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http://square.cjb.cc/bolts.htm
"Self Tightening Bolts theory. Warning: this page is only a theory, not a fact." That's a good description. Could someone please explain what self-tightening and self-locking bolts are and give examples. The author may have the latter in mind. "Figure 4.1 This picture explains the great inertia and centrifugal force" "When ever there is a difference in inertial force (as pointed out with the arrows) the pulley will move. Not 180-ft-lb torque can hold the pulley still." I wonder what this is about. |
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karl wrote:
> "Figure 4.1 This picture explains the great inertia and > centrifugal force" As a complete aside, this reminds me of a former high-school physics teacher's pet rant: "centrifual" force, or the observed outward-from-center force on a spinning object, he would always insist, is not a real force. The real force in play is centripetal force, or the tendency of the point on the object wanting to continue in a straight direction on tangent to the spin, is the ACTUAL force at work. "Centrifugal" force is only an imaginary thing. --- avast! Antivirus: Outbound message clean. Virus Database (VPS): 0545-0, 11/07/2005 Tested on: 11/7/2005 6:12:53 PM avast! - copyright (c) 1988-2005 ALWIL Software. http://www.avast.com |
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"karl" <ottokarl@cognisurf.com> wrote in message news:1131379111.763649.136380@g14g2000cwa.googlegr oups.com...
> http://square.cjb.cc/bolts.htm > "Self Tightening Bolts theory. > Warning: this page is only a theory, not a fact." > That's a good description. > Could someone please explain what self-tightening and > self-locking bolts are and give examples. The author may > have the latter in mind. > "Figure 4.1 This picture explains the great inertia and > centrifugal force" > "When ever there is a difference in inertial force (as > pointed out with the arrows) the pulley will move. Not > 180-ft-lb torque can hold the pulley still." > I wonder what this is about. What this mean is that the object in motion will move in the direction of movement. But when there is a force that tries to change that motion usually from the engine or transmission the pulley will move when it's not intended to. Scroll down to Figure 4.2. It may explain more about centrifugal force not centripetal force. Centripetal is moving or directed toward a center or axis. The theory is that the centrifugal force can effect the bolt's movement in some way or just simply tighten up bolt. |
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Burt S. wrote:
> "karl" <ottokarl@cognisurf.com> wrote in message news:1131379111.763649.136380@g14g2000cwa.googlegr oups.com... > >>http://square.cjb.cc/bolts.htm > > >> "Self Tightening Bolts theory. >> Warning: this page is only a theory, not a fact." > > >>That's a good description. > > >>Could someone please explain what self-tightening and >>self-locking bolts are and give examples. The author may >>have the latter in mind. > > >> "Figure 4.1 This picture explains the great inertia and >> centrifugal force" >> "When ever there is a difference in inertial force (as >> pointed out with the arrows) the pulley will move. Not >> 180-ft-lb torque can hold the pulley still." > > >>I wonder what this is about. > > > What this mean is that the object in motion will move in the direction > of movement. But when there is a force that tries to change that > motion usually from the engine or transmission the pulley will move > when it's not intended to. Scroll down to Figure 4.2. It may explain > more about centrifugal force not centripetal force. Centripetal is > moving or directed toward a center or axis. The theory is that the > centrifugal force can effect the bolt's movement in some way or > just simply tighten up bolt. http://en.wikipedia.org/wiki/Centrifugal_force --- avast! Antivirus: Outbound message clean. Virus Database (VPS): 0545-0, 11/07/2005 Tested on: 11/8/2005 9:27:05 AM avast! - copyright (c) 1988-2005 ALWIL Software. http://www.avast.com |
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"karl" <ottokarl@cognisurf.com> wrote in message
news:1131379111.763649.136380@g14g2000cwa.googlegr oups.com... > http://square.cjb.cc/bolts.htm > > "Self Tightening Bolts theory. > Warning: this page is only a theory, not a fact." > > > That's a good description. > > Could someone please explain what self-tightening and > self-locking bolts are and give examples. The author may > have the latter in mind. > > > > "Figure 4.1 This picture explains the great inertia and > centrifugal force" > > "When ever there is a difference in inertial force (as > pointed out with the arrows) the pulley will move. Not > 180-ft-lb torque can hold the pulley still." > > > I wonder what this is about. > I am unconvinced by this theory. 1) If microscopic ratchet teeth are created to cause the bolt to self-tighten, wouldn't they be destroyed when the god-awful tight bolt is broken loose? The bolt at least should be specified as a "use once" item, regardless of how the mating threads in the crank fare. 2) In order to tighten, the bolt will have to move with respect to the pulley. That means the washer must have similar ratcheting action, and on a similar microscopic level to allow the ratchet to occur with miniscule motion. That means if the washer is less than pristine and is reused the bolt won't self-tighten. 3) The forces are downright outrageous. In round numbers, if the washer diameter is 1/2 inch and the bolt thread diameter is 1/4 inch, to tighten past the 200 ft-lb mark the bolt head has to experience 5000 pounds force from one side to the other, or 10000 pounds force on one side relative to the center. The equivalent force on the thread is double that. 4) If there is significant motion of the pulley relative to the crank, the mating surfaces will wallow out. We see it often enough with splined drive axles that are insufficiently torqued. Altogether, it doesn't add up. Torsional forces between the pulley and crank must act unidirectionally on the bolt, with several tons of force being transferred through both sides of the washer and without damaging the pulley or crank mating surfaces, with enough movement to materially tighten the bolt. The theorized ratchet mechanism has to operate on a microscopic basis, not be damaged in removal, and to allow effortless unthreading when the bolt is broken loose. It must work over a wide range of lubrication, including a penetrant oil film or being cleaned with brake cleaner. I'm glad I haven't been asked to design something like that, particularly if I could just specify tightening to a different torque in the first place. Mike |
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"Michael Pardee" <michaeltnull@cybertrails.com> wrote
> "karl" <ottokarl@cognisurf.com> wrote > > http://square.cjb.cc/bolts.htm > > > > "Self Tightening Bolts theory. > > Warning: this page is only a theory, not a fact." > > > > > > That's a good description. > > > > Could someone please explain what self-tightening and > > self-locking bolts are and give examples. The author may > > have the latter in mind. > > > > > > > > "Figure 4.1 This picture explains the great inertia and > > centrifugal force" > > > > "When ever there is a difference in inertial force (as > > pointed out with the arrows) the pulley will move. Not > > 180-ft-lb torque can hold the pulley still." > > > > > > I wonder what this is about. > > > I am unconvinced by this theory. > > 1) If microscopic ratchet teeth are created to cause the bolt to > self-tighten, wouldn't they be destroyed when the god-awful tight bolt is > broken loose? The bolt at least should be specified as a "use once" item, > regardless of how the mating threads in the crank fare. > > 2) In order to tighten, the bolt will have to move with respect to the > pulley. That means the washer must have similar ratcheting action, and on a > similar microscopic level to allow the ratchet to occur with miniscule > motion. That means if the washer is less than pristine and is reused the > bolt won't self-tighten. > > 3) The forces are downright outrageous. In round numbers, if the washer > diameter is 1/2 inch and the bolt thread diameter is 1/4 inch, to tighten > past the 200 ft-lb mark the bolt head has to experience 5000 pounds force > from one side to the other, or 10000 pounds force on one side relative to > the center. The equivalent force on the thread is double that. It's the stresses in the bolt, not the forces acting on the side of it, that matter. Specifically, torquing down on a bolt is the equivalent of stretching it until it holds two things together. The torquing causes the threads to act against each other so as to place the bolt in tension (as opposed to compression). For correlating torque to the axial load it produces, one finds somewhat crude estimates like that given at the bottom of http://www.engineersedge.com/torque.htm . But of course, this formula will require tweaking depending on conditions. E.g. fine thread vs. coarse thread. Anyway, it's really about 200 ft-lbs. divided over the six edges of the roughly 1.7/2 cm (= about .33 inch = about 0.028 foot) radius bolt head (for a 91 Civic, for one), anyway. (This Civic's pulley bolt has a 17 mm head and 14 mm nominal diameter.) So something like 200/6/(0.028) = about 1200 pounds is applied to each bolt head edge. Key word being "edge." Then one has to think about what it means to "apply" this force to the whole edge. It's distributed over the surface of the edge, for one thing. If one took 1200 lbs. and set it on a bar of steel with a cross-sectional area of about 1/8 inch by 1/8 inch = 1/64 inch (conservative for this back-of-the-envelope calculation), the stress would still be only 1200*64 = 77000 psi, far below the yield strength of typical steels. And it's not being applied perpendicularly to each face, but more in shear, besides. > 4) If there is significant motion of the pulley relative to the crank, the > mating surfaces will wallow out. Which mating surfaces? > We see it often enough with splined drive > axles that are insufficiently torqued. > > Altogether, it doesn't add up. Torsional forces between the pulley and crank > must act unidirectionally on the bolt, with several tons of force being > transferred through both sides of the washer and If the above is supposed to relate to your earlier calculation, then I think there's a conceptual error here. > without damaging the pulley > or crank mating surfaces, with enough movement to materially tighten the > bolt. The theorized ratchet mechanism has to operate on a microscopic basis, > not be damaged in removal, and to allow effortless unthreading when the bolt > is broken loose. It must work over a wide range of lubrication, including a > penetrant oil film or being cleaned with brake cleaner. I'm glad I haven't > been asked to design something like that, particularly if I could just > specify tightening to a different torque in the first place. I have doubts that a cold bolt-pulley-crankshaft assembly would hold up to a hand application of 300 ft-lbs. of tightening torque. 'Cause crude estimators like the one I cite above indicate this would produce in the neighborhood of 300(12)/(.2*.55) = 32700 lbs. of axial load in the bolt, or 32700 / (Pi r^2) = about 137,000 psi of tensile stress in the bolt, which is mighty close to the yield strength (~ 130,000 to 150,000) of many steels. This is too close for engineering comfort. Which is why I am led to believe galling, aggravated by extreme heat cycling and the high loads of that pulley working on an initially pretty tight bolt, plays at least some role and possibly all of it. |
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"Elle" <honda.lioness@nospam.earthlink.net> wrote in message
news:CQbcf.1796$Id6.229@newsread1.news.pas.earthli nk.net... > "Michael Pardee" <michaeltnull@cybertrails.com> wrote >> "karl" <ottokarl@cognisurf.com> wrote >> > http://square.cjb.cc/bolts.htm >> > >> > "Self Tightening Bolts theory. >> > Warning: this page is only a theory, not a fact." >> > >> > >> > That's a good description. >> > >> > Could someone please explain what self-tightening and >> > self-locking bolts are and give examples. The author may >> > have the latter in mind. >> > >> > >> > >> > "Figure 4.1 This picture explains the great inertia and >> > centrifugal force" >> > >> > "When ever there is a difference in inertial force (as >> > pointed out with the arrows) the pulley will move. Not >> > 180-ft-lb torque can hold the pulley still." >> > >> > >> > I wonder what this is about. >> > >> I am unconvinced by this theory. >> >> 1) If microscopic ratchet teeth are created to cause the bolt to >> self-tighten, wouldn't they be destroyed when the god-awful tight bolt is >> broken loose? The bolt at least should be specified as a "use once" item, >> regardless of how the mating threads in the crank fare. >> >> 2) In order to tighten, the bolt will have to move with respect to the >> pulley. That means the washer must have similar ratcheting action, and on > a >> similar microscopic level to allow the ratchet to occur with miniscule >> motion. That means if the washer is less than pristine and is reused the >> bolt won't self-tighten. >> >> 3) The forces are downright outrageous. In round numbers, if the washer >> diameter is 1/2 inch and the bolt thread diameter is 1/4 inch, to tighten >> past the 200 ft-lb mark the bolt head has to experience 5000 pounds force >> from one side to the other, or 10000 pounds force on one side relative to >> the center. The equivalent force on the thread is double that. > > It's the stresses in the bolt, not the forces acting on the side of it, > that > matter. Specifically, torquing down on a bolt is the equivalent of > stretching it until it holds two things together. The torquing causes the > threads to act against each other so as to place the bolt in tension (as > opposed to compression). > > For correlating torque to the axial load it produces, one finds somewhat > crude estimates like that given at the bottom of > http://www.engineersedge.com/torque.htm . But of course, this formula will > require tweaking depending on conditions. E.g. fine thread vs. coarse > thread. > > Anyway, it's really about 200 ft-lbs. divided over the six edges of the > roughly 1.7/2 cm (= about .33 inch = about 0.028 foot) radius bolt head > (for > a 91 Civic, for one), anyway. (This Civic's pulley bolt has a 17 mm head > and > 14 mm nominal diameter.) So something like 200/6/(0.028) = about 1200 > pounds > is applied to each bolt head edge. Key word being "edge." Then one has to > think about what it means to "apply" this force to the whole edge. It's > distributed over the surface of the edge, for one thing. If one took 1200 > lbs. and set it on a bar of steel with a cross-sectional area of about 1/8 > inch by 1/8 inch = 1/64 inch (conservative for this back-of-the-envelope > calculation), the stress would still be only 1200*64 = 77000 psi, far > below > the yield strength of typical steels. And it's not being applied > perpendicularly to each face, but more in shear, besides. > >> 4) If there is significant motion of the pulley relative to the crank, >> the >> mating surfaces will wallow out. > > Which mating surfaces? > >> We see it often enough with splined drive >> axles that are insufficiently torqued. >> >> Altogether, it doesn't add up. Torsional forces between the pulley and > crank >> must act unidirectionally on the bolt, with several tons of force being >> transferred through both sides of the washer and > > If the above is supposed to relate to your earlier calculation, then I > think > there's a conceptual error here. > >> without damaging the pulley >> or crank mating surfaces, with enough movement to materially tighten the >> bolt. The theorized ratchet mechanism has to operate on a microscopic > basis, >> not be damaged in removal, and to allow effortless unthreading when the > bolt >> is broken loose. It must work over a wide range of lubrication, including > a >> penetrant oil film or being cleaned with brake cleaner. I'm glad I >> haven't >> been asked to design something like that, particularly if I could just >> specify tightening to a different torque in the first place. > > I have doubts that a cold bolt-pulley-crankshaft assembly would hold up to > a > hand application of 300 ft-lbs. of tightening torque. 'Cause crude > estimators like the one I cite above indicate this would produce in the > neighborhood of 300(12)/(.2*.55) = 32700 lbs. of axial load in the bolt, > or > 32700 / (Pi r^2) = about 137,000 psi of tensile stress in the bolt, which > is > mighty close to the yield strength (~ 130,000 to 150,000) of many steels. > This is too close for engineering comfort. > > Which is why I am led to believe galling, aggravated by extreme heat > cycling > and the high loads of that pulley working on an initially pretty tight > bolt, > plays at least some role and possibly all of it. > > I think we are talking about two separate things. I'm looking at what is required for force from the theorized pulley movement (in the original link) to tighten the bolt beyond 200 ft-lbs, rather than the tightening being from application of a socket. I don't see how that could be transmitted through the washer, even if pulley/crank movement occurred without wallowing out the mating surface between the crank and pulley. Miscommunication aside, we seem to be on the same page. The bolt isn't turning to tighten itself, it's just sticking. Mike |
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On 2005-11-09, Michael Pardee <michaeltnull@cybertrails.com> wrote:
> Miscommunication aside, we seem to be on the same page..... Maybe so, but the page is too damn long. Trim your posts, ferchrysakes! nb |
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"Michael Pardee" <michaeltnull@cybertrails.com> wrote
> I think we are talking about two separate things. I'm looking at what is > required for force from the theorized pulley movement (in the original link) > to tighten the bolt beyond 200 ft-lbs, rather than the tightening being from > application of a socket. Oh. That is different. Some of my comments still apply, but I think it's too much of a morass to sort out, under the circumstances. > I don't see how that could be transmitted through > the washer, even if pulley/crank movement occurred without wallowing out the > mating surface between the crank and pulley. > > Miscommunication aside, we seem to be on the same page. The bolt isn't > turning to tighten itself, it's just sticking. I don't claim the bolt sticks when it tightens in operation (in theory). I do propose that the crankshaft-pulley assembly moves relative to the bolt at times. No big deal. Some time maybe we'll get some studies of whether the bolt does move relative to the shaft under some operating conditions. Related aside: Does anyone know whether Honda specifies replacing this bolt after so many timing belt changes? Someone here noted that dealer service shops apparently mark the bolt each time it has been removed. There could be a few reasons for this. I'm thinking one of them is to keep a record of how many times the bolt has been loaded yada a certain way. |
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> From: "alt.autos.honda group" <noreply@googlegroups.com>
> Date: Wed, 09 Nov 2005 03:56:52 +0000 > > ================================================== =========================== > TOPIC: Self Tightening Bolts, Self Locking Bolts > http://groups.google.com/group/alt.a...a7a83c13f47050 > ================================================== =========================== > > == 2 of 3 == > Date: Wed 9 Nov 2005 00:58 > From: "Elle" > > "Michael Pardee" <michaeltnull@cybertrails.com> wrote > > "karl" <ottokarl@cognisurf.com> wrote > > > http://square.cjb.cc/bolts.htm > > > snip > > It's the stresses in the bolt, not the forces acting on the > side of it, that matter. Specifically, torquing down on a > bolt is the equivalent of stretching it until it holds two > things together. The torquing causes the threads to act > against each other so as to place the bolt in tension (as > opposed to compression). > > For correlating torque to the axial load it produces, one > finds somewhat crude estimates like that given at the bottom > of http://www.engineersedge.com/torque.htm . But of course, > this formula will require tweaking depending on conditions. > E.g. fine thread vs. coarse thread. | http://www.engineersedge.com/torque.htm | Design Considerations | | The first requirement in determining the amount of torque | to apply is a knowledge of the desired bolt stress. This | stress based on the yield strength of the bolt material. It | is recommended that the induced stress not be allowed to | exceed 80% of the yield strength. In the design of a | fastener application which will be subject to external | loading, whether static or dynamic, it will be necessary to | establish bolt size and allowable stress in accordance with | current engineering practice. | | The mathematical relationship between torque applied and | the resulting tension force in the bolt has been determined | to be as follows: | | T = Torque required (inch pounds) | F = Bolt tension desired (Axial Load) (pounds). | D = Nominal bolt diameter. (major dia.) | EQUATION: T = .2 D F | | This relationship is based on the assumption that regular | series nuts and bolts with rolled threads are used, acting | on surfaces without lubrication. What a rubbish! This formula is simply wrong, dead wrong! The bolt diameter is irrelevant, but the pitch, which is inversely proportional to the Force, is missing from this formula. "The [CORRECT] mathematical relationship between torque applied and the resulting tension force in the bolt," ignoring friction, is: T = Torque required F = Bolt tension or compression desired (Axial Load) P = Pitch T = P*F/2*Pi, or F = T*2*Pi/P It is likely that the constant ".2" in the wrong formula T = .2 D F is chosen such that for common threads reasonable results are obtained, but it is irresponsible not to point out the limitation of this formula. |
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