, you can often find cheap surplus (used) 12" Fresnel lenses at American Science and Surplus and Scientifics (the new owner of the Edmund Scientific Catalog) for as little as $3. And to answer another only slightly less frequently asked question, no the beloved Dershem Memorial Lens is not for sale. We decided it would go to the first of us to get a Ph.D. (in other words, to first order we left it up to fate) and Chris Chaput was the proud winner. Thus Dr. Chris now owns the lens and (for obvious reasons) it is kept at least 1000 miles away from him at all times. People also ask, "What was the area of the focus?" The best we ever got was about a centimeter across. The lens was somewhat flexible so the corners didn't tend to contribute much. A professor at U of M who had one of these said he built a frame with cross supports and was able to get more of the lens to contribute to the focus. A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
And to answer another only slightly less frequently asked question, no the beloved Dershem Memorial Lens is not for sale. We decided it would go to the first of us to get a Ph.D. (in other words, to first order we left it up to fate) and Chris Chaput was the proud winner. Thus Dr. Chris now owns the lens and (for obvious reasons) it is kept at least 1000 miles away from him at all times. People also ask, "What was the area of the focus?" The best we ever got was about a centimeter across. The lens was somewhat flexible so the corners didn't tend to contribute much. A professor at U of M who had one of these said he built a frame with cross supports and was able to get more of the lens to contribute to the focus. A lot of people want to know what temperatures we achieved. It's hard to make this estimate, the real question should be how much power the lens can supply (and you can see more about this below). But in terms of estimates, we certainly melted aluminum which has a melting point of 660.37 degC. We never quite managed to melt copper with the old lens but (melting point of 1083.4 degC) but we have with the new one (see below) so I think we could have if the sidewalk had not been so fragile. Assuming a black body target and that the sun supplies 1340 W/m^2 (before atmospheric absorption) we calculated that we should be able to melt quartz (1610 degC) but in practice I don't believe we achieved temperatures that high. The New Lens Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu
OPTICS DEFINITIONS (LENSES AND MIRRORS) focal point-the point on the axis of a lens or mirror to which parallel rays of light converge or from which they ...
Dec 13, 2018 — It is well known that light filed can be decomposed into polarized field and unpolarized field. But, is it possible to consider this sum as ...
A canadian penny. Like coupons, I think the redemption value of these is $.01 per 20, so why not destroy it? Actually we never managed to completely destroy it, as whatever we placed it on would perish long before the penny would. (Which brings me to the next entry . . .) We did completely oxidize the surface, however. A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
I don't even remember who's head it was. Or maybe I won't say to save that person embarrassment. But it was far enough from the focal point to do too much damage. Or at least that is the claim. A canadian penny. Like coupons, I think the redemption value of these is $.01 per 20, so why not destroy it? Actually we never managed to completely destroy it, as whatever we placed it on would perish long before the penny would. (Which brings me to the next entry . . .) We did completely oxidize the surface, however. A sidewalk. It seems that normal concrete will start emitting plumes of smoke just before it pops, leaving a crater about the size of a quarter, and ejecting the aforementioned canadian penny in some random direction. Kids, always wear safety goggles when playing with giant Fresnel lenses. Lots of chalk. Chalk actually burns under this thing. Aluminum cans. So do aluminum cans. They smell really bad. The floor. It is never a good idea to use the lens indoors. Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
Large scale 3D Morphable Models J. Booth, A. Roussos, A. Ponniah, D. Dunaway, S. Zafeiriou. International Journal of Computer Vision (IJCV), April 2017
Mike's car. Well, not yet. But it's plastic, so it would go up in no time at all. Or maybe we could just shrink-wrap the body around the frame.
Here are a few pictures of our new lens (from Alltronics.com) and our first test target. The target was (certainly past tense) a zinc penny. The copper turned into a black crust and the zinc ran out the side (that silver blob going up in these pictures). The target stage was some shale like rock we had sitting around, which would flake when heated but didn't pop and eject the target. We have since taken many targets and caused them to melt/incinerate/explode (it's a pain to clean pop off the lens) and soon I will add a few more pictures. Impressive as destroying a penny may seem, I estimated that we may have only managed to get maybe 10 percent of the available energy hitting the lens (roughly 1kW) into the penny: Mass of a zinc penny: 0.0025 kg Specific heat of zinc: 390 J/kgK Melting point of zinc: 419.58 degC Thus 20degC to about 420degC takes 390 J Latent heat of fusion for zinc: 1.1x10e5 J/kg Thus to melt the penny takes about 275 J We heated the liquid zinc considerably as well, but I will ignore that. Total energy in the penny: > 665 J It takes something under or around 6 seconds to melt a penny: 665 J / 6 sec gives us a lower limit of about >= 111 Watts Sunlight at the earth: 1365 W/m^2 Transmission of the earth's atmosphere: maybe 65-70% at this angle with some clouds? Area of the lens is about 1.1m^2 Power on the lens: approx. 1000 W Power to the penny >= 10.0% This is likely at least a slight underestimate of the lens' output for at least a couple reasons: it was slightly cloudy and the sun was not all that high (effective transmission may have been much lower); likely a lot of the energy went into the stage instead of the target (the metal stage we used later was pretty badly warped when we were done). We hope to improve on this by making stands and will try to measure it more carefully. This is optically a better lens than the old Edmunds one (better image) and as Edmunds points out, optically better Fresnel lenses tend to be less efficient light concentrators, so maybe that's part of our problem too -- there was a nice central focus (smaller than the penny) but a lot of the light was scattered into a much larger area, at least a foot across. This may make the lens more useful for diffuse heat applications (cooking) than concentrated ones. We'll see . . . returN Return Why are you here? / What does it all mean? / bclee@umich.edu