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Storing gas at high temperature for rocket propellant.
This page gives the equation for the velocity of the exhaust gas of a
rocket: Rocket engine nozzle. http://en.wikipedia.org/wiki/Rocket_...engine_nozzles Since the Isp (specific impulse) of a propellant in units of seconds is found by just dividing this by 9.8 m/s^2, the Isp is maximized by making the exhaust speed as high as possible. In the formula this can be achieved by making the exhaust be high temperature. Usually in rockets this is done by using a high energy chemical reaction, such as by burning H2 with O2. However, in the formula you see the exhaust speed is also dependent in an inverse fashion on the molecular mass of the exhaust products. For burning H2, you get H2O with a molecular mass of 18. Can we get the exhaust gas simply by just H2 with a molecular mass of 2? One way this could be done would be simply by storing the hydrogen at high temperature. Since rocket launches last only about 8 minutes the tanks would only have to be insulated to maintain the temperature inside for that length of time. If we stored the hydrogen at 3000 K, the exhaust velocity in vacuum would be 9344 m/s, significantly better than the 4550 m/s maximum exhaust speed of H2/LOX engines. The problem would be storing the H2 at the high temperature and the accompanying high pressure. Carbon-carbon composites are known to return their high strength at high temperature. This book reference gives the tensile strength as 700 MPa and states it actually *increases* as temperature increases to the highest measured temperature given, 2000 K: http://books.google.com/books?id=d52...m=22&ct=result However, the melting point of carbon (actually it sublimates at 1 bar pressure) is about 4000 K. Since the tensile strength is actually increasing at 2000 K quite likely it continues to increase beyond this and likely will remain high at least up to 3000 K. Carbon-carbon for example is used for rocket nozzles for temperatures exceeding 3000 K: Nondestructive Characterisation of Carbon/Carbon Brake Disks Using Ultrasonics. "C/C composite is consisted of a fiber based on carbon precursors embedded in a carbon matrix and has such properties as low density, high thermal conductivity and shock resistance, low thermal expansion and high modulus. The C/C composite is applied for structures in high temperature condition, such as a brake disk of aircraft, a nozzle of rocket engine and etc., because C/C composite not only withstands high temperature approaching 3000oC, but actually increases in strength." http://www.ndt.net/apcndt2001/papers/1109/1109.htm TW/SNTP - TECHNICAL CONCEPTS AND DEVELOPMENT ACTIVITIES. "The high exhaust temperature requires either a transpiration or regeneratively cooled nozzle, or a radiation-cooled carbon-carbon nozzle. The carbon-carbon nozzle was used as the baseline, given its low mass and simple design. Carbon-carbon nozzles have been tested in solid-rocket motors at temperatures up to 4000 K. But development of coatings (TaC, ZrC and NbC are candidates) will be required to avoid hydrogen erosion." http://www.fas.org/nuke/space/c08tw_3.htm Carbon-carbon composites though are porous so it is uncertain if they can be used for hydrogen storage at high temperature. An advantage of the carbon-carbon though is that it could be used as a single high strength, high temperature tank rather than numerous microspheres or microtubes. However, microspheres or microtubes might allow higher temperatures and/or pressures. For example synthetic diamond of micron-scale size can be made cheaply and may have higher tensile strength than natural diamond: Brief Communications Nature 421, 599-600 (6 February 2003) Materials: Ultrahard polycrystalline diamond from graphite. "Polycrystalline diamonds are harder and tougher than single-crystal diamonds and are therefore valuable for cutting and polishing other hard materials, but naturally occurring polycrystalline diamond is unusual and its production is slow. Here we describe the rapid synthesis of pure sintered polycrystalline diamond by direct conversion of graphite under static high pressure and temperature. Surprisingly, this synthesized diamond is ultrahard and so could be useful in the manufacture of scientific and industrial tools." http://www.nature.com/nature/journal...l/421599b.html Since these synthetic diamonds are harder than natural diamond, they very likely also are of higher tensile strength. This page says though there has been varying measured amounts for natural diamonds tensile strength one experiment, and some theoretical work, suggests it could be as high as 60 GPa: Material properties of diamond. http://en.wikipedia.org/wiki/Materia...ies_of_diamond And this page says at pressures of 60 GPa, 600 kilobars, diamond can remain solid up to 6,000 K: Modeling the Phase Diagram of Carbon. PRL 94, 145701 (2005) PHYSICAL REVIEW LETTERS 15 APRIL 2005 http://www.amolf.nl/publications/pdf/4312.pdf At a temperature of 6,000 K, the H2 would have an exhaust velocity of 13,200 m/s. However, there would be the problem of keeping the diamond at the high pressure required to remain solid. You could supply the high pressure on the inside of the diamond microspheres by the H2 gas but how to apply the high pressure to the outside? You would also have the problem of releasing the hydrogen when needed. One possibility might be to expose the diamond to oxygen. Carbon will burn in oxygen at temperatures of 600 C and above. The carbon tanks holding the H2 at high temperature will have to be kept in inert gas or in vacuum to prevent contact with oxygen until the H2 is to be released. Another possibility for the high temperature material for the microspheres or microtubes to hold the H2 might be high temperature, refractory, materials. One is tantalum hafnium carbide, which has a melting point of about 4,500 K. These would also need to be made to have high tensile strength. It is common that when materials are made into 'whiskers' at the microscale they achieve GPa tensile strengths. One method to make the whiskers is the vapor-liquid-solid method: Growing Crystals with the VLS Process (Vapor - Liquid - Solid) http://www.hbci.com/~wenonah/new/crystals.htm It is necessary to hold the hydrogen at high pressure since it will be a high temperature gas. For instance at room temperature, say 300 K, and at 1 bar, H2 has a density about 1/10th kg/m^3. So at 3,000 K the pressure would be 10 bar. However, at a density of only .1 kg/m^3, the volume would be prohibitive for tens of thousands to hundreds of thousands of kilos of H2. So to get a reasonable volume for the H2 we will need much higher pressure. By multiplying the density by a factor of 1,000 to 100 kg/m^3, somewhat better than that of liquid hydrogen, the pressure would also be multiplied by 1,000 to 10,000 bar, 1 GPa, with the temperature kept at 3,000 K. Bob Clark |
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Storing gas at high temperature for rocket propellant.
Dear Robert Clark:
On Aug 29, 12:13*pm, Robert Clark wrote: .... *It is necessary to hold the hydrogen at high pressure since it will be a high temperature gas. And when you release the pressure, you lose the temperature, and hence the thrust. "Half" of what you store is lost this way. Chemical, fusion, or fission are *the* ways to store energy for later release. David A. Smith |
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Storing gas at high temperature for rocket propellant.
"Robert Clark" wrote in message ... This page gives the equation for the velocity of the exhaust gas of a rocket: Rocket engine nozzle. http://en.wikipedia.org/wiki/Rocket_...engine_nozzles Since the Isp (specific impulse) of a propellant in units of seconds is found by just dividing this by 9.8 m/s^2, the Isp is maximized by making the exhaust speed as high as possible. In the formula this can be achieved by making the exhaust be high temperature. Usually in rockets this is done by using a high energy chemical reaction, such as by burning H2 with O2. However, in the formula you see the exhaust speed is also dependent in an inverse fashion on the molecular mass of the exhaust products. For burning H2, you get H2O with a molecular mass of 18. Can we get the exhaust gas simply by just H2 with a molecular mass of 2? One way this could be done would be simply by storing the hydrogen at high temperature. Since rocket launches last only about 8 minutes the tanks would only have to be insulated to maintain the temperature inside for that length of time. If we stored the hydrogen at 3000 K, the exhaust velocity in vacuum would be 9344 m/s, significantly better than the 4550 m/s maximum exhaust speed of H2/LOX engines. The problem would be storing the H2 at the high temperature and the accompanying high pressure. Carbon-carbon composites are known to return their high strength at high temperature. This book reference gives the tensile strength as 700 MPa and states it actually *increases* as temperature increases to the highest measured temperature given, 2000 K: http://books.google.com/books?id=d52...m=22&ct=result However, the melting point of carbon (actually it sublimates at 1 bar pressure) is about 4000 K. Since the tensile strength is actually increasing at 2000 K quite likely it continues to increase beyond this and likely will remain high at least up to 3000 K. Carbon-carbon for example is used for rocket nozzles for temperatures exceeding 3000 K: Nondestructive Characterisation of Carbon/Carbon Brake Disks Using Ultrasonics. "C/C composite is consisted of a fiber based on carbon precursors embedded in a carbon matrix and has such properties as low density, high thermal conductivity and shock resistance, low thermal expansion and high modulus. The C/C composite is applied for structures in high temperature condition, such as a brake disk of aircraft, a nozzle of rocket engine and etc., because C/C composite not only withstands high temperature approaching 3000oC, but actually increases in strength." http://www.ndt.net/apcndt2001/papers/1109/1109.htm TW/SNTP - TECHNICAL CONCEPTS AND DEVELOPMENT ACTIVITIES. "The high exhaust temperature requires either a transpiration or regeneratively cooled nozzle, or a radiation-cooled carbon-carbon nozzle. The carbon-carbon nozzle was used as the baseline, given its low mass and simple design. Carbon-carbon nozzles have been tested in solid-rocket motors at temperatures up to 4000 K. But development of coatings (TaC, ZrC and NbC are candidates) will be required to avoid hydrogen erosion." http://www.fas.org/nuke/space/c08tw_3.htm Carbon-carbon composites though are porous so it is uncertain if they can be used for hydrogen storage at high temperature. An advantage of the carbon-carbon though is that it could be used as a single high strength, high temperature tank rather than numerous microspheres or microtubes. However, microspheres or microtubes might allow higher temperatures and/or pressures. For example synthetic diamond of micron-scale size can be made cheaply and may have higher tensile strength than natural diamond: Brief Communications Nature 421, 599-600 (6 February 2003) Materials: Ultrahard polycrystalline diamond from graphite. "Polycrystalline diamonds are harder and tougher than single-crystal diamonds and are therefore valuable for cutting and polishing other hard materials, but naturally occurring polycrystalline diamond is unusual and its production is slow. Here we describe the rapid synthesis of pure sintered polycrystalline diamond by direct conversion of graphite under static high pressure and temperature. Surprisingly, this synthesized diamond is ultrahard and so could be useful in the manufacture of scientific and industrial tools." http://www.nature.com/nature/journal...l/421599b.html Since these synthetic diamonds are harder than natural diamond, they very likely also are of higher tensile strength. This page says though there has been varying measured amounts for natural diamonds tensile strength one experiment, and some theoretical work, suggests it could be as high as 60 GPa: Material properties of diamond. http://en.wikipedia.org/wiki/Materia...ies_of_diamond And this page says at pressures of 60 GPa, 600 kilobars, diamond can remain solid up to 6,000 K: Modeling the Phase Diagram of Carbon. PRL 94, 145701 (2005) PHYSICAL REVIEW LETTERS 15 APRIL 2005 http://www.amolf.nl/publications/pdf/4312.pdf At a temperature of 6,000 K, the H2 would have an exhaust velocity of 13,200 m/s. However, there would be the problem of keeping the diamond at the high pressure required to remain solid. You could supply the high pressure on the inside of the diamond microspheres by the H2 gas but how to apply the high pressure to the outside? You would also have the problem of releasing the hydrogen when needed. One possibility might be to expose the diamond to oxygen. Carbon will burn in oxygen at temperatures of 600 C and above. The carbon tanks holding the H2 at high temperature will have to be kept in inert gas or in vacuum to prevent contact with oxygen until the H2 is to be released. Another possibility for the high temperature material for the microspheres or microtubes to hold the H2 might be high temperature, refractory, materials. One is tantalum hafnium carbide, which has a melting point of about 4,500 K. These would also need to be made to have high tensile strength. It is common that when materials are made into 'whiskers' at the microscale they achieve GPa tensile strengths. One method to make the whiskers is the vapor-liquid-solid method: Growing Crystals with the VLS Process (Vapor - Liquid - Solid) http://www.hbci.com/~wenonah/new/crystals.htm It is necessary to hold the hydrogen at high pressure since it will be a high temperature gas. For instance at room temperature, say 300 K, and at 1 bar, H2 has a density about 1/10th kg/m^3. So at 3,000 K the pressure would be 10 bar. However, at a density of only .1 kg/m^3, the volume would be prohibitive for tens of thousands to hundreds of thousands of kilos of H2. So to get a reasonable volume for the H2 we will need much higher pressure. By multiplying the density by a factor of 1,000 to 100 kg/m^3, somewhat better than that of liquid hydrogen, the pressure would also be multiplied by 1,000 to 10,000 bar, 1 GPa, with the temperature kept at 3,000 K. Bob Clark Oh dear... this sounds like rocket science. "the exhaust speed is also dependent in an inverse fashion on the molecular mass of the exhaust products. For burning H2, you get H2O with a molecular mass of 18. " Are you saying the newer synthetic diamond rockets would worker better than the old-fashioned steam rockets? Or if it's molecular weight you want, maybe throwing old car batteries or even spent uranium from nuclear plants out the exhaust pipe would work, although the EPA might object because they want unleaded fuel? But even if you could overcome that minor problem, you still have to lift the mass to height h before you can throw it down again, have you considered that? What about an inverse cost fashion? Don't give up your day job just yet. |
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Storing gas at high temperature for rocket propellant.
On Aug 29, 3:13*pm, Robert Clark wrote:
This page gives the equation for the velocity of the exhaust gas of a rocket: Rocket engine nozzle.http://en.wikipedia.org/wiki/Rocket_...Analysis_of_ga... Since the Isp (specific impulse) of a propellant in units of seconds is found by just dividing this by 9.8 m/s^2, the Isp is maximized by making the exhaust speed as high as possible. In the formula this can be achieved by making the exhaust be high temperature. Usually in rockets this is done by using a high energy chemical reaction, such as by burning H2 with O2. However, in the formula you see the exhaust speed is also dependent in an inverse fashion on the molecular mass of the exhaust products. For burning H2, you get H2O with a molecular mass of 18. Can we get the exhaust gas simply by just H2 with a molecular mass of 2? One way this could be done would be simply by storing the hydrogen at high temperature. Since rocket launches last only about 8 minutes the tanks would only have to be insulated to maintain the temperature inside for that length of time. If we stored the hydrogen at 3000 K, the exhaust velocity in vacuum would be 9344 m/s, significantly better than the 4550 m/s maximum exhaust speed of H2/LOX engines. *The problem would be storing the H2 at the high temperature and the accompanying high pressure. Carbon-carbon composites are known to return their high strength at high temperature. This book reference gives the tensile strength as 700 MPa and states it *actually *increases* as temperature increases to the highest measured temperature given, 2000 K: http://books.google.com/books?id=d52...lpg=PA516&dq=c... * However, the melting point of carbon (actually it sublimates at 1 bar pressure) *is about 4000 K. Since the tensile strength is actually increasing at 2000 K quite likely it continues to increase beyond this and likely will remain high at least up to 3000 K. Carbon-carbon for example is used for rocket nozzles for temperatures exceeding 3000 K: Nondestructive Characterisation of Carbon/Carbon Brake Disks Using Ultrasonics. "C/C composite is consisted of a fiber based on carbon precursors embedded in a carbon matrix and has such properties as low density, high thermal conductivity and shock resistance, low thermal expansion and high modulus. The C/C composite is applied for structures in high temperature condition, such as a brake disk of aircraft, a nozzle of rocket engine and etc., because C/C composite not only withstands high temperature approaching 3000oC, but actually increases in strength."http://www.ndt.net/apcndt2001/papers/1109/1109.htm TW/SNTP - TECHNICAL CONCEPTS AND DEVELOPMENT ACTIVITIES. "The high exhaust temperature requires either a transpiration or regeneratively cooled nozzle, or a radiation-cooled carbon-carbon nozzle. The carbon-carbon nozzle was used as the baseline, given its low mass and simple design. Carbon-carbon nozzles have been tested in solid-rocket motors at temperatures up to 4000 K. But development of coatings (TaC, ZrC and NbC are candidates) will be required to avoid hydrogen erosion."http://www.fas.org/nuke/space/c08tw_3.htm *Carbon-carbon composites though are porous so it is uncertain if they can be used for hydrogen storage at high temperature. An advantage of the carbon-carbon though is that it could be used as a single high strength, high temperature tank rather than numerous microspheres or microtubes. * However, microspheres or microtubes might allow higher temperatures and/or pressures. For example synthetic diamond of micron-scale size can be made cheaply and may have higher tensile strength than natural diamond: Brief Communications Nature 421, 599-600 (6 February 2003) Materials: Ultrahard polycrystalline diamond from graphite. "Polycrystalline diamonds are harder and tougher than single-crystal diamonds and are therefore valuable for cutting and polishing other hard materials, but naturally occurring polycrystalline diamond is unusual and its production is slow. Here we describe the rapid synthesis of pure sintered polycrystalline diamond by direct conversion of graphite under static high pressure and temperature. Surprisingly, this synthesized diamond is ultrahard and so could be useful in the manufacture of scientific and industrial tools."http://www.nature.com/nature/journal/v421/n6923/full/421599b.html *Since these synthetic diamonds are harder than natural diamond, they very likely also are of higher tensile strength. This page says though there has been varying measured amounts for natural diamonds tensile strength one experiment, and some theoretical work, suggests it could be as high as 60 GPa: Material properties of diamond.http://en.wikipedia.org/wiki/Materia...ies_of_diamond *And this page says at pressures of 60 GPa, 600 kilobars, diamond can remain solid up to 6,000 K: Modeling the Phase Diagram of Carbon. PRL 94, 145701 (2005) PHYSICAL REVIEW LETTERS 15 APRIL 2005http://www.amolf.nl/publications/pdf/4312.pdf *At a temperature of 6,000 K, the H2 would have an exhaust velocity of 13,200 m/s. However, there would be the problem of keeping the diamond at the high pressure required to remain solid. You could supply the high pressure on the inside of the diamond microspheres by the H2 gas but how to apply the high pressure to the outside? *You would also have the problem of releasing the hydrogen when needed. One possibility might be to expose the diamond to oxygen. Carbon will burn in oxygen at temperatures of 600 C and above. The carbon tanks holding the H2 at high temperature will have to be kept in inert gas or in vacuum to prevent contact with oxygen until the H2 is to be released. *Another possibility for the high temperature material for the microspheres or microtubes to hold the H2 might be high temperature, refractory, materials. One is tantalum hafnium carbide, which has a melting point of about 4,500 K. These would also need to be made to have high tensile strength. It is common that when materials are made into 'whiskers' at the microscale they achieve GPa tensile strengths. One method to make the whiskers is the vapor-liquid-solid method: Growing Crystals with the VLS Process (Vapor - Liquid - Solid)http://www.hbci.com/~wenonah/new/crystals.htm *It is necessary to hold the hydrogen at high pressure since it will be a high temperature gas. For instance at room temperature, say 300 K, and at 1 bar, H2 has a density about 1/10th kg/m^3. So at 3,000 K the pressure would be 10 bar. However, at a density of only .1 kg/m^3, the volume would be prohibitive for tens of thousands to hundreds of thousands of kilos of H2. So to get a reasonable volume for the H2 we will need much higher pressure. By multiplying the density by a factor of 1,000 to 100 kg/m^3, somewhat better than that of liquid hydrogen, the pressure would also be multiplied by 1,000 to 10,000 bar, 1 GPa, with the temperature kept at 3,000 K. * * Bob Clark The book reference: http://books.google.com/books?id=d52...m=22&ct=result also shows that carbon fiber initially dips in tensile strength at high temperatures but then starts rising again as you approach 2000K so they may as well retain their strength at 3000K. So it may work to use them as microtubes since their tensile strength can be 10 times greater than carbon-carbon composites: 7 GPa, 1,000,000 psi. However, it still needs to be determined if they can retain this strength radially as hollow tubes. The highest known strength would be obtained by carbon nanotubes or fullerenes. Experiments have shown they can have tensile strength as high as 150 GPa. A problem with using them however is the hydrogen molecule is so small that in experiments with nanotubes at high pressures some of the hydrogen leaks out between the carbon atoms of the nanotubes. Perhaps this can be solved with multiwalled nanotubes or fullerene "onions" by having the layers be arranged so that a carbon atom of one layer blocks the opening in another layer. Bob Clark |
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Storing gas at high temperature for rocket propellant.
Dear Robert Clark:
"Robert Clark" wrote in message ... .... The highest known strength would be obtained by carbon nanotubes or fullerenes. Experiments have shown they can have tensile strength as high as 150 GPa. A problem with using them however is the hydrogen molecule is so small that in experiments with nanotubes at high pressures some of the hydrogen leaks out between the carbon atoms of the nanotubes. Perhaps this can be solved with multiwalled nanotubes or fullerene "onions" by having the layers be arranged so that a carbon atom of one layer blocks the opening in another layer. High temperature hydrogen will attack the carbon matrix, and you will have a massive failure. http://www.pubmedcentral.nih.gov/art...?artid=1091643 David A. Smith |
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Storing gas at high temperature for rocket propellant.
On Aug 30, 12:44 pm, "N:dlzc D:aol T:com \(dlzc\)"
wrote: Dear Robert Clark: "Robert Clark" wrote in message ... ... The highest known strength would be obtained by carbon nanotubes or fullerenes. Experiments have shown they can have tensile strength as high as 150 GPa. A problem with using them however is the hydrogen molecule is so small that in experiments with nanotubes at high pressures some of the hydrogen leaks out between the carbon atoms of the nanotubes. Perhaps this can be solved with multiwalled nanotubes or fullerene "onions" by having the layers be arranged so that a carbon atom of one layer blocks the opening in another layer. High temperature hydrogen will attack the carbon matrix, and you will have a massive failure.http://www.pubmedcentral.nih.gov/art...?artid=1091643 David A. Smith An interesting article. Specifically it is about H3: Trihydrogen cation. http://en.wikipedia.org/wiki/Trihydrogen_cation This is apparently highly reactive. Anyone know the energy release when reacted with oxygen? H3 appears when hydrogen is ionized. Perhaps it won't be too prevalent at the lower end of the temperatures I mentioned, say at 3000 K. We might be able to coat the carbon tanks with highly refractory materials such as tantalum hafnium carbide which has a melting point of 4500 K. Bob Clark |
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Storing gas at high temperature for rocket propellant.
On Aug 30, 6:25 am, Robert Clark wrote:
On Aug 29, 3:13 pm, Robert Clark wrote: This page gives the equation for the velocity of the exhaust gas of a rocket: Rocket engine nozzle.http://en.wikipedia.org/wiki/Rocket_...Analysis_of_ga... Since the Isp (specific impulse) of a propellant in units of seconds is found by just dividing this by 9.8 m/s^2, the Isp is maximized by making the exhaust speed as high as possible. In the formula this can be achieved by making the exhaust be high temperature. Usually in rockets this is done by using a high energy chemical reaction, such as by burning H2 with O2. However, in the formula you see the exhaust speed is also dependent in an inverse fashion on the molecular mass of the exhaust products. For burning H2, you get H2O with a molecular mass of 18. Can we get the exhaust gas simply by just H2 with a molecular mass of 2? One way this could be done would be simply by storing the hydrogen at high temperature. Since rocket launches last only about 8 minutes the tanks would only have to be insulated to maintain the temperature inside for that length of time. If we stored the hydrogen at 3000 K, the exhaust velocity in vacuum would be 9344 m/s, significantly better than the 4550 m/s maximum exhaust speed of H2/LOX engines. The problem would be storing the H2 at the high temperature and the accompanying high pressure. Carbon-carbon composites are known to return their high strength at high temperature. This book reference gives the tensile strength as 700 MPa and states it actually *increases* as temperature increases to the highest measured temperature given, 2000 K: http://books.google.com/books?id=d52...lpg=PA516&dq=c... However, the melting point of carbon (actually it sublimates at 1 bar pressure) is about 4000 K. Since the tensile strength is actually increasing at 2000 K quite likely it continues to increase beyond this and likely will remain high at least up to 3000 K. Carbon-carbon for example is used for rocket nozzles for temperatures exceeding 3000 K: Nondestructive Characterisation of Carbon/Carbon Brake Disks Using Ultrasonics. "C/C composite is consisted of a fiber based on carbon precursors embedded in a carbon matrix and has such properties as low density, high thermal conductivity and shock resistance, low thermal expansion and high modulus. The C/C composite is applied for structures in high temperature condition, such as a brake disk of aircraft, a nozzle of rocket engine and etc., because C/C composite not only withstands high temperature approaching 3000oC, but actually increases in strength."http://www.ndt.net/apcndt2001/papers/1109/1109.htm TW/SNTP - TECHNICAL CONCEPTS AND DEVELOPMENT ACTIVITIES. "The high exhaust temperature requires either a transpiration or regeneratively cooled nozzle, or a radiation-cooled carbon-carbon nozzle. The carbon-carbon nozzle was used as the baseline, given its low mass and simple design. Carbon-carbon nozzles have been tested in solid-rocket motors at temperatures up to 4000 K. But development of coatings (TaC, ZrC and NbC are candidates) will be required to avoid hydrogen erosion."http://www.fas.org/nuke/space/c08tw_3.htm Carbon-carbon composites though are porous so it is uncertain if they can be used for hydrogen storage at high temperature. An advantage of the carbon-carbon though is that it could be used as a single high strength, high temperature tank rather than numerous microspheres or microtubes. However, microspheres or microtubes might allow higher temperatures and/or pressures. For example synthetic diamond of micron-scale size can be made cheaply and may have higher tensile strength than natural diamond: Brief Communications Nature 421, 599-600 (6 February 2003) Materials: Ultrahard polycrystalline diamond from graphite. "Polycrystalline diamonds are harder and tougher than single-crystal diamonds and are therefore valuable for cutting and polishing other hard materials, but naturally occurring polycrystalline diamond is unusual and its production is slow. Here we describe the rapid synthesis of pure sintered polycrystalline diamond by direct conversion of graphite under static high pressure and temperature. Surprisingly, this synthesized diamond is ultrahard and so could be useful in the manufacture of scientific and industrial tools."http://www.nature.com/nature/journal/v421/n6923/full/421599b.html Since these synthetic diamonds are harder than natural diamond, they very likely also are of higher tensile strength. This page says though there has been varying measured amounts for natural diamonds tensile strength one experiment, and some theoretical work, suggests it could be as high as 60 GPa: Material properties of diamond.http://en.wikipedia.org/wiki/Materia...ies_of_diamond And this page says at pressures of 60 GPa, 600 kilobars, diamond can remain solid up to 6,000 K: Modeling the Phase Diagram of Carbon. PRL 94, 145701 (2005) PHYSICAL REVIEW LETTERS 15 APRIL 2005http://www.amolf.nl/publications/pdf/4312.pdf At a temperature of 6,000 K, the H2 would have an exhaust velocity of 13,200 m/s. However, there would be the problem of keeping the diamond at the high pressure required to remain solid. You could supply the high pressure on the inside of the diamond microspheres by the H2 gas but how to apply the high pressure to the outside? You would also have the problem of releasing the hydrogen when needed. One possibility might be to expose the diamond to oxygen. Carbon will burn in oxygen at temperatures of 600 C and above. The carbon tanks holding the H2 at high temperature will have to be kept in inert gas or in vacuum to prevent contact with oxygen until the H2 is to be released. Another possibility for the high temperature material for the microspheres or microtubes to hold the H2 might be high temperature, refractory, materials. One is tantalum hafnium carbide, which has a melting point of about 4,500 K. These would also need to be made to have high tensile strength. It is common that when materials are made into 'whiskers' at the microscale they achieve GPa tensile strengths. One method to make the whiskers is the vapor-liquid-solid method: Growing Crystals with the VLS Process (Vapor - Liquid - Solid)http://www.hbci.com/~wenonah/new/crystals.htm It is necessary to hold the hydrogen at high pressure since it will be a high temperature gas. For instance at room temperature, say 300 K, and at 1 bar, H2 has a density about 1/10th kg/m^3. So at 3,000 K the pressure would be 10 bar. However, at a density of only .1 kg/m^3, the volume would be prohibitive for tens of thousands to hundreds of thousands of kilos of H2. So to get a reasonable volume for the H2 we will need much higher pressure. By multiplying the density by a factor of 1,000 to 100 kg/m^3, somewhat better than that of liquid hydrogen, the pressure would also be multiplied by 1,000 to 10,000 bar, 1 GPa, with the temperature kept at 3,000 K. Bob Clark The book reference: http://books.google.com/books?id=d52...lpg=PA516&dq=c... also shows that carbon fiber initially dips in tensile strength at high temperatures but then starts rising again as you approach 2000K so they may as well retain their strength at 3000K. So it may work to use them as microtubes since their tensile strength can be 10 times greater than carbon-carbon composites: 7 GPa, 1,000,000 psi. However, it still needs to be determined if they can retain this strength radially as hollow tubes. The highest known strength would be obtained by carbon nanotubes or fullerenes. Experiments have shown they can have tensile strength as high as 150 GPa. A problem with using them however is the hydrogen molecule is so small that in experiments with nanotubes at high pressures some of the hydrogen leaks out between the carbon atoms of the nanotubes. Perhaps this can be solved with multiwalled nanotubes or fullerene "onions" by having the layers be arranged so that a carbon atom of one layer blocks the opening in another layer. Bob Clark There's no problem in using commercial basalt composites (plasma metallic coated if need be) for safe containment of h2o2, much less that of the c12h26 or whatever else gets the most thrust energy/kg out of the h2o2. ~ Brad Guth Brad_Guth Brad.Guth BradGuth |
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Storing gas at high temperature for rocket propellant.
On Aug 30, 10:52*am, BradGuth wrote:
On Aug 30, 6:25 am, Robert Clark wrote: On Aug 29, 3:13 pm, Robert Clark wrote: This page gives the equation for the velocity of the exhaust gas of a rocket: Rocket engine nozzle.http://en.wikipedia.org/wiki/Rocket_...Analysis_of_ga... Since the Isp (specific impulse) of a propellant in units of seconds is found by just dividing this by 9.8 m/s^2, the Isp is maximized by making the exhaust speed as high as possible. In the formula this can be achieved by making the exhaust be high temperature. Usually in rockets this is done by using a high energy chemical reaction, such as by burning H2 with O2. However, in the formula you see the exhaust speed is also dependent in an inverse fashion on the molecular mass of the exhaust products. For burning H2, you get H2O with a molecular mass of 18. Can we get the exhaust gas simply by just H2 with a molecular mass of 2? One way this could be done would be simply by storing the hydrogen at high temperature. Since rocket launches last only about 8 minutes the tanks would only have to be insulated to maintain the temperature inside for that length of time. If we stored the hydrogen at 3000 K, the exhaust velocity in vacuum would be 9344 m/s, significantly better than the 4550 m/s maximum exhaust speed of H2/LOX engines. *The problem would be storing the H2 at the high temperature and the accompanying high pressure. Carbon-carbon composites are known to return their high strength at high temperature. This book reference gives the tensile strength as 700 MPa and states it *actually *increases* as temperature increases to the highest measured temperature given, 2000 K: http://books.google.com/books?id=d52...lpg=PA516&dq=c... * However, the melting point of carbon (actually it sublimates at 1 bar pressure) *is about 4000 K. Since the tensile strength is actually increasing at 2000 K quite likely it continues to increase beyond this and likely will remain high at least up to 3000 K. Carbon-carbon for example is used for rocket nozzles for temperatures exceeding 3000 K: Nondestructive Characterisation of Carbon/Carbon Brake Disks Using Ultrasonics. "C/C composite is consisted of a fiber based on carbon precursors embedded in a carbon matrix and has such properties as low density, high thermal conductivity and shock resistance, low thermal expansion and high modulus. The C/C composite is applied for structures in high temperature condition, such as a brake disk of aircraft, a nozzle of rocket engine and etc., because C/C composite not only withstands high temperature approaching 3000oC, but actually increases in strength."http://www.ndt.net/apcndt2001/papers/1109/1109.htm TW/SNTP - TECHNICAL CONCEPTS AND DEVELOPMENT ACTIVITIES. "The high exhaust temperature requires either a transpiration or regeneratively cooled nozzle, or a radiation-cooled carbon-carbon nozzle. The carbon-carbon nozzle was used as the baseline, given its low mass and simple design. Carbon-carbon nozzles have been tested in solid-rocket motors at temperatures up to 4000 K. But development of coatings (TaC, ZrC and NbC are candidates) will be required to avoid hydrogen erosion."http://www.fas.org/nuke/space/c08tw_3.htm *Carbon-carbon composites though are porous so it is uncertain if they can be used for hydrogen storage at high temperature. An advantage of the carbon-carbon though is that it could be used as a single high strength, high temperature tank rather than numerous microspheres or microtubes. * However, microspheres or microtubes might allow higher temperatures and/or pressures. For example synthetic diamond of micron-scale size can be made cheaply and may have higher tensile strength than natural diamond: Brief Communications Nature 421, 599-600 (6 February 2003) Materials: Ultrahard polycrystalline diamond from graphite. "Polycrystalline diamonds are harder and tougher than single-crystal diamonds and are therefore valuable for cutting and polishing other hard materials, but naturally occurring polycrystalline diamond is unusual and its production is slow. Here we describe the rapid synthesis of pure sintered polycrystalline diamond by direct conversion of graphite under static high pressure and temperature. Surprisingly, this synthesized diamond is ultrahard and so could be useful in the manufacture of scientific and industrial tools."http://www.nature.com/nature/journal/v421/n6923/full/421599b.html *Since these synthetic diamonds are harder than natural diamond, they very likely also are of higher tensile strength. This page says though there has been varying measured amounts for natural diamonds tensile strength one experiment, and some theoretical work, suggests it could be as high as 60 GPa: Material properties of diamond.http://en.wikipedia.org/wiki/Materia...ies_of_diamond *And this page says at pressures of 60 GPa, 600 kilobars, diamond can remain solid up to 6,000 K: Modeling the Phase Diagram of Carbon. PRL 94, 145701 (2005) PHYSICAL REVIEW LETTERS 15 APRIL 2005http://www..amolf.nl/publications/pdf/4312.pdf *At a temperature of 6,000 K, the H2 would have an exhaust velocity of 13,200 m/s. However, there would be the problem of keeping the diamond at the high pressure required to remain solid. You could supply the high pressure on the inside of the diamond microspheres by the H2 gas but how to apply the high pressure to the outside? *You would also have the problem of releasing the hydrogen when needed. One possibility might be to expose the diamond to oxygen. Carbon will burn in oxygen at temperatures of 600 C and above. The carbon tanks holding the H2 at high temperature will have to be kept in inert gas or in vacuum to prevent contact with oxygen until the H2 is to be released. *Another possibility for the high temperature material for the microspheres or microtubes to hold the H2 might be high temperature, refractory, materials. One is tantalum hafnium carbide, which has a melting point of about 4,500 K. These would also need to be made to have high tensile strength. It is common that when materials are made into 'whiskers' at the microscale they achieve GPa tensile strengths. One method to make the whiskers is the vapor-liquid-solid method: Growing Crystals with the VLS Process (Vapor - Liquid - Solid)http://www.hbci.com/~wenonah/new/crystals.htm *It is necessary to hold the hydrogen at high pressure since it will be a high temperature gas. For instance at room temperature, say 300 K, and at 1 bar, H2 has a density about 1/10th kg/m^3. So at 3,000 K the pressure would be 10 bar. However, at a density of only .1 kg/m^3, the volume would be prohibitive for tens of thousands to hundreds of thousands of kilos of H2. So to get a reasonable volume for the H2 we will need much higher pressure. By multiplying the density by a factor of 1,000 to 100 kg/m^3, somewhat better than that of liquid hydrogen, the pressure would also be multiplied by 1,000 to 10,000 bar, 1 GPa, with the temperature kept at 3,000 K. * * Bob Clark * The book reference: http://books.google.com/books?id=d52...lpg=PA516&dq=c... *also shows that carbon fiber initially dips in tensile strength at high temperatures but then starts rising again as you approach 2000K so they may as well retain their strength at 3000K. So it may work to use them as microtubes since their tensile strength can be 10 times greater than carbon-carbon composites: 7 GPa, *1,000,000 psi. However, it still needs to be determined if they can retain this strength radially as hollow tubes. *The highest known strength would be obtained by carbon nanotubes or fullerenes. Experiments have shown they can have tensile strength as high as 150 GPa. A problem with using them however is the hydrogen molecule is so small that in experiments with nanotubes at high pressures some of the hydrogen leaks out between the carbon atoms of the nanotubes. Perhaps this can be solved with multiwalled nanotubes or fullerene "onions" by having the layers be arranged so that a carbon atom of one layer blocks the opening in another layer. * * Bob Clark There's no problem in using commercial basalt composites (plasma metallic coated if need be) for safe containment of h2o2, much less that of the c12h26 or whatever else gets the most thrust energy/kg out of the h2o2. * ~ Brad Guth Brad_Guth Brad.Guth BradGuth Hydrogen peroxide as fuel is stupid. Enormously stupid. Its' like mixing liquid oxygen and liquid hydrogen together in one tank stupid. |
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Storing gas at high temperature for rocket propellant.
On Aug 30, 1:19 pm, Eric Gisse wrote:
On Aug 30, 10:52 am, BradGuth wrote: On Aug 30, 6:25 am, Robert Clark wrote: On Aug 29, 3:13 pm, Robert Clark wrote: This page gives the equation for the velocity of the exhaust gas of a rocket: Rocket engine nozzle.http://en.wikipedia.org/wiki/Rocket_...Analysis_of_ga... Since the Isp (specific impulse) of a propellant in units of seconds is found by just dividing this by 9.8 m/s^2, the Isp is maximized by making the exhaust speed as high as possible. In the formula this can be achieved by making the exhaust be high temperature. Usually in rockets this is done by using a high energy chemical reaction, such as by burning H2 with O2. However, in the formula you see the exhaust speed is also dependent in an inverse fashion on the molecular mass of the exhaust products. For burning H2, you get H2O with a molecular mass of 18. Can we get the exhaust gas simply by just H2 with a molecular mass of 2? One way this could be done would be simply by storing the hydrogen at high temperature. Since rocket launches last only about 8 minutes the tanks would only have to be insulated to maintain the temperature inside for that length of time. If we stored the hydrogen at 3000 K, the exhaust velocity in vacuum would be 9344 m/s, significantly better than the 4550 m/s maximum exhaust speed of H2/LOX engines. The problem would be storing the H2 at the high temperature and the accompanying high pressure. Carbon-carbon composites are known to return their high strength at high temperature. This book reference gives the tensile strength as 700 MPa and states it actually *increases* as temperature increases to the highest measured temperature given, 2000 K: http://books.google.com/books?id=d52...lpg=PA516&dq=c... However, the melting point of carbon (actually it sublimates at 1 bar pressure) is about 4000 K. Since the tensile strength is actually increasing at 2000 K quite likely it continues to increase beyond this and likely will remain high at least up to 3000 K. Carbon-carbon for example is used for rocket nozzles for temperatures exceeding 3000 K: Nondestructive Characterisation of Carbon/Carbon Brake Disks Using Ultrasonics. "C/C composite is consisted of a fiber based on carbon precursors embedded in a carbon matrix and has such properties as low density, high thermal conductivity and shock resistance, low thermal expansion and high modulus. The C/C composite is applied for structures in high temperature condition, such as a brake disk of aircraft, a nozzle of rocket engine and etc., because C/C composite not only withstands high temperature approaching 3000oC, but actually increases in strength."http://www.ndt.net/apcndt2001/papers/1109/1109.htm TW/SNTP - TECHNICAL CONCEPTS AND DEVELOPMENT ACTIVITIES. "The high exhaust temperature requires either a transpiration or regeneratively cooled nozzle, or a radiation-cooled carbon-carbon nozzle. The carbon-carbon nozzle was used as the baseline, given its low mass and simple design. Carbon-carbon nozzles have been tested in solid-rocket motors at temperatures up to 4000 K. But development of coatings (TaC, ZrC and NbC are candidates) will be required to avoid hydrogen erosion."http://www.fas.org/nuke/space/c08tw_3.htm Carbon-carbon composites though are porous so it is uncertain if they can be used for hydrogen storage at high temperature. An advantage of the carbon-carbon though is that it could be used as a single high strength, high temperature tank rather than numerous microspheres or microtubes. However, microspheres or microtubes might allow higher temperatures and/or pressures. For example synthetic diamond of micron-scale size can be made cheaply and may have higher tensile strength than natural diamond: Brief Communications Nature 421, 599-600 (6 February 2003) Materials: Ultrahard polycrystalline diamond from graphite. "Polycrystalline diamonds are harder and tougher than single-crystal diamonds and are therefore valuable for cutting and polishing other hard materials, but naturally occurring polycrystalline diamond is unusual and its production is slow. Here we describe the rapid synthesis of pure sintered polycrystalline diamond by direct conversion of graphite under static high pressure and temperature. Surprisingly, this synthesized diamond is ultrahard and so could be useful in the manufacture of scientific and industrial tools."http://www.nature.com/nature/journal/v421/n6923/full/421599b.html Since these synthetic diamonds are harder than natural diamond, they very likely also are of higher tensile strength. This page says though there has been varying measured amounts for natural diamonds tensile strength one experiment, and some theoretical work, suggests it could be as high as 60 GPa: Material properties of diamond.http://en.wikipedia.org/wiki/Materia...ies_of_diamond And this page says at pressures of 60 GPa, 600 kilobars, diamond can remain solid up to 6,000 K: Modeling the Phase Diagram of Carbon. PRL 94, 145701 (2005) PHYSICAL REVIEW LETTERS 15 APRIL 2005http://www.amolf.nl/publications/pdf/4312.pdf At a temperature of 6,000 K, the H2 would have an exhaust velocity of 13,200 m/s. However, there would be the problem of keeping the diamond at the high pressure required to remain solid. You could supply the high pressure on the inside of the diamond microspheres by the H2 gas but how to apply the high pressure to the outside? You would also have the problem of releasing the hydrogen when needed. One possibility might be to expose the diamond to oxygen. Carbon will burn in oxygen at temperatures of 600 C and above. The carbon tanks holding the H2 at high temperature will have to be kept in inert gas or in vacuum to prevent contact with oxygen until the H2 is to be released. Another possibility for the high temperature material for the microspheres or microtubes to hold the H2 might be high temperature, refractory, materials. One is tantalum hafnium carbide, which has a melting point of about 4,500 K. These would also need to be made to have high tensile strength. It is common that when materials are made into 'whiskers' at the microscale they achieve GPa tensile strengths. One method to make the whiskers is the vapor-liquid-solid method: Growing Crystals with the VLS Process (Vapor - Liquid - Solid)http://www.hbci.com/~wenonah/new/crystals.htm It is necessary to hold the hydrogen at high pressure since it will be a high temperature gas. For instance at room temperature, say 300 K, and at 1 bar, H2 has a density about 1/10th kg/m^3. So at 3,000 K the pressure would be 10 bar. However, at a density of only .1 kg/m^3, the volume would be prohibitive for tens of thousands to hundreds of thousands of kilos of H2. So to get a reasonable volume for the H2 we will need much higher pressure. By multiplying the density by a factor of 1,000 to 100 kg/m^3, somewhat better than that of liquid hydrogen, the pressure would also be multiplied by 1,000 to 10,000 bar, 1 GPa, with the temperature kept at 3,000 K. Bob Clark The book reference: http://books.google.com/books?id=d52...lpg=PA516&dq=c... also shows that carbon fiber initially dips in tensile strength at high temperatures but then starts rising again as you approach 2000K so they may as well retain their strength at 3000K. So it may work to use them as microtubes since their tensile strength can be 10 times greater than carbon-carbon composites: 7 GPa, 1,000,000 psi. However, it still needs to be determined if they can retain this strength radially as hollow tubes. The highest known strength would be obtained by carbon nanotubes or fullerenes. Experiments have shown they can have tensile strength as high as 150 GPa. A problem with using them however is the hydrogen molecule is so small that in experiments with nanotubes at high pressures some of the hydrogen leaks out between the carbon atoms of the nanotubes. Perhaps this can be solved with multiwalled nanotubes or fullerene "onions" by having the layers be arranged so that a carbon atom of one layer blocks the opening in another layer. Bob Clark There's no problem in using commercial basalt composites (plasma metallic coated if need be) for safe containment of h2o2, much less that of the c12h26 or whatever else gets the most thrust energy/kg out of the h2o2. ~ Brad Guth Brad_Guth Brad.Guth BradGuth Hydrogen peroxide as fuel is stupid. Enormously stupid. Its' like mixing liquid oxygen and liquid hydrogen together in one tank stupid. Your profound but typically foolish nayism is noted. The combined fuel and bulk of h2o2 oxidizer as fly-by-rocket energy density that isn't cryogenic or having to be pressurized is actually offering a fairly good Isp, especially once taking the all inclusive GLOW inert mass into account. ~ Brad Guth Brad_Guth Brad.Guth BradGuth |
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Storing gas at high temperature for rocket propellant.
Brad, We've gone over this before. The only person who is naysaying around here is YOU! You don't want to hear, or remember things that run counter to what you want to be true - regardless of their truth or falsity. lol. Why is that Brad? Because of the way those beliefs allow you to FEEL about yourself. haha.. GIVE IT UP ASSHOLE! lol. Check it out dude; - these are FACTS - not fiction - so, i realize you have a little difficulty dealing with them; As a monopropellant rocket at 98% concentration specific impulse is 160 seconds. (the SSME has a specific impulse of 455 seconds) As a fuel it contains 2.7 MJ/kg (gasoline contains 46.9 MJ/kg) As a cost-effective fuel it costs $40 per kg http://www.h2o2-4u.com/price.html gasoline costs $1.20 per kg The high costs are the result of the difficulty of manufacturing the stuff and its instability. The high costs have to do with the method by which hydrogen peroxide is manufactured. About 500,000 tons of hydrogen peroxide is produced in the USA each year, primarily as "green" bleaching agents such as perborates and percarbonates for the paper and textile industries. Other significant uses include wastewater treatment and hydrometallurgical processes (for example, the extraction of uranium by oxidation). The most widely used processing method is the AO (Autoxidation) process. A reaction mixture is fed to the first reactor which contains a carrier solvent and anthraquinones (usually 2-ethyl or 2-pentyl- anthraquinone). A stream containing the hydrocarbon-based carrier solvent is usually referred to as the "work solution". This first reactor in the series of two is known as the hydrogenator as hydgrogen is also fed to this reactor and a hydrogenation reaction occurs over a Ni or Pd catalysts. The products from the hydrogenator are filtered (to remove catalyst particles) and cooled before being fed to the second reactor which is referred to as the oxidizer. In the second reactor, air or oxygen enriched air is introduced to the work solution to reverse the previous reaction via oxidation. The contaminated air from the oxidizer is fed to a carbon adsorption unit and then to a vent condenser. The work solution, now containing nearly 40% hydrogen peroxide by weight, is cooled once again before being fed to a liquid-liquid extraction unit. Water is fed to the extractor and acts as the extracting agent. The hydrogen peroxide is miscible in water while the solvents are not. Then the H2O2-water layer can be removed and sent to Vacuum Column I and the solvent is sent to be purified before it is recycled. Feed to Vacuum Column I is preheated with the column condensate (mostly water) which is then either refluxed back to the column or sent to the extractor. In some cases, there are multiple columns to separate the H2O2-water mixture from the extractor depending on the deserved purity of the product). While water is removed as an overhead product, the hydrogen peroxide is further concentrated as the bottom product. Finally, the hydrogen peroxide product is cooled before being treated with an inhibitor (to prevent oxidation) and sent to storage. So, there you have it. Now, despite its high cost, and despite its low energy content, hydrogen peroxide has seen use as a rocket propellant, and as fuel in specialty applications, like torpedoes that have to work underwater without air. I have even suggested Brad that if you have a better way to make H2O2 - than the process described above - one that is cheaper and more productive - then the first step is to implement that process and OWN the BLEACH markets. After that, you can do whatever the hell you want! lol. You'd be a billionaire. There are even applications that H2O2 would be ideally suited for that could be developed. These applications are niche markets, but they're still HUGE.. A 60% solution of the stuff, does not pose an explosion risk - but would be dandy to drive a small steam source to power a MEMs scale steam turbine to power laptops and portable equipment reliably. In resonse to a request from you Brad I even worked out a technique to use H2O2 as a solvent in an ink to produce self powered inkjet printheads. haha - that is, you have portable inkjet printers that are powered by the ink they use. H2O2 with 2.7 MJ/kg despite its terrible energy density is about 5x as energy dense as a lithium ion battery. So, you could have a dandy little package for cell phones or laptops that would last 5x longer than batteries, and be recharged with $1 refills purchase at your local CVS. This would make several billions - per year. - something to do after you've dominated the bleach markets. A larger version might also even drive a pollution free electric car - like the Tesla - but you wouldn't be able to recharge it efficiently and the mess you'd have if you had a wreck! You'd have to carry hundreds of gallons of the stuff ...and you'd never really compete with batteries - a refill would cost nearly a thousand dollars - but there are those that would proudly pay it I'm sure - ifyou advertised properly - and they did it with a solar panel attached to the equipment. So, Brad, despite your idea being dumb, i have worked out a way for you to develop this economically - and for two years you've done nothing, while at the same time, totally ignored reality. Which proves what I said at the outset. You don't care about reality. You only care about how running your mouth makes you feel - and that's you in a nutshell. .. .. |
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