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#1
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| why ???????????? my schoolteacher and unicersity lecturer both denied it existed. one even claimed that the force which kept a motorcyclist on the wall in the wall of death was the centripetal force. i lost interest in physics after this. shouldnt all physics teachers and professors be dragged along to nasa for compulsory teaching on this subject ? |
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#2
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| [Only registered users see links. ] wrote in message news:<[Only registered users see links. ]>. .. Makes sense to me Sam: Motorcyclists exert - center fleeing - centrifugal force on the walls of death; which in turn keep them on the walls with a restraining centripetal force. They should also learn the difference between concepts, such as weight and mass; and measures of these concepts. |
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#3
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| [Only registered users see links. ] wrote in news:sphtf05oeh2rsjnfbubvo4qbspgqjoqemu@ 4ax.com: Because as defined by physicists, the centrifugal force is in fact a fictitious force. Unfortunately, the popular explanations regarding it generally miss the mark and make for a lot of confusion. That's wrong, but probably not for the reason you think it is. It's momentum that keeps the motorcycle against the wall, not the force exerted by the wall. However, the force exerted by the wall on the motorcycle is, indeed, a centripetal force, since it's directed toward the center of the cage. Why? Whether or not the subject is of interest to you shouldn't depend on other people's knowledge or lack thereof. -- Steve Gray [Only registered users see links. ] |
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#4
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| > not according to nasa it isnt. it all depends on which reference frame you choose. the only real forces are the 4 fundamental forces of nature and all other forces are inertial forces. the centrifugal force is an inertial force. not so. [Only registered users see links. ] Wind the car up, place it inside the vertical, circular track, and let go. The car speeds forward, up the track and around. It keeps looping around the track until the spring is unwound and friction slows it. Eventually, the car will no longer be able to loop to the top of the track and around, and gravity will make it fall down. Why was the car at first, when it went fast, able to loop around the track, but not later after it had slowed? Answer: At first, the car's great speed around the circular track created a lot of centrifugal force. That force pushed it hard against the track, and the downward force of gravity could not pull it off. Only after the car had slowed and the centrifugal force became reduced was gravity able to make it fall. A general note: Centrifugal force is felt whenever you go quickly around a curve -- on a merry-go-round, in a car speeding around a tight curve, or when you swing an object tied to a string in circles overhead. |
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#5
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| [Only registered users see links. ]PAM (Steven Gray) wrote in message news:<Xns952DCC28FBD1sgray2cflrrcom@65.32.1.7>... Cut< Except when you know darn well that your teacher is teaching you wrong: It's obvious that the motorcyclist is exerting a centrifugal force on the wall; just as the clothes in a spin dry washer are exerting a centrifugal force that squeezes the water out of them. |
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#6
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| On 22 Jul 2004 03:58:18 -0700, [Only registered users see links. ] (Donald G. Shead) wrote: it was my school physics teacher who first introduced us to circular motion and we students all argued with him that a centrifugal force existed in the washing machine and on the wall of death. he had been taught - badly - that there was no such thing as centrifugal force and insisted it was centripetal force which kept the clothes on the drum and the cyclist on the wall. you could tell he was unhappy about his argument as it clearly made no sense to him or us. despite what some people say the education system in the UK (Scotland especially ) is very outmoded. it is still stuck in a 19th century model of learning which explains why Scotland has produced no scientific geniuses for almost 100 years when it used to produce them by the truck load. US education seems much more student-centric and more focused on understanding rather than the dry , pedagogic style common in Scottish universities. The NASA article on Centrifugal force is an excellent example of the US style of teaching compared with the Scottish (University of St Andrews Maths site being an honorable exception) |
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#7
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| <[Only registered users see links. ]> wrote in message news:[Only registered users see links. ]... That is correct. In a inertial (non-rotating) reference frame there is no such thing as centrifugal force. In a rotating reference frame it is necessary to introduce two new forces if you want to keep the laws of physics the same as in an inertial frame. The two new forces are the centrifugal force and the coriolis force. It is usually better to do physics in an inertial frame especially when teaching basic physics. In more advanced physics there are cases where a rotating frame is more convenient. The answer depends on which reference frame you use. Your answer is correct if you use a frame rotating with the car. Martin Hogbin |
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#8
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| <[Only registered users see links. ]> wrote in message news:[Only registered users see links. ]... You need to fully understand physics in inertial frames before starting to consider rotating ones. I doubt it. Some things, such as large scale meteorology, are better suited to being explained a rotating frame. Others, such as the example below are much better considered in an inertial frame. A stone is being whirled round on a string. The string is cut and the stone flies off. Explain what is happening in a reference frame rotating with the original motion of the stone. Martin Hogbin |
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#9
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| On Thu, 22 Jul 2004 22:02:53 +0000 (UTC), "Martin Hogbin" <[Only registered users see links. ]> wrote: there are two main horizontal forces at work . a centrifugal force equal to mv^2/ r and a centripetal force provided by the tension in the string. while the stone is attached to the string the two forces are in equillibrium. as the velocity of the stone increases the centrifugal force becomes so great that it passes the tensile breaking point of the string and the string snaps. ie the Tension in the string can only go to a maximum level whereas the centrifugal force is potentially infinite. this is directly analogous to the car going round a bend and the draughts piece on the turntable. the stone then flies off in a radial direction. how is that ? |
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#10
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| On Fri, 23 Jul 2004 06:37:07 +0100, [Only registered users see links. ] wrote: PS this answer is for a stone being whirled in a flat horizontal circle. for a vertical circle the answer is slightly different but the principle remains the same. in the horizointal circle if someone cuts the string there is no longer any Tension in the string to counteract the outward centre-fleeing (centrifugal) force and the stone flies off in a radial direction. |
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