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Centrifugal force

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1161:, the net force acting on them is therefore zero (all forces acting on them cancel each other out). If the car enters a curve that bends to the left, the passenger experiences an apparent force that seems to be pulling them towards the right. This is the fictitious centrifugal force. It is needed within the passengers' local frame of reference to explain their sudden tendency to start accelerating to the right relative to the car—a tendency which they must resist by applying a lefttward force to the car (for instance, a frictional force against the seat) in order to remain in a fixed position inside. Since they push the seat toward the right, Newton's third law says that the seat pushes them towards the left. The centrifugal force must be included in the passenger's reference frame (in which the passenger remains at rest): it counteracts the leftward force applied to the passenger by the seat, and explains why this otherwise unbalanced force does not cause them to accelerate. However, it would be apparent to a stationary observer watching from an overpass above that the frictional force exerted on the passenger by the seat is not being balanced; it constitutes a net force to the left, causing the passenger to accelerate toward the inside of the curve, as they must in order to keep moving with the car rather than proceeding in a straight line as they otherwise would. Thus the "centrifugal force" they feel is the result of a "centrifugal tendency" caused by inertia. Similar effects are encountered in aeroplanes and 2710: 1935: 1250:, the same two real forces act upon the object. However, the object is moving in a circular path as the Earth rotates and therefore experiencing a centripetal acceleration. When considered in an inertial frame (that is to say, one that is not rotating with the Earth), the non-zero acceleration means that force of gravity will not balance with the force from the spring. In order to have a net centripetal force, the magnitude of the restoring force of the spring must be less than the magnitude of force of gravity. This reduced restoring force in the spring is reflected on the scale as less weight — about 0.3% less at the equator than at the poles. In the Earth reference frame (in which the object being weighed is at rest), the object does not appear to be accelerating; however, the two real forces, gravity and the force from the spring, are the same magnitude and do not balance. The centrifugal force must be included to make the sum of the forces be zero to match the apparent lack of acceleration. 2705:{\displaystyle {\begin{aligned}{\boldsymbol {a}}&={\frac {\mathrm {d} ^{2}{\boldsymbol {r}}}{\mathrm {d} t^{2}}}={\frac {\mathrm {d} }{\mathrm {d} t}}{\frac {\mathrm {d} {\boldsymbol {r}}}{\mathrm {d} t}}={\frac {\mathrm {d} }{\mathrm {d} t}}\left(\left+{\boldsymbol {\omega }}\times {\boldsymbol {r}}\ \right)\\&=\left+{\boldsymbol {\omega }}\times \left+{\frac {\mathrm {d} {\boldsymbol {\omega }}}{\mathrm {d} t}}\times {\boldsymbol {r}}+{\boldsymbol {\omega }}\times {\frac {\mathrm {d} {\boldsymbol {r}}}{\mathrm {d} t}}\\&=\left+{\boldsymbol {\omega }}\times \left+{\frac {\mathrm {d} {\boldsymbol {\omega }}}{\mathrm {d} t}}\times {\boldsymbol {r}}+{\boldsymbol {\omega }}\times \left(\left+{\boldsymbol {\omega }}\times {\boldsymbol {r}}\ \right)\\&=\left+{\frac {\mathrm {d} {\boldsymbol {\omega }}}{\mathrm {d} t}}\times {\boldsymbol {r}}+2{\boldsymbol {\omega }}\times \left+{\boldsymbol {\omega }}\times ({\boldsymbol {\omega }}\times {\boldsymbol {r}})\ .\end{aligned}}} 3682: 742: 1143:) is required. These fictitious forces are necessary for the formulation of correct equations of motion in a rotating reference frame and allow Newton's laws to be used in their normal form in such a frame (with one exception: the fictitious forces do not obey Newton's third law: they have no equal and opposite counterparts). Newton's third law requires the counterparts to exist within the same frame of reference, hence centrifugal and centripetal force, which do not, are not action and reaction (as is sometimes erroneously contended). 755: 5475: 3372: 3045: 3360: 1123:" is generally taken to be an inertial frame. Any system can be analyzed in an inertial frame (and so with no centrifugal force). However, it is often more convenient to describe a rotating system by using a rotating frame—the calculations are simpler, and descriptions more intuitive. When this choice is made, fictitious forces, including the centrifugal force, arise. 1193:, in this case provided by the string, must be continuously applied to the stone. As soon as it is removed (for example if the string breaks) the stone moves in a straight line, as viewed from above. In this inertial frame, the concept of centrifugal force is not required as all motion can be properly described using only real forces and Newton's laws of motion. 1222:" at any point on the Earth's surface is actually a combination of gravitational and centrifugal forces. However, the fictitious forces can be of arbitrary size. For example, in an Earth-bound reference system (where the earth is represented as stationary), the fictitious force (the net of Coriolis and centrifugal forces) is enormous and is responsible for the 3609:)} are sometimes called centrifugal forces. In the case of motion in a central potential the Lagrangian centrifugal force has the same form as the fictitious centrifugal force derived in a co-rotating frame. However, the Lagrangian use of "centrifugal force" in other, more general cases has only a limited connection to the Newtonian definition. 1000:, as it might be called, a subject about which I have more to say than I am able to do at present. But, in order that those interested in these things can sooner enjoy these new and not useless speculations, and in order that their publication not be prevented by some accident, I have decided, contrary to my plan, to add this fifth part . 2841:. Therefore, the observer perceives the extra terms as contributions due to fictitious forces. These terms in the apparent acceleration are independent of mass; so it appears that each of these fictitious forces, like gravity, pulls on an object in proportion to its mass. When these forces are added, the equation of motion has the form: 2844: 1126:
In a reference frame rotating about an axis through its origin, all objects, regardless of their state of motion, appear to be under the influence of a radially (from the axis of rotation) outward force that is proportional to their mass, to the distance from the axis of rotation of the frame, and to
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All measurements of position and velocity must be made relative to some frame of reference. For example, an analysis of the motion of an object in an airliner in flight could be made relative to the airliner, to the surface of the Earth, or even to the Sun. A reference frame that is at rest (or one
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was proposed where, instead of absolute rotation, the motion of the distant stars relative to the local inertial frame gives rise through some (hypothetical) physical law to the centrifugal force and other inertia effects. Today's view is based upon the idea of an inertial frame of reference, which
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There is another kind of oscillation in addition to the one we have examined up to this point; namely, a motion in which a suspended weight is moved around through the circumference of a circle. From this we were led to the construction of another clock at about the same time we invented the first
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in the spring, acting upward. Since the object is stationary and not accelerating, there is no net force acting on the object and the force from the spring is equal in magnitude to the force of gravity on the object. In this case, the balance shows the value of the force of gravity on the object.
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In the inertial frame of reference (upper part of the picture), the black ball moves in a straight line. However, the observer (brown dot) who is standing in the rotating/non-inertial frame of reference (lower part of the picture) sees the object as following a curved path due to the Coriolis and
3418:, the balance between containment by gravitational attraction and dispersal by centrifugal force. That the Earth is itself an oblate spheroid, bulging at the equator where the radial distance and hence the centrifugal force is larger, is taken as one of the evidences for its absolute rotation. 1196:
In a frame of reference rotating with the stone around the same axis as the stone, the stone is stationary. However, the force applied by the string is still acting on the stone. If one were to apply Newton's laws in their usual (inertial frame) form, one would conclude that the stone should
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In these scenarios, the effects attributed to centrifugal force are only observed in the local frame (the frame in which the object is stationary) if the object is undergoing absolute rotation relative to an inertial frame. By contrast, in an inertial frame, the observed effects arise as a
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A common experience that gives rise to the idea of a centrifugal force is encountered by passengers riding in a vehicle, such as a car, that is changing direction. If a car is traveling at a constant speed along a straight road, then a passenger inside is not accelerating and, according to
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around its axis. Because the rotation is slow, the fictitious forces it produces are often small, and in everyday situations can generally be neglected. Even in calculations requiring high precision, the centrifugal force is generally not explicitly included, but rather lumped in with the
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From the perspective of the rotating frame, the additional force terms are experienced just like the real external forces and contribute to the apparent acceleration. The additional terms on the force side of the equation can be recognized as, reading from left to right, the
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consequence of the inertia and the known forces without the need to introduce a centrifugal force. Based on this argument, the privileged frame, wherein the laws of physics take on the simplest form, is a stationary frame in which no fictitious forces need to be invoked.
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If a stone is whirled round on a string, in a horizontal plane, the only real force acting on the stone in the horizontal plane is applied by the string (gravity acts vertically). There is a net force on the stone in the horizontal plane which acts toward the center.
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Nevertheless, all of these systems can also be described without requiring the concept of centrifugal force, in terms of motions and forces in a stationary frame, at the cost of taking somewhat more care in the consideration of forces and motions within the system.
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are used in science and industry to separate substances. In the reference frame spinning with the centrifuge, the centrifugal force induces a hydrostatic pressure gradient in fluid-filled tubes oriented perpendicular to the axis of rotation, giving rise to large
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accelerate in the direction of the net applied force—towards the axis of rotation—which it does not do. The centrifugal force and other fictitious forces must be included along with the real forces in order to apply Newton's laws of motion in the rotating frame.
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Within this view of physics, any other phenomenon that is usually attributed to centrifugal force can be used to identify absolute rotation. For example, the oblateness of a sphere of freely flowing material is often explained in terms of centrifugal force. The
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the centrifugal force and all other fictitious forces disappear. Similarly, as the centrifugal force is proportional to the distance from object to the axis of rotation of the frame, the centrifugal force vanishes for objects that lie upon the axis.
3040:{\displaystyle {\boldsymbol {F}}-m{\frac {\mathrm {d} {\boldsymbol {\omega }}}{\mathrm {d} t}}\times {\boldsymbol {r}}-2m{\boldsymbol {\omega }}\times \left-m{\boldsymbol {\omega }}\times ({\boldsymbol {\omega }}\times {\boldsymbol {r}})=m\left\ .} 1808: 3225: 3385:
Three scenarios were suggested by Newton to answer the question of whether the absolute rotation of a local frame can be detected; that is, if an observer can decide whether an observed object is rotating or if the observer is rotating.
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is used in small engine-powered devices such as chain saws, go-karts and model helicopters. It allows the engine to start and idle without driving the device but automatically and smoothly engages the drive as the engine speed rises.
3105: 2784:. An observer unaware of the rotation would expect this to be zero in the absence of outside forces. However, Newton's laws of motion apply only in the inertial frame and describe dynamics in terms of the absolute acceleration 1131:
of the frame. This is the centrifugal force. As humans usually experience centrifugal force from within the rotating reference frame, e.g. on a merry-go-round or vehicle, this is much more well-known than centripetal force.
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argument. According to Newton, in each scenario the centrifugal force would be observed in the object's local frame (the frame where the object is stationary) only if the frame were rotating with respect to absolute space.
2839: 5094:, a kind of "centrifugal force" arises ... We call this force "democratic centrifugal force". Of course, DCF is different from the ordinary centrifugal force, and it arises even in a system of zero angular momentum. 1499: 1860: 1084:
privileges observers for which the laws of physics take on their simplest form, and in particular, frames that do not use centrifugal forces in their equations of motion in order to describe motions correctly.
1656: 96: 1930: 1721: 3175: 1940: 4308: 1262:, so an object at the poles is slightly closer to the center of the Earth than one at the equator; this effect combines with the centrifugal force to produce the observed weight difference. 27: 4970: 3526:
to refer to the particular fictitious force that arises in rotating frames, there are a few limited instances in the literature of the term applied to other distinct physical concepts.
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Noninertial forces, like centrifugal and Coriolis forces, can be eliminated by jumping into a reference frame that moves with constant velocity, the frame that Newton called inertial.
3314: 3265: 4911: 3316:, and unlike the Coriolis force in particular, it is independent of the motion of the particle in the rotating frame. As expected, for a non-rotating inertial frame of reference 5000: 4866: 120: 877: 5092: 3227:, respectively. Unlike the other two fictitious forces, the centrifugal force always points radially outward from the axis of rotation of the rotating frame, with magnitude 3582: 3292: 3180: 1616: 3494:
which push low-density particles inward. Elements or particles denser than the fluid move outward under the influence of the centrifugal force. This is effectively
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about their center of mass. The tension in the string will be proportional to the centrifugal force on each sphere as it rotates around the common center of mass.
3056: 5250: 3659:, that is, a force that is centrifugally directed, which is a reactive force equal and opposite to the centripetal force that is curving the path of the mass. 1238:
at one of the Earth's poles, there are two forces acting on the object: the Earth's gravity, which acts in a downward direction, and the equal and opposite
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In fact, the observed weight difference is more — about 0.53%. Earth's gravity is a bit stronger at the poles than at the equator, because the Earth is
5159:"The intrinsic derivative and centrifugal forces in general relativity: II. Applications to circular orbits in some stationary axisymmetric spacetimes" 2787: 3375:
When analysed in a rotating reference frame of the planet, centrifugal force causes rotating planets to assume the shape of an oblate spheroid.
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The operations of numerous common rotating mechanical systems are most easily conceptualized in terms of centrifugal force. For example:
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one. I originally intended to publish here a lengthy description of these clocks, along with matters pertaining to circular motion and
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of time—such as the velocity and acceleration vectors of an object—will differ from its time derivatives in the stationary frame. If
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The concept of the reactive centrifugal force is sometimes used in mechanics and engineering. It is sometimes referred to as just
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Geometrical Structures Of Phase Space In Multi-dimensional Chaos: Applications to chemical reaction dynamics in complex systems
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the other body that provides the centripetal force and its direction is from that other body toward the body in curved motion.
3509:'s spin forces riders against a wall and allows riders to be elevated above the machine's floor in defiance of Earth's gravity. 1591:{\displaystyle {\frac {\mathrm {d} {\boldsymbol {P}}}{\mathrm {d} t}}=\left+{\boldsymbol {\omega }}\times {\boldsymbol {P}}\ ,} 52: 3637: 3483:
are production methods that use centrifugal force to disperse liquid metal or plastic throughout the negative space of a mold.
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Christiaan Huygens' the pendulum clock, or, Geometrical demonstrations concerning the motion of pendula as applied to clocks
3827: 3113: 1865: 5366: 3438:, as the engine changes speed. In the reference frame of the spinning masses, centrifugal force causes the radial movement. 3636:
is provided by a centripetal force, which is exerted on the body in curved motion by some other body. In accordance with
1283: 449: 4471: 3907:(Andrew Motte translation of 1729, revised by Florian Cajori ed.). University of California Press. pp. 10–12. 5479: 3447: 5291: 5225: 3939: 3912: 3821: 3394:. The shape of the surface becomes concave to balance the centrifugal force against the other forces upon the liquid. 843: 779: 3480: 4920: 3681: 741: 3319: 115: 4796: 1628:
in the stationary frame is the sum of its apparent rate of change in the rotating frame and a rate of rotation
370: 110: 4820: 4383: 1185:, were it not for this net force acting on the stone, the stone would travel in a straight line, according to 3297: 3230: 4814: 3695: 3595: 1293: 815: 772: 759: 520: 443: 365: 208: 4871: 4408: 1226:
orbiting around the Earth. This is due to the large mass and velocity of the Sun (relative to the Earth).
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or a much more extensive list of variables. Within this formulation the motion is described in terms of
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A Catalogue of the Manuscripts of Christiaan Huygens including a concordance with his Oeuvres Complètes
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By applying the transformation above from the stationary to the rotating frame three times (twice to
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about detection of absolute motion. Newton suggested two arguments to answer the question of whether
1042: 413: 5068: 4338: 5109:"The intrinsic derivative and centrifugal forces in general relativity: I. Theoretical foundations" 4571: 3633: 3552: 3495: 1803:{\displaystyle {\boldsymbol {a}}={\frac {\mathrm {d} ^{2}{\boldsymbol {r}}}{\mathrm {d} t^{2}}}\ ,} 1273: 1108: 1012:
and replied "I pray you return my humble thanks I am glad we can expect another discourse of the
983: 910: 689: 533: 810:(also called an "inertial" or "pseudo" force) that appears to act on all objects when viewed in a 3539: 3220:{\displaystyle -m{\boldsymbol {\omega }}\times ({\boldsymbol {\omega }}\times {\boldsymbol {r}})} 639: 403: 5049:. In Mikito Toda; Tamiki Komatsuzaki; Stuart A. Rice; Tetsuro Konishi; R. Stephen Berry (eds.). 3856: 3270: 679: 4659: 4192: 684: 501: 5457: 5422: 5405: 5316: 5281: 5019: 4682: 4599: 4538: 4502: 4259: 3963: 5495: 5215: 5046: 4769: 4626: 4444: 4232: 3929: 3902: 3705: 3415: 3359: 1601: 1092: 694: 669: 355: 173: 4708: 4092: 3434:
regulates the speed of an engine by using spinning masses that move radially, adjusting the
5378: 5331: 5180: 5130: 4351: 4209: 4127: 4049: 3535: 3431: 3100:{\displaystyle -m\mathrm {d} {\boldsymbol {\omega }}/\mathrm {d} t\times {\boldsymbol {r}}} 2722: 1619: 988: 890: 714: 674: 582: 578: 570: 560: 350: 343: 99: 4261:
Introduction to Mechanics and Symmetry: A Basic Exposition of Classical Mechanical Systems
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Restuccia, S.; Toroš, M.; Gibson, G. M.; Ulbricht, H.; Faccio, D.; Padgett, M. J. (2019).
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equal to the rate of rotation and is directed along the axis of rotation according to the
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is the position vector of the particle (not to be confused with radius, as used above.)
1041:("centrifugal force"). Around this time, the concept is also further evolved by Newton, 5510: 5347: 5196: 5170: 5146: 5120: 4653: 4326: 4285: 4143: 4073: 4039: 3991: 3850: 3641: 3640:, the body in curved motion exerts an equal and opposite force on the other body. This 3618: 3586: 3462: 3442: 1296:
that is rotating relative to an inertial reference frame denoted the stationary frame.
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In the late 18th century, the modern conception of the centrifugal force evolved as a "
1017: 949: 894: 619: 360: 235: 203: 163: 4675: 4170: 3598:. Among the generalized forces, those involving the square of the time derivatives {(d 960: 5515: 5450: 5428: 5351: 5343: 5297: 5287: 5231: 5221: 5054: 5025: 4868:. These are further classified into two types. Terms involving a product of the type 4802: 4775: 4748: 4714: 4686: 4632: 4605: 4575: 4544: 4508: 4481: 4450: 4414: 4265: 4238: 4228: 4147: 4139: 4098: 4077: 4065: 3979: 3969: 3945: 3935: 3908: 3860: 3817: 3770: 3380: 1190: 1064: 923: 629: 586: 538: 479: 255: 245: 138: 20: 5270:. Michigan State University, "Acceleration and force in circular motion", §5b, p. 7. 5200: 5150: 5386: 5339: 5188: 5138: 4135: 4061: 4057: 3715: 3591: 3398: 1466: 1279: 1219: 1128: 1072: 1053: 886: 834: 803: 724: 704: 649: 644: 590: 565: 420: 278: 223: 198: 5264: 4736: 4543:(Reprint of Fourth Edition of 1970 ed.). Dover Publications. Chapter 4, §5. 4358: 4027: 3811: 3629: 3411: 3391: 3367:
liquids rotating around a vertical axis is an upward-opening circular paraboloid.
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As is evident from the first terms ..., which are proportional to the square of
4794: 3455: 954: 5505: 3687: 3502: 3108: 1235: 1162: 1136: 746: 654: 555: 272: 5192: 5142: 2834:{\displaystyle {\frac {\mathrm {d} ^{2}{\boldsymbol {r}}}{\mathrm {d} t^{2}}}} 1304:
In a rotating frame of reference, the time derivatives of any vector function
1139:. If the rate of rotation of the frame changes, a third fictitious force (the 5489: 4118:
Kobayashi, Yukio (2008). "Remarks on viewing situation in a rotating frame".
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centrifugal force although this usage is deprecated in elementary mechanics.
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Motion relative to a rotating frame results in another fictitious force: the
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Around 1914, the analogy between centrifugal force (sometimes used to create
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as generated by centrifugal force as opposed to being generated by gravity.
3476: 1736: 1046: 1005: 906: 699: 624: 313: 193: 922:, a real frame-independent Newtonian force that exists as a reaction to a 4169:. Goddard Space Flight Center Space Physics Data Facility. Archived from 3364: 3051: 1140: 1120: 26: 5175: 5125: 3632:, is accelerating toward a center at any particular point in time. This 1739:(that is, acceleration in an inertial frame) of the particle, given by: 5156: 5106: 4413:(Reprint of Second Edition of 1942 ed.). Read Books. p. 347. 4210:
The Feynman Lectures on Physics Vol. I Ch. 12: Characteristics of Force
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that moves with no rotation and at constant velocity) relative to the "
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is the vector sum of the physical forces applied to the particle and
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with respect to the stationary frame is related to by the equation:
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An elementary treatise on analytic mechanics: with numerous examples
5158: 5108: 4713:(Reprint of 1970 University of Toronto ed.). Dover. p. 1. 4223: 881:
This fictitious force is often applied to rotating devices, such as
4044: 3435: 1855:{\textstyle {\frac {\mathrm {d} {\boldsymbol {r}}}{\mathrm {d} t}}} 425: 308: 283: 4771:
Cartesian Impedance Control of Redundant and Flexible-Joint Robots
4624: 4097:. Sausalito CA: University Science Books. Chapter 9, pp. 344 ff. 3458:
used in many automobile seat belts operate on the same principle.
1247: 1166: 398: 251: 168: 5286:(2nd ed.). New Delhi: Prentice-Hall of India. p. 121. 4257: 3927: 1932:), the absolute acceleration of the particle can be written as: 1165:
where the magnitude of the apparent force is often reported in "
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from the axis of rotation of a frame of reference rotating with
5474: 3968:. Ingrid V. Eriksson. New York: Nova Science Publishers. 2008. 3931:
Mach's principle : from Newton's bucket to quantum gravity
3885:(in French). Vol. 7. The Hague: M. Nijhoff. 1897. p.  1651:{\displaystyle {\boldsymbol {\omega }}\times {\boldsymbol {P}}} 457: 303: 213: 4449:(Third ed.). Oxford: Butterworth-Heinemann. p. 128. 4406: 3522:
While the majority of the scientific literature uses the term
1111:. It does not exist when a system is described relative to an 4795:
Shuzhi S. Ge; Tong Heng Lee; Christopher John Harris (1998).
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attributable to the motion of the rotating frame. The vector
1206: 293: 288: 230: 5047:"Effects of an intrinsic metric of molecular internal space" 4025: 5220:. Princeton, N.J.: Princeton University Press. p. 47. 4597: 4469: 4013:
Mechanics, mechanical waves, kinetic theory, thermodynamics
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Confusingly, the term has sometimes also been used for the
823: 298: 261: 4300: 3473:-level gravity on mice with gravity simulated in this way. 3465:, as in proposed designs for rotating space stations. The 1209:
constitutes a rotating reference frame because it rotates
1189:. In order to keep the stone moving in a circular path, a 5253:. Vol. 25. American Journal of Physics. p. 325. 5017: 3549:}, which can be as simple as the usual polar coordinates 3294:
is the component of the position vector perpendicular to
1223: 91:{\displaystyle {\textbf {F}}={\frac {d\mathbf {p} }{dt}}} 3538:. Lagrangian mechanics formulates mechanics in terms of 4798:
Adaptive Neural Network Control of Robotic Manipulators
1925:{\textstyle {\frac {\mathrm {d} }{\mathrm {d} t}}\left} 1716:{\displaystyle {\boldsymbol {F}}=m{\boldsymbol {a}}\ ,} 1299: 1059:
Centrifugal force has also played a role in debates in
5410:(25th ed.). D. Van Nostrand Company. p. 357. 3170:{\displaystyle -2m{\boldsymbol {\omega }}\times \left} 1868: 1825: 1414:
with respect to the rotating frame is, by definition,
5071: 4986: 4923: 4874: 4852: 4823: 4743:(2 ed.). Cambridge University Press. p. 90 3555: 3322: 3300: 3273: 3233: 3183: 3116: 3059: 2847: 2790: 2725: 1938: 1745: 1690: 1634: 1604: 1502: 846: 55: 5403: 5364: 5157:
Donato Bini; Paolo Carini; Robert T Jantzen (1997).
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Donato Bini; Paolo Carini; Robert T Jantzen (1997).
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directed along the axes of the rotating frame (i.e.
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Centrifugal force is an outward force apparent in a
4737:"Generalized coordinates and kinematic constraints" 2719:The apparent acceleration in the rotating frame is 1230:
Weight of an object at the poles and on the equator
5449: 5213: 5086: 5044: 4994: 4964: 4905: 4860: 4838: 4733:For a description of generalized coordinates, see 4674: 4090: 3576: 3342: 3308: 3286: 3259: 3219: 3169: 3099: 3039: 2833: 2776: 2704: 1924: 1854: 1802: 1715: 1650: 1610: 1590: 871: 90: 5424:Robotics: a reference guide to the new technology 4706: 4536: 4382:. Arlington, Texas: S.A.W.E., Inc. Archived from 3928:Julian B. Barbour; Herbert Pfister, eds. (1995). 5487: 5420: 5251:"Centrifugal Forces and Newton's Laws of Motion" 4734: 4567:Contemporary Physics and the Limits of Knowledge 4500: 3655:This reaction force is sometimes described as a 3505:make use of centrifugal forces. For instance, a 1151: 4234:Theoretical Mechanics of Particles and Continua 4028:"Photon Bunching in a Rotating Reference Frame" 4011:Richard T. Weidner and Robert L. Sells (1973). 5248: 4237:. Courier Dover Publications. pp. 38–39. 4160: 1680:Newton's law of motion for a particle of mass 5447: 4767: 4651: 4625:I. Bernard Cohen; George Edwin Smith (2002). 4307:Knight, Judson (2016). Schlager, Neil (ed.). 3855:. Ames: Iowa State University Press. p.  1016:, which speculation may prove of good use in 936:History of centrifugal and centripetal forces 780: 4965:{\displaystyle {\dot {q}}_{i}{\dot {q}}_{j}} 4917:while those involving a product of the type 4563: 4504:A universe of atoms, an atom in the universe 3904:Philosophiae naturalis principia mathematica 3900: 5265:"Acceleration and force in circular motion" 4604:. Cambridge University Press. p. 324. 4258:Jerrold E. Marsden; Tudor S. Ratiu (1999). 4015:(2 ed.). Allyn and Bacon. p. 123. 3628:. A body undergoing curved motion, such as 3617:In another instance the term refers to the 3461:Centrifugal forces can be used to generate 3343:{\displaystyle ({\boldsymbol {\omega }}=0)} 1218:: the strength and direction of the local " 4631:. Cambridge University Press. p. 43. 3529: 787: 773: 5174: 5163:International Journal of Modern Physics D 5124: 5113:International Journal of Modern Physics D 4530: 4494: 4436: 4407:John L. Synge; Byron A. Griffith (2007). 4361:, Cornell University, retrieved June 2007 4288:. Encyclopædia Britannica. 17 August 2016 4219: 4217: 4117: 4043: 3848: 3517: 952:' notes and letters. Note, that in Latin 31:centrifugal forces present in this frame. 5099: 4839:{\displaystyle {\boldsymbol {\dot {q}}}} 4727: 3803: 3761: 3759: 3370: 3358: 1622:. In other words, the rate of change of 814:. It is directed radially away from the 25: 5279: 5257: 5011: 4988: 4854: 4827: 4710:The variational principles of mechanics 4699: 4540:The Variational Principles of Mechanics 4370: 4364: 4251: 4084: 3956: 3327: 3309:{\displaystyle {\boldsymbol {\omega }}} 3302: 3210: 3202: 3191: 3145: 3127: 3093: 3072: 3003: 2970: 2962: 2951: 2923: 2903: 2889: 2868: 2849: 2807: 2746: 2685: 2677: 2666: 2641: 2621: 2610: 2589: 2549: 2507: 2499: 2474: 2449: 2441: 2420: 2387: 2367: 2335: 2288: 2272: 2264: 2243: 2210: 2190: 2158: 2116: 2108: 2083: 2026: 1971: 1944: 1901: 1835: 1770: 1747: 1703: 1692: 1644: 1636: 1578: 1570: 1545: 1512: 1246:When the same object is weighed on the 5488: 5456:. Princeton University Press. p.  5441: 5414: 5397: 5214:Mook, Delo E.; Thomas Vargish (1987). 4681:. Greenwood Publishing Group. p.  4598:Louis N. Hand; Janet D. Finch (1998). 4470:Louis N. Hand; Janet D. Finch (1998). 4463: 4306: 4214: 3921: 3882:Œuvres complètes de Christiaan Huygens 3612: 3260:{\displaystyle m\omega ^{2}r_{\perp }} 1406:), then the first time derivative of 1234:If an object is weighed with a simple 1091:) and gravitational forces led to the 913:such as a rotating coordinate system. 5314: 5308: 5242: 4846:where the coefficients may depend on 4705:For an introduction, see for example 4672: 4557: 4507:(2 ed.). Springer. p. 249. 4400: 3965:Science education in the 21st century 3893: 3809: 3765: 3756: 3701:Centrifugal mechanism of acceleration 974:means "fleeing from the center" in a 948:("centrifugal force") is attested in 818:. The magnitude of centrifugal force 469:Newton's law of universal gravitation 5207: 5038: 5018:R. K. Mittal; I. J. Nagrath (2003). 4906:{\displaystyle {{\dot {q}}_{i}}^{2}} 4801:. World Scientific. pp. 47–48. 3771:"Christiaan Huygens' Great Treasure" 3397:The tension in a string joining two 3354: 1300:Time derivatives in a rotating frame 1172: 4761: 3899:An English translation is found at 1292:is regarded as a special case of a 1284:Mechanics of planar particle motion 1056:" arising in a rotating reference. 987:, Huygens writes (as translated by 970:) means "fleeing, avoiding". Thus, 450:Mechanics of planar particle motion 58: 13: 4788: 4658:. Harper & Brothers. pp.  4278: 3934:. Boston: Birkhäuser. p. 69. 3830:from the original on 16 March 2020 3791:from the original on 13 April 2018 3469:would have studied the effects of 3390:The shape of the surface of water 3155: 3140: 3082: 3067: 3010: 2992: 2930: 2918: 2875: 2863: 2814: 2796: 2753: 2735: 2648: 2636: 2596: 2584: 2556: 2538: 2481: 2469: 2427: 2415: 2394: 2382: 2342: 2324: 2295: 2283: 2250: 2238: 2217: 2205: 2165: 2147: 2090: 2078: 2055: 2049: 2033: 2021: 2007: 2001: 1978: 1960: 1908: 1896: 1878: 1872: 1842: 1830: 1777: 1759: 1552: 1540: 1519: 1507: 1211:once every 23 hours and 56 minutes 14: 5527: 5467: 5024:. Tata McGraw-Hill. p. 202. 4995:{\displaystyle {\boldsymbol {q}}} 4980:. The third type is functions of 4861:{\displaystyle {\boldsymbol {q}}} 4628:The Cambridge companion to Newton 4163:"Frames of Reference: The Basics" 3534:One of these instances occurs in 1288:For the following formalism, the 5473: 5427:. Greenwood Press. p. 267. 5317:"Introducing motion in a circle" 4830: 3680: 754: 753: 740: 73: 5358: 5273: 4666: 4645: 4618: 4591: 4521: 4443:LD Landau; LM Lifshitz (1976). 4427: 4345: 4203: 4185: 4154: 4111: 4019: 3421: 1675: 1102: 872:{\displaystyle F=m\omega ^{2}r} 5452:Physics for the Inquiring Mind 5367:"Physics, the pioneer science" 5315:Roche, John (September 2001). 5087:{\displaystyle {\dot {\phi }}} 4815:Euler–Lagrange equations 4313:. Thomson Learning. p. 47 4062:10.1103/physrevlett.123.110401 4004: 3873: 3849:Blackwell, Richard J. (1986). 3842: 3733: 3596:Euler–Lagrange equations 3571: 3556: 3337: 3323: 3214: 3198: 2974: 2958: 2689: 2673: 1067:can be detected: the rotating 909:, when they are analyzed in a 1: 5404:Edward Albert Bowser (1920). 5365:Lloyd William Taylor (1959). 5045:T Yanao; K Takatsuka (2005). 4741:Dynamics of Multibody Systems 4373:"Precise Measurement of Mass" 3810:Yoder, Joella (17 May 2013). 3750: 3657:centrifugal inertial reaction 3577:{\displaystyle (r,\ \theta )} 3448:Inertial drum brake ascenders 1342:with respect to unit vectors 1267: 1159:Newton's second law of motion 1152:Vehicle driving round a curve 376:Koopman–von Neumann mechanics 4167:From Stargazers to Starships 3696:Balancing of rotating masses 3638:Newton's third law of motion 3177:, and the centrifugal force 1294:non-inertial reference frame 1187:Newton's first law of motion 911:non–inertial reference frame 444:Non-inertial reference frame 7: 5371:American Journal of Physics 4120:European Journal of Physics 4091:John Robert Taylor (2004). 3673: 3624:to a centripetal force, or 1684:written in vector form is: 1290:rotating frame of reference 1183:inertial frame of reference 1146: 1113:inertial frame of reference 812:rotating frame of reference 371:Appell's equation of motion 241:Inertial frame of reference 10: 5532: 5344:10.1088/0031-9120/36/5/305 4707:Cornelius Lanczos (1986). 4537:Cornelius Lanczos (1986). 4478:Cambridge University Press 4352:"Curious About Astronomy?" 4140:10.1088/0143-0807/29/3/019 3648:the body in curved motion 3626:reactive centrifugal force 3414:shape reflects, following 3378: 3287:{\displaystyle r_{\perp }} 1277: 1271: 1037:, Newton further develops 1008:received Huygens work via 933: 929: 919:reactive centrifugal force 18: 5421:Joseph A. Angelo (2007). 5193:10.1142/S021827189700011X 5155:. The companion paper is 5143:10.1142/S021827189700011X 4735:Ahmed A. Shabana (2003). 4501:Mark P Silverman (2002). 4371:Boynton, Richard (2001). 4357:January 17, 2015, at the 4264:. Springer. p. 251. 3467:Mars Gravity Biosatellite 1469:of the rotating frame is 1043:Gottfried Wilhelm Leibniz 5165:(Submitted manuscript). 5115:(Submitted manuscript). 4774:. Springer. p. 23. 4673:Myers, Rusty L. (2006). 4572:Rutgers University Press 3726: 3634:centripetal acceleration 2714: 1274:Rotating reference frame 1200: 1109:rotating reference frame 984:Horologium Oscillatorium 534:Rotating reference frame 366:Hamilton–Jacobi equation 19:Not to be confused with 5280:Mohanty, A. K. (1994). 5263:Signell, Peter (2002). 5249:G. David Scott (1957). 4410:Principles of Mechanics 4197:Encyclopædia Britannica 4161:David P. Stern (2006). 4032:Physical Review Letters 3540:generalized coordinates 3530:In Lagrangian mechanics 1611:{\displaystyle \times } 475:Newton's laws of motion 335:Newton's laws of motion 5448:Eric M Rogers (1960). 5088: 4996: 4966: 4907: 4862: 4840: 4768:Christian Ott (2008). 4652:Simon Newcomb (1878). 4527:Taylor (2005). p. 329. 4433:Taylor (2005). p. 342. 3996:: CS1 maint: others ( 3578: 3518:Other uses of the term 3376: 3368: 3344: 3310: 3288: 3261: 3221: 3171: 3101: 3041: 2835: 2778: 2706: 1926: 1856: 1804: 1717: 1652: 1612: 1592: 1334:are the components of 1002: 965: 959: 953: 873: 502:Simple harmonic motion 415:Euler's laws of motion 209:D'Alembert's principle 92: 32: 16:Type of inertial force 5089: 5053:. Wiley. p. 98. 4997: 4967: 4908: 4863: 4841: 4677:The basics of physics 4564:Morton Tavel (2002). 3901:Isaac Newton (1934). 3706:Equivalence principle 3579: 3496:Archimedes' principle 3374: 3363:The interface of two 3362: 3345: 3311: 3289: 3262: 3222: 3172: 3102: 3042: 2836: 2779: 2777:{\displaystyle \left} 2707: 1927: 1857: 1805: 1718: 1653: 1613: 1593: 1093:equivalence principle 993: 891:centrifugal governors 874: 356:Hamiltonian mechanics 174:Statistical mechanics 93: 29: 5482:at Wikimedia Commons 5069: 5021:Robotics and Control 5004:gravitational forces 5002:only and are called 4984: 4921: 4872: 4850: 4821: 4601:Analytical Mechanics 4473:Analytical Mechanics 3590:, using in place of 3553: 3536:Lagrangian mechanics 3432:centrifugal governor 3392:rotating in a bucket 3320: 3298: 3271: 3231: 3181: 3114: 3057: 2845: 2788: 2723: 1936: 1866: 1823: 1743: 1688: 1632: 1620:vector cross product 1602: 1500: 1475:then the derivative 1260:not a perfect sphere 989:Richard J. Blackwell 899:centrifugal railways 895:centrifugal clutches 844: 579:Angular acceleration 571:Rotational frequency 351:Lagrangian mechanics 344:Analytical mechanics 100:Second law of motion 53: 5383:1961AmJPh..29..563T 5336:2001PhyEd..36..399R 5185:1997IJMPD...6..143B 5135:1997IJMPD...6..143B 4380:Sawe Paper No. 3147 4286:"Centrifugal force" 4225:Alexander L. Fetter 4132:2008EJPh...29..599K 4094:Classical Mechanics 4054:2019PhRvL.123k0401R 3613:As a reactive force 3481:centrifugal casting 1465:. If the absolute 1216:gravitational force 1061:classical mechanics 976:literal translation 958:means "center" and 808:Newtonian mechanics 431:Harmonic oscillator 409:Equations of motion 44:Classical mechanics 38:Part of a series on 5084: 4992: 4962: 4915:centrifugal forces 4903: 4858: 4836: 3587:generalized forces 3574: 3463:artificial gravity 3443:centrifugal clutch 3416:Clairaut's theorem 3377: 3369: 3340: 3306: 3284: 3257: 3217: 3167: 3097: 3037: 2831: 2774: 2702: 2700: 1922: 1852: 1800: 1713: 1648: 1608: 1588: 1127:the square of the 1097:general relativity 1089:artificial gravity 1018:natural philosophy 950:Christiaan Huygens 869: 747:Physics portal 361:Routhian mechanics 236:Frame of reference 88: 33: 5501:Fictitious forces 5480:Centrifugal force 5478:Media related to 5434:978-1-57356-337-6 5391:10.1119/1.1937847 5324:Physics Education 5217:Inside relativity 5081: 5060:978-0-471-71157-5 5031:978-0-07-048293-7 4953: 4934: 4887: 4833: 4808:978-981-02-3452-2 4781:978-3-540-69253-9 4754:978-0-521-54411-5 4720:978-0-486-65067-8 4692:978-0-313-32857-2 4655:Popular astronomy 4638:978-0-521-65696-2 4611:978-0-521-57572-0 4581:978-0-8135-3077-2 4550:978-0-486-65067-8 4514:978-0-387-95437-0 4487:978-0-521-57572-0 4456:978-0-7506-2896-9 4420:978-1-4067-4670-9 4310:Centripetal Force 4271:978-0-387-98643-2 4244:978-0-486-43261-8 4229:John Dirk Walecka 4199:. April 30, 2015. 4104:978-1-891389-22-1 3975:978-1-60021-951-1 3866:978-0-8138-0933-5 3664:centrifugal force 3644:force is exerted 3567: 3524:centrifugal force 3381:Absolute rotation 3355:Absolute rotation 3033: 3025: 2938: 2883: 2829: 2768: 2694: 2656: 2604: 2571: 2513: 2489: 2435: 2402: 2357: 2303: 2258: 2225: 2180: 2122: 2098: 2063: 2041: 2015: 1993: 1916: 1886: 1850: 1796: 1792: 1709: 1584: 1560: 1527: 1264: 1191:centripetal force 1173:Stone on a string 1065:absolute rotation 998:centrifugal force 924:centripetal force 887:centrifugal pumps 800:Centrifugal force 797: 796: 544:Centrifugal force 539:Centripetal force 495:Euler's equations 480:Relative velocity 256:Moment of inertia 86: 60: 21:Centripetal force 5523: 5477: 5462: 5461: 5455: 5445: 5439: 5438: 5418: 5412: 5411: 5401: 5395: 5394: 5362: 5356: 5355: 5321: 5312: 5306: 5305: 5277: 5271: 5261: 5255: 5254: 5246: 5240: 5239: 5211: 5205: 5204: 5178: 5154: 5128: 5103: 5097: 5096: 5093: 5091: 5090: 5085: 5083: 5082: 5074: 5042: 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3807: 3801: 3800: 3798: 3796: 3790: 3775: 3763: 3744: 3737: 3716:Lagrangian point 3690: 3685: 3684: 3583: 3581: 3580: 3575: 3565: 3399:spheres rotating 3349: 3347: 3346: 3341: 3330: 3315: 3313: 3312: 3307: 3305: 3293: 3291: 3290: 3285: 3283: 3282: 3266: 3264: 3263: 3258: 3256: 3255: 3246: 3245: 3226: 3224: 3223: 3218: 3213: 3205: 3194: 3176: 3174: 3173: 3168: 3166: 3162: 3158: 3153: 3148: 3143: 3130: 3106: 3104: 3103: 3098: 3096: 3085: 3080: 3075: 3070: 3046: 3044: 3043: 3038: 3031: 3030: 3026: 3024: 3023: 3022: 3013: 3007: 3006: 3001: 3000: 2995: 2988: 2973: 2965: 2954: 2943: 2939: 2937: 2933: 2927: 2926: 2921: 2915: 2906: 2892: 2884: 2882: 2878: 2872: 2871: 2866: 2860: 2852: 2840: 2838: 2837: 2832: 2830: 2828: 2827: 2826: 2817: 2811: 2810: 2805: 2804: 2799: 2792: 2783: 2781: 2780: 2775: 2773: 2769: 2767: 2766: 2765: 2756: 2750: 2749: 2744: 2743: 2738: 2731: 2711: 2709: 2708: 2703: 2701: 2692: 2688: 2680: 2669: 2661: 2657: 2655: 2651: 2645: 2644: 2639: 2633: 2624: 2613: 2605: 2603: 2599: 2593: 2592: 2587: 2581: 2576: 2572: 2570: 2569: 2568: 2559: 2553: 2552: 2547: 2546: 2541: 2534: 2522: 2518: 2514: 2511: 2510: 2502: 2494: 2490: 2488: 2484: 2478: 2477: 2472: 2466: 2452: 2444: 2436: 2434: 2430: 2424: 2423: 2418: 2412: 2407: 2403: 2401: 2397: 2391: 2390: 2385: 2379: 2370: 2362: 2358: 2356: 2355: 2354: 2345: 2339: 2338: 2333: 2332: 2327: 2320: 2308: 2304: 2302: 2298: 2292: 2291: 2286: 2280: 2275: 2267: 2259: 2257: 2253: 2247: 2246: 2241: 2235: 2230: 2226: 2224: 2220: 2214: 2213: 2208: 2202: 2193: 2185: 2181: 2179: 2178: 2177: 2168: 2162: 2161: 2156: 2155: 2150: 2143: 2131: 2127: 2123: 2120: 2119: 2111: 2103: 2099: 2097: 2093: 2087: 2086: 2081: 2075: 2064: 2062: 2058: 2052: 2047: 2042: 2040: 2036: 2030: 2029: 2024: 2018: 2016: 2014: 2010: 2004: 1999: 1994: 1992: 1991: 1990: 1981: 1975: 1974: 1969: 1968: 1963: 1956: 1947: 1931: 1929: 1928: 1923: 1921: 1917: 1915: 1911: 1905: 1904: 1899: 1893: 1887: 1885: 1881: 1875: 1870: 1861: 1859: 1858: 1853: 1851: 1849: 1845: 1839: 1838: 1833: 1827: 1815: 1809: 1807: 1806: 1801: 1794: 1793: 1791: 1790: 1789: 1780: 1774: 1773: 1768: 1767: 1762: 1755: 1750: 1735:is the absolute 1734: 1728: 1722: 1720: 1719: 1714: 1707: 1706: 1695: 1683: 1667: 1663: 1657: 1655: 1654: 1649: 1647: 1639: 1627: 1617: 1615: 1614: 1609: 1597: 1595: 1594: 1589: 1582: 1581: 1573: 1565: 1561: 1559: 1555: 1549: 1548: 1543: 1537: 1528: 1526: 1522: 1516: 1515: 1510: 1504: 1495: 1487: 1474: 1467:angular velocity 1464: 1413: 1405: 1361: 1341: 1333: 1311: 1280:Fictitious force 1253: 1129:angular velocity 1081:Mach's principle 1073:rotating spheres 1054:fictitious force 903:planetary orbits 878: 876: 875: 870: 865: 864: 839: 835:angular velocity 829:at the distance 822:on an object of 816:axis of rotation 804:fictitious force 789: 782: 775: 762: 757: 756: 749: 745: 744: 650:Johann Bernoulli 645:Daniel Bernoulli 566:Tangential speed 470: 446: 421:Fictitious force 416: 268:Mechanical power 258: 199:Angular momentum 97: 95: 94: 89: 87: 85: 77: 76: 67: 62: 61: 35: 34: 5531: 5530: 5526: 5525: 5524: 5522: 5521: 5520: 5486: 5485: 5470: 5465: 5446: 5442: 5435: 5419: 5415: 5402: 5398: 5363: 5359: 5319: 5313: 5309: 5294: 5283:Fluid mechanics 5278: 5274: 5262: 5258: 5247: 5243: 5228: 5212: 5208: 5176:gr-qc/0106014v1 5126:gr-qc/0106014v1 5104: 5100: 5073: 5072: 5070: 5067: 5066: 5061: 5043: 5039: 5032: 5016: 5012: 4987: 4985: 4982: 4981: 4978:Coriolis forces 4956: 4945: 4944: 4943: 4937: 4926: 4925: 4924: 4922: 4919: 4918: 4897: 4890: 4879: 4878: 4877: 4876: 4875: 4873: 4870: 4869: 4853: 4851: 4848: 4847: 4825: 4824: 4822: 4819: 4818: 4809: 4793: 4789: 4782: 4766: 4762: 4755: 4732: 4728: 4721: 4704: 4700: 4693: 4671: 4667: 4650: 4646: 4639: 4623: 4619: 4612: 4596: 4592: 4582: 4562: 4558: 4551: 4535: 4531: 4526: 4522: 4515: 4499: 4495: 4488: 4480:. p. 267. 4468: 4464: 4457: 4441: 4437: 4432: 4428: 4421: 4405: 4401: 4392: 4390: 4386: 4375: 4369: 4365: 4359:Wayback Machine 4350: 4346: 4334: 4333: 4324: 4323: 4316: 4314: 4305: 4301: 4291: 4289: 4284: 4283: 4279: 4272: 4256: 4252: 4245: 4222: 4215: 4208: 4204: 4191: 4190: 4186: 4176: 4174: 4173:on 6 April 2020 4159: 4155: 4116: 4112: 4105: 4089: 4085: 4024: 4020: 4009: 4005: 3989: 3988: 3976: 3962: 3961: 3957: 3942: 3926: 3922: 3915: 3898: 3894: 3879: 3878: 3874: 3867: 3847: 3843: 3833: 3831: 3824: 3808: 3804: 3794: 3792: 3788: 3773: 3764: 3757: 3753: 3748: 3747: 3741:vim centrifugam 3738: 3734: 3729: 3686: 3679: 3676: 3666:rather than as 3630:circular motion 3615: 3603: 3554: 3551: 3550: 3547: 3532: 3520: 3503:amusement rides 3424: 3412:oblate spheroid 3383: 3357: 3326: 3321: 3318: 3317: 3301: 3299: 3296: 3295: 3278: 3274: 3272: 3269: 3268: 3251: 3247: 3241: 3237: 3232: 3229: 3228: 3209: 3201: 3190: 3182: 3179: 3178: 3154: 3149: 3144: 3139: 3138: 3134: 3126: 3115: 3112: 3111: 3092: 3081: 3076: 3071: 3066: 3058: 3055: 3054: 3018: 3014: 3009: 3008: 3002: 2996: 2991: 2990: 2989: 2987: 2983: 2969: 2961: 2950: 2929: 2928: 2922: 2917: 2916: 2914: 2910: 2902: 2888: 2874: 2873: 2867: 2862: 2861: 2859: 2848: 2846: 2843: 2842: 2822: 2818: 2813: 2812: 2806: 2800: 2795: 2794: 2793: 2791: 2789: 2786: 2785: 2761: 2757: 2752: 2751: 2745: 2739: 2734: 2733: 2732: 2730: 2726: 2724: 2721: 2720: 2717: 2699: 2698: 2684: 2676: 2665: 2647: 2646: 2640: 2635: 2634: 2632: 2628: 2620: 2609: 2595: 2594: 2588: 2583: 2582: 2580: 2564: 2560: 2555: 2554: 2548: 2542: 2537: 2536: 2535: 2533: 2529: 2520: 2519: 2506: 2498: 2480: 2479: 2473: 2468: 2467: 2465: 2461: 2460: 2456: 2448: 2440: 2426: 2425: 2419: 2414: 2413: 2411: 2393: 2392: 2386: 2381: 2380: 2378: 2374: 2366: 2350: 2346: 2341: 2340: 2334: 2328: 2323: 2322: 2321: 2319: 2315: 2306: 2305: 2294: 2293: 2287: 2282: 2281: 2279: 2271: 2263: 2249: 2248: 2242: 2237: 2236: 2234: 2216: 2215: 2209: 2204: 2203: 2201: 2197: 2189: 2173: 2169: 2164: 2163: 2157: 2151: 2146: 2145: 2144: 2142: 2138: 2129: 2128: 2115: 2107: 2089: 2088: 2082: 2077: 2076: 2074: 2070: 2069: 2065: 2054: 2053: 2048: 2046: 2032: 2031: 2025: 2020: 2019: 2017: 2006: 2005: 2000: 1998: 1986: 1982: 1977: 1976: 1970: 1964: 1959: 1958: 1957: 1955: 1948: 1943: 1939: 1937: 1934: 1933: 1907: 1906: 1900: 1895: 1894: 1892: 1888: 1877: 1876: 1871: 1869: 1867: 1864: 1863: 1841: 1840: 1834: 1829: 1828: 1826: 1824: 1821: 1820: 1811: 1785: 1781: 1776: 1775: 1769: 1763: 1758: 1757: 1756: 1754: 1746: 1744: 1741: 1740: 1730: 1724: 1702: 1691: 1689: 1686: 1685: 1681: 1678: 1670:right-hand rule 1665: 1659: 1643: 1635: 1633: 1630: 1629: 1623: 1603: 1600: 1599: 1577: 1569: 1551: 1550: 1544: 1539: 1538: 1536: 1532: 1518: 1517: 1511: 1506: 1505: 1503: 1501: 1498: 1497: 1489: 1476: 1470: 1454: 1438: 1422: 1415: 1407: 1399: 1387: 1375: 1363: 1343: 1335: 1332: 1325: 1319: 1313: 1305: 1302: 1286: 1276: 1270: 1240:restoring force 1232: 1203: 1175: 1163:roller coasters 1154: 1149: 1105: 1069:bucket argument 1010:Henry Oldenburg 1004:The same year, 940:From 1659, the 938: 932: 860: 856: 845: 842: 841: 837: 793: 752: 739: 738: 731: 730: 729: 604: 596: 595: 575: 529:Circular motion 523: 513: 512: 511: 468: 438: 435: 414: 393: 385: 384: 381: 380: 338: 328: 320: 319: 318: 277: 273:Mechanical work 266: 250: 188: 180: 179: 178: 133: 125: 102: 78: 72: 68: 66: 57: 56: 54: 51: 50: 24: 17: 12: 11: 5: 5529: 5519: 5518: 5513: 5508: 5503: 5498: 5484: 5483: 5469: 5468:External links 5466: 5464: 5463: 5440: 5433: 5413: 5396: 5357: 5330:(5): 399–405. 5307: 5292: 5272: 5256: 5241: 5226: 5206: 5169:(1): 143–198. 5119:(1): 143–198. 5098: 5080: 5077: 5059: 5037: 5030: 5010: 4990: 4959: 4952: 4949: 4940: 4933: 4930: 4900: 4893: 4886: 4883: 4856: 4832: 4829: 4807: 4787: 4780: 4760: 4753: 4726: 4719: 4698: 4691: 4665: 4644: 4637: 4617: 4610: 4590: 4580: 4574:. p. 93. 4556: 4549: 4529: 4520: 4513: 4493: 4486: 4462: 4455: 4435: 4426: 4419: 4399: 4363: 4344: 4299: 4277: 4270: 4250: 4243: 4213: 4202: 4184: 4153: 4126:(3): 599–606. 4110: 4103: 4083: 4038:(11): 110401. 4018: 4003: 3974: 3955: 3940: 3920: 3913: 3892: 3872: 3865: 3841: 3822: 3802: 3754: 3752: 3749: 3746: 3745: 3731: 3730: 3728: 3725: 3724: 3723: 3718: 3713: 3708: 3703: 3698: 3692: 3691: 3688:Physics portal 3675: 3672: 3614: 3611: 3601: 3573: 3570: 3564: 3561: 3558: 3545: 3531: 3528: 3519: 3516: 3511: 3510: 3499: 3492:buoyant forces 3484: 3474: 3459: 3439: 3423: 3420: 3403: 3402: 3395: 3379:Main article: 3356: 3353: 3339: 3336: 3333: 3329: 3325: 3304: 3281: 3277: 3254: 3250: 3244: 3240: 3236: 3216: 3212: 3208: 3204: 3200: 3197: 3193: 3189: 3186: 3165: 3161: 3157: 3152: 3147: 3142: 3137: 3133: 3129: 3125: 3122: 3119: 3109:Coriolis force 3095: 3091: 3088: 3084: 3079: 3074: 3069: 3065: 3062: 3036: 3029: 3021: 3017: 3012: 3005: 2999: 2994: 2986: 2982: 2979: 2976: 2972: 2968: 2964: 2960: 2957: 2953: 2949: 2946: 2942: 2936: 2932: 2925: 2920: 2913: 2909: 2905: 2901: 2898: 2895: 2891: 2887: 2881: 2877: 2870: 2865: 2858: 2855: 2851: 2825: 2821: 2816: 2809: 2803: 2798: 2772: 2764: 2760: 2755: 2748: 2742: 2737: 2729: 2716: 2713: 2697: 2691: 2687: 2683: 2679: 2675: 2672: 2668: 2664: 2660: 2654: 2650: 2643: 2638: 2631: 2627: 2623: 2619: 2616: 2612: 2608: 2602: 2598: 2591: 2586: 2579: 2575: 2567: 2563: 2558: 2551: 2545: 2540: 2532: 2528: 2525: 2523: 2521: 2517: 2509: 2505: 2501: 2497: 2493: 2487: 2483: 2476: 2471: 2464: 2459: 2455: 2451: 2447: 2443: 2439: 2433: 2429: 2422: 2417: 2410: 2406: 2400: 2396: 2389: 2384: 2377: 2373: 2369: 2365: 2361: 2353: 2349: 2344: 2337: 2331: 2326: 2318: 2314: 2311: 2309: 2307: 2301: 2297: 2290: 2285: 2278: 2274: 2270: 2266: 2262: 2256: 2252: 2245: 2240: 2233: 2229: 2223: 2219: 2212: 2207: 2200: 2196: 2192: 2188: 2184: 2176: 2172: 2167: 2160: 2154: 2149: 2141: 2137: 2134: 2132: 2130: 2126: 2118: 2114: 2110: 2106: 2102: 2096: 2092: 2085: 2080: 2073: 2068: 2061: 2057: 2051: 2045: 2039: 2035: 2028: 2023: 2013: 2009: 2003: 1997: 1989: 1985: 1980: 1973: 1967: 1962: 1954: 1951: 1949: 1946: 1942: 1941: 1920: 1914: 1910: 1903: 1898: 1891: 1884: 1880: 1874: 1848: 1844: 1837: 1832: 1799: 1788: 1784: 1779: 1772: 1766: 1761: 1753: 1749: 1712: 1705: 1701: 1698: 1694: 1677: 1674: 1664:has magnitude 1646: 1642: 1638: 1607: 1587: 1580: 1576: 1572: 1568: 1564: 1558: 1554: 1547: 1542: 1535: 1531: 1525: 1521: 1514: 1509: 1452: 1436: 1420: 1397: 1385: 1373: 1330: 1323: 1317: 1301: 1298: 1272:Main article: 1269: 1266: 1236:spring balance 1231: 1228: 1202: 1199: 1174: 1171: 1153: 1150: 1148: 1145: 1137:Coriolis force 1104: 1101: 1039:vis centrifuga 1014:vis centrifuga 934:Main article: 931: 928: 868: 863: 859: 855: 852: 849: 795: 794: 792: 791: 784: 777: 769: 766: 765: 764: 763: 750: 733: 732: 728: 727: 722: 717: 712: 707: 702: 697: 692: 687: 682: 677: 672: 667: 662: 657: 652: 647: 642: 637: 632: 627: 622: 617: 612: 606: 605: 602: 601: 598: 597: 594: 593: 574: 573: 568: 563: 558: 556:Coriolis force 553: 552: 551: 541: 536: 531: 525: 524: 519: 518: 515: 514: 510: 509: 504: 499: 498: 497: 492: 482: 477: 472: 465: 454: 453: 452: 447: 434: 433: 428: 423: 418: 411: 406: 401: 395: 394: 391: 390: 387: 386: 383: 382: 379: 378: 373: 368: 363: 358: 353: 347: 341: 339: 332: 329: 326: 325: 322: 321: 317: 316: 311: 306: 301: 296: 291: 286: 281: 275: 270: 264: 259: 248: 243: 238: 233: 228: 227: 226: 221: 211: 206: 201: 196: 190: 189: 186: 185: 182: 181: 177: 176: 171: 166: 161: 156: 151: 146: 141: 135: 134: 131: 130: 127: 126: 124: 123: 118: 113: 107: 104: 103: 98: 84: 81: 75: 71: 65: 47: 46: 40: 39: 15: 9: 6: 4: 3: 2: 5528: 5517: 5514: 5512: 5509: 5507: 5504: 5502: 5499: 5497: 5494: 5493: 5491: 5481: 5476: 5472: 5471: 5459: 5454: 5453: 5444: 5436: 5430: 5426: 5425: 5417: 5409: 5408: 5400: 5392: 5388: 5384: 5380: 5376: 5372: 5368: 5361: 5353: 5349: 5345: 5341: 5337: 5333: 5329: 5325: 5318: 5311: 5303: 5299: 5295: 5293:81-203-0894-8 5289: 5285: 5284: 5276: 5269: 5266: 5260: 5252: 5245: 5237: 5233: 5229: 5227:0-691-08472-6 5223: 5219: 5218: 5210: 5202: 5198: 5194: 5190: 5186: 5182: 5177: 5172: 5168: 5164: 5160: 5152: 5148: 5144: 5140: 5136: 5132: 5127: 5122: 5118: 5114: 5110: 5102: 5095: 5078: 5075: 5062: 5056: 5052: 5048: 5041: 5033: 5027: 5023: 5022: 5014: 5007: 5005: 4979: 4975: 4957: 4950: 4947: 4938: 4931: 4928: 4916: 4898: 4891: 4884: 4881: 4816: 4813:In the above 4810: 4804: 4800: 4799: 4791: 4783: 4777: 4773: 4772: 4764: 4756: 4750: 4746: 4742: 4738: 4730: 4722: 4716: 4712: 4711: 4702: 4694: 4688: 4684: 4679: 4678: 4669: 4661: 4657: 4656: 4648: 4640: 4634: 4630: 4629: 4621: 4613: 4607: 4603: 4602: 4594: 4587: 4583: 4577: 4573: 4569: 4568: 4560: 4552: 4546: 4542: 4541: 4533: 4524: 4516: 4510: 4506: 4505: 4497: 4489: 4483: 4479: 4475: 4474: 4466: 4458: 4452: 4448: 4447: 4439: 4430: 4422: 4416: 4412: 4411: 4403: 4389:on 2007-02-27 4385: 4381: 4374: 4367: 4360: 4356: 4353: 4348: 4340: 4328: 4312: 4311: 4303: 4287: 4281: 4273: 4267: 4263: 4262: 4254: 4246: 4240: 4236: 4235: 4230: 4226: 4220: 4218: 4211: 4206: 4198: 4194: 4188: 4172: 4168: 4164: 4157: 4149: 4145: 4141: 4137: 4133: 4129: 4125: 4121: 4114: 4106: 4100: 4096: 4095: 4087: 4079: 4075: 4071: 4067: 4063: 4059: 4055: 4051: 4046: 4041: 4037: 4033: 4029: 4022: 4014: 4007: 3999: 3993: 3985: 3981: 3977: 3971: 3967: 3966: 3959: 3951: 3947: 3943: 3941:0-8176-3823-7 3937: 3933: 3932: 3924: 3916: 3914:9780520009271 3910: 3906: 3905: 3896: 3888: 3884: 3883: 3876: 3868: 3862: 3858: 3854: 3853: 3845: 3829: 3825: 3823:9789004235656 3819: 3815: 3814: 3806: 3787: 3783: 3779: 3772: 3768: 3767:Yoder, Joella 3762: 3760: 3755: 3742: 3736: 3732: 3722: 3721:Lamm equation 3719: 3717: 3714: 3712: 3709: 3707: 3704: 3702: 3699: 3697: 3694: 3693: 3689: 3683: 3678: 3671: 3669: 3665: 3660: 3658: 3653: 3651: 3647: 3643: 3639: 3635: 3631: 3627: 3623: 3620: 3610: 3608: 3604: 3597: 3593: 3592:Newton's laws 3589: 3588: 3568: 3562: 3559: 3548: 3541: 3537: 3527: 3525: 3515: 3508: 3504: 3500: 3497: 3493: 3488: 3485: 3482: 3478: 3475: 3472: 3468: 3464: 3460: 3457: 3456:inertia reels 3453: 3452:rock climbing 3449: 3444: 3440: 3437: 3433: 3429: 3428: 3427: 3419: 3417: 3413: 3407: 3400: 3396: 3393: 3389: 3388: 3387: 3382: 3373: 3366: 3361: 3352: 3334: 3331: 3279: 3275: 3252: 3248: 3242: 3238: 3234: 3206: 3195: 3187: 3184: 3163: 3159: 3150: 3135: 3131: 3123: 3120: 3117: 3110: 3089: 3086: 3077: 3063: 3060: 3053: 3047: 3034: 3027: 3019: 3015: 2997: 2984: 2980: 2977: 2966: 2955: 2947: 2944: 2940: 2934: 2911: 2907: 2899: 2896: 2893: 2885: 2879: 2856: 2853: 2823: 2819: 2801: 2770: 2762: 2758: 2740: 2727: 2712: 2695: 2681: 2670: 2662: 2658: 2652: 2629: 2625: 2617: 2614: 2606: 2600: 2577: 2573: 2565: 2561: 2543: 2530: 2526: 2524: 2515: 2503: 2495: 2491: 2485: 2462: 2457: 2453: 2445: 2437: 2431: 2408: 2404: 2398: 2375: 2371: 2363: 2359: 2351: 2347: 2329: 2316: 2312: 2310: 2299: 2276: 2268: 2260: 2254: 2231: 2227: 2221: 2198: 2194: 2186: 2182: 2174: 2170: 2152: 2139: 2135: 2133: 2124: 2112: 2104: 2100: 2094: 2071: 2066: 2059: 2043: 2037: 2011: 1995: 1987: 1983: 1965: 1952: 1950: 1918: 1912: 1889: 1882: 1846: 1817: 1814: 1797: 1786: 1782: 1764: 1751: 1738: 1733: 1727: 1710: 1699: 1696: 1673: 1671: 1662: 1640: 1626: 1621: 1605: 1585: 1574: 1566: 1562: 1556: 1533: 1529: 1523: 1494: 1493: 1486: 1482: 1481: 1473: 1468: 1463: 1462: 1458: 1451: 1447: 1446: 1442: 1435: 1431: 1430: 1426: 1419: 1412: 1411: 1404: 1403: 1396: 1392: 1391: 1384: 1380: 1379: 1372: 1368: 1367: 1360: 1359: 1354: 1353: 1348: 1347: 1340: 1339: 1329: 1322: 1316: 1310: 1309: 1297: 1295: 1291: 1285: 1281: 1275: 1265: 1263: 1261: 1256: 1251: 1249: 1244: 1241: 1237: 1227: 1225: 1221: 1217: 1212: 1208: 1198: 1194: 1192: 1188: 1184: 1179: 1170: 1168: 1164: 1160: 1144: 1142: 1138: 1133: 1130: 1124: 1122: 1116: 1114: 1110: 1100: 1098: 1094: 1090: 1085: 1082: 1079:Around 1883, 1077: 1074: 1070: 1066: 1062: 1057: 1055: 1050: 1048: 1044: 1040: 1036: 1035: 1029: 1027: 1024:, as well as 1023: 1019: 1015: 1011: 1007: 1001: 999: 992: 990: 986: 985: 979: 977: 973: 969: 968: 963: 962: 957: 956: 951: 947: 946:vi centrifuga 943: 937: 927: 925: 921: 920: 914: 912: 908: 907:banked curves 904: 900: 896: 892: 888: 884: 879: 866: 861: 857: 853: 850: 847: 836: 832: 828: 825: 821: 817: 813: 809: 805: 801: 790: 785: 783: 778: 776: 771: 770: 768: 767: 761: 751: 748: 743: 737: 736: 735: 734: 726: 723: 721: 718: 716: 713: 711: 708: 706: 703: 701: 698: 696: 693: 691: 688: 686: 683: 681: 678: 676: 673: 671: 668: 666: 663: 661: 658: 656: 653: 651: 648: 646: 643: 641: 638: 636: 633: 631: 628: 626: 623: 621: 618: 616: 613: 611: 608: 607: 600: 599: 592: 588: 584: 580: 577: 576: 572: 569: 567: 564: 562: 559: 557: 554: 550: 547: 546: 545: 542: 540: 537: 535: 532: 530: 527: 526: 522: 517: 516: 508: 505: 503: 500: 496: 493: 491: 488: 487: 486: 483: 481: 478: 476: 473: 471: 466: 463: 459: 456: 455: 451: 448: 445: 441: 437: 436: 432: 429: 427: 424: 422: 419: 417: 412: 410: 407: 405: 402: 400: 397: 396: 389: 388: 377: 374: 372: 369: 367: 364: 362: 359: 357: 354: 352: 349: 348: 346: 345: 340: 337: 336: 331: 330: 324: 323: 315: 312: 310: 307: 305: 302: 300: 297: 295: 292: 290: 287: 285: 282: 280: 276: 274: 271: 269: 265: 263: 260: 257: 253: 249: 247: 244: 242: 239: 237: 234: 232: 229: 225: 222: 220: 217: 216: 215: 212: 210: 207: 205: 202: 200: 197: 195: 192: 191: 184: 183: 175: 172: 170: 167: 165: 162: 160: 157: 155: 152: 150: 147: 145: 142: 140: 137: 136: 129: 128: 122: 119: 117: 114: 112: 109: 108: 106: 105: 101: 82: 79: 69: 63: 49: 48: 45: 42: 41: 37: 36: 28: 22: 5496:Acceleration 5451: 5443: 5423: 5416: 5406: 5399: 5374: 5370: 5360: 5327: 5323: 5310: 5282: 5275: 5267: 5259: 5244: 5216: 5209: 5166: 5162: 5116: 5112: 5105:See p. 5 in 5101: 5064: 5050: 5040: 5020: 5013: 5003: 4977: 4973: 4914: 4812: 4797: 4790: 4770: 4763: 4744: 4740: 4729: 4709: 4701: 4676: 4668: 4654: 4647: 4627: 4620: 4600: 4593: 4585: 4566: 4559: 4539: 4532: 4523: 4503: 4496: 4472: 4465: 4445: 4438: 4429: 4409: 4402: 4391:. Retrieved 4384:the original 4379: 4366: 4347: 4315:. Retrieved 4309: 4302: 4290:. Retrieved 4280: 4260: 4253: 4233: 4205: 4196: 4193:"Centrifuge" 4187: 4175:. Retrieved 4171:the original 4166: 4156: 4123: 4119: 4113: 4093: 4086: 4035: 4031: 4021: 4012: 4006: 3964: 3958: 3930: 3923: 3903: 3895: 3881: 3875: 3851: 3844: 3832:. Retrieved 3812: 3805: 3793:. Retrieved 3781: 3777: 3740: 3735: 3711:Folk physics 3667: 3663: 3661: 3656: 3654: 3649: 3645: 3616: 3606: 3599: 3585: 3543: 3533: 3523: 3521: 3512: 3477:Spin casting 3425: 3422:Applications 3408: 3404: 3384: 3048: 2718: 1862:and once to 1818: 1812: 1737:acceleration 1731: 1725: 1679: 1676:Acceleration 1660: 1624: 1618:denotes the 1491: 1490: 1484: 1479: 1478: 1471: 1460: 1459: 1456: 1449: 1444: 1443: 1440: 1433: 1428: 1427: 1424: 1417: 1409: 1408: 1401: 1400: 1394: 1389: 1388: 1382: 1377: 1376: 1370: 1365: 1364: 1357: 1356: 1351: 1350: 1345: 1344: 1337: 1336: 1327: 1320: 1314: 1307: 1306: 1303: 1287: 1257: 1254: 1252: 1245: 1233: 1204: 1195: 1180: 1176: 1155: 1134: 1125: 1117: 1106: 1103:Introduction 1086: 1078: 1058: 1051: 1047:Robert Hooke 1038: 1032: 1031:In 1687, in 1030: 1013: 1006:Isaac Newton 1003: 997: 994: 982: 981:In 1673, in 980: 971: 945: 939: 917: 915: 880: 830: 826: 819: 799: 798: 589: / 585: / 583:displacement 581: / 543: 442: / 404:Displacement 342: 333: 327:Formulations 314:Virtual work 254: / 194:Acceleration 187:Fundamentals 4976:are called 4913:are called 4335:|work= 3487:Centrifuges 3052:Euler force 1141:Euler force 1121:fixed stars 972:centrifugus 883:centrifuges 725:von Neumann 392:Core topics 5490:Categories 5377:(8): 173. 4393:2007-01-21 4045:1906.03400 3751:References 3739:In Latin: 3365:immiscible 1278:See also: 1268:Derivation 1071:, and the 660:d'Alembert 640:Maupertuis 603:Scientists 485:Rigid body 159:Kinematics 5511:Mechanics 5352:250827660 5079:˙ 5076:ϕ 4951:˙ 4932:˙ 4885:˙ 4831:˙ 4446:Mechanics 4337:ignored ( 4327:cite book 4148:120947179 4078:182952610 3992:cite book 3984:165958146 3816:. 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Index

Centripetal force

Classical mechanics
Second law of motion
History
Timeline
Textbooks
Applied
Celestial
Continuum
Dynamics
Kinematics
Kinetics
Statics
Statistical mechanics
Acceleration
Angular momentum
Couple
D'Alembert's principle
Energy
kinetic
potential
Force
Frame of reference
Inertial frame of reference
Impulse
Inertia
Moment of inertia
Mass
Mechanical power

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