Knowledge (XXG)

Generalized coordinates

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737: 996: 969: 1096: 857: 1066: 869: 895: 8368: 3999: 7693: 3757: 5310: 3964: 750: 9250: 6978: 7326: 5756: 2732: 8044: 5079: 3002: 8340: 1408: 6442: 9023: 7688:{\displaystyle T={\frac {1}{2}}m_{1}\mathbf {v} _{1}\cdot \mathbf {v} _{1}+{\frac {1}{2}}m_{2}\mathbf {v} _{2}\cdot \mathbf {v} _{2}={\frac {1}{2}}(m_{1}+m_{2})L_{1}^{2}{\dot {\theta }}_{1}^{2}+{\frac {1}{2}}m_{2}L_{2}^{2}{\dot {\theta }}_{2}^{2}+m_{2}L_{1}L_{2}\cos(\theta _{2}-\theta _{1}){\dot {\theta }}_{1}{\dot {\theta }}_{2}.} 6701: 9012: 2241: 2519: 9727:
Some authors set the constraint equations to a constant for convenience with some constraint equations (e.g. pendulums), others set it to zero. It makes no difference because the constant can be subtracted to give zero on one side of the equation. Also, in Lagrange's equations of the first kind, only
7721: 5305:{\displaystyle {\frac {d}{dt}}{\frac {\partial T}{\partial {\dot {x}}}}-{\frac {\partial T}{\partial x}}=F_{x}+\lambda {\frac {\partial f}{\partial x}},\quad {\frac {d}{dt}}{\frac {\partial T}{\partial {\dot {y}}}}-{\frac {\partial T}{\partial y}}=F_{y}+\lambda {\frac {\partial f}{\partial y}}.} 5057: 2791: 8055: 9535: 3491: 6135: 2037: 3741: 9390: 5589: 1188: 7142: 6198: 9245:{\displaystyle \delta W=\left(\sum _{j=1}^{m}\mathbf {F} _{j}\cdot {\frac {\partial \mathbf {r} _{j}}{\partial q_{1}}}\right)\delta {q}_{1}+\ldots +\left(\sum _{j=1}^{m}\mathbf {F} _{j}\cdot {\frac {\partial \mathbf {r} _{j}}{\partial q_{n}}}\right)\delta {q}_{n}.} 7315: 6973:{\displaystyle \delta \mathbf {r} _{1}=(L_{1}\cos \theta _{1},L_{1}\sin \theta _{1})\delta \theta _{1},\quad \delta \mathbf {r} _{2}=(L_{1}\cos \theta _{1},L_{1}\sin \theta _{1})\delta \theta _{1}+(L_{2}\cos \theta _{2},L_{2}\sin \theta _{2})\delta \theta _{2}} 6673: 2482: 3307: 8868: 5464: 2078: 4600: 4891: 5951: 2727:{\displaystyle {\dot {\mathbf {r} }}_{k}\cdot {\dot {\mathbf {r} }}_{k}=\sum _{i,j=1}^{n}\left({\frac {\partial \mathbf {r} _{k}}{\partial q_{i}}}\cdot {\frac {\partial \mathbf {r} _{k}}{\partial q_{j}}}\right){\dot {q}}_{i}{\dot {q}}_{j},} 3150: 8039:{\displaystyle (m_{1}+m_{2})L_{1}^{2}{\ddot {\theta }}_{1}+m_{2}L_{1}L_{2}{\ddot {\theta }}_{2}\cos(\theta _{2}-\theta _{1})+m_{2}L_{1}L_{2}{\dot {\theta _{2}}}^{2}\sin(\theta _{1}-\theta _{2})=-(m_{1}+m_{2})gL_{1}\sin \theta _{1},} 8803: 8578: 6555: 4902: 2997:{\displaystyle ds_{k}^{2}=d\mathbf {r} _{k}\cdot d\mathbf {r} _{k}=\sum _{i,j=1}^{n}\left({\frac {\partial \mathbf {r} _{k}}{\partial q_{i}}}\cdot {\frac {\partial \mathbf {r} _{k}}{\partial q_{j}}}\right)dq_{i}dq_{j}\,,} 2350:
An example of such a constraint is a rolling wheel or knife-edge that constrains the direction of the velocity vector. Non-holonomic constraints can also involve next-order derivatives such as generalized accelerations.
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The relationship between the use of generalized coordinates and Cartesian coordinates to characterize the movement of a mechanical system can be illustrated by considering the constrained dynamics of a simple pendulum.
1734: 8335:{\displaystyle m_{2}L_{2}^{2}{\ddot {\theta }}_{2}+m_{2}L_{1}L_{2}{\ddot {\theta }}_{1}\cos(\theta _{2}-\theta _{1})+m_{2}L_{1}L_{2}{\dot {\theta _{1}}}^{2}\sin(\theta _{2}-\theta _{1})=-m_{2}gL_{2}\sin \theta _{2}.} 9643: 3942: 4686: 1852: 3586: 9401: 4339: 3337: 2279:
A mechanical system can involve constraints on both the generalized coordinates and their derivatives. Constraints of this type are known as non-holonomic. First-order non-holonomic constraints have the form
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One generalized coordinate (one degree of freedom) on paths in 2D. Only one generalized coordinate is needed to uniquely specify positions on the curve. In these examples, that variable is either arc length
5962: 5727: 4481: 3837:; either one is determined from the other. The constraint force is the reaction force the wire exerts on the bead to keep it on the wire, and the non-constraint applied force is gravity acting on the bead. 2246:
and so generally depends on the generalized velocities and coordinates. Since we are free to specify the initial values of the generalized coordinates and velocities separately, the generalized coordinates
1872: 8477: 4235: 3616: 2345: 1403:{\displaystyle {\begin{aligned}&\mathbf {r} _{1}=(x_{1},y_{1},z_{1}),\\&\mathbf {r} _{2}=(x_{2},y_{2},z_{2}),\\&\qquad \qquad \vdots \\&\mathbf {r} _{N}=(x_{N},y_{N},z_{N})\end{aligned}}} 9265: 5664: 5494: 1590:). It is ideal to use the minimum number of coordinates needed to define the configuration of the entire system, while taking advantage of the constraints on the system. These quantities are known as 91: 115: 6437:{\displaystyle \mathbf {r} _{1}=(L_{1}\sin \theta _{1},-L_{1}\cos \theta _{1}),\quad \mathbf {r} _{2}=(L_{1}\sin \theta _{1},-L_{1}\cos \theta _{1})+(L_{2}\sin \theta _{2},-L_{2}\cos \theta _{2}).} 6989: 1193: 821:
An example of a generalized coordinate would be to describe the position of a pendulum using the angle of the pendulum relative to vertical, rather than by the x and y position of the pendulum.
7153: 4772: 6586: 4133: 1761:. A degree of freedom corresponds to one quantity that changes the configuration of the system, for example the angle of a pendulum, or the arc length traversed by a bead along a wire. 1498: 2374: 1040:
Generalized coordinates are usually selected to provide the minimum number of independent coordinates that define the configuration of a system, which simplifies the formulation of
9007:{\displaystyle \delta \mathbf {r} _{j}={\frac {\partial \mathbf {r} _{j}}{\partial q_{1}}}\delta {q}_{1}+\ldots +{\frac {\partial \mathbf {r} _{j}}{\partial q_{n}}}\delta {q}_{n},} 8621:. Only two coordinates are needed instead of three, because the position of the bob can be parameterized by two numbers, and the constraint equation connects the three coordinates 4405: 3180: 824:
Although there may be many possible choices for generalized coordinates for a physical system, they are generally selected to simplify calculations, such as the solution of the
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If it is possible to find from the constraints as many independent variables as there are degrees of freedom, these can be used as generalized coordinates. The position vector
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constraint equations. There is not necessarily one constraint equation for each particle, and if there are no constraints on the system then there are no constraint equations.
5321: 2236:{\displaystyle \mathbf {v} _{k}={\dot {\mathbf {r} }}_{k}={\frac {d\mathbf {r} _{k}}{dt}}=\sum _{j=1}^{n}{\frac {\partial \mathbf {r} _{k}}{\partial q_{j}}}{\dot {q}}_{j}\,.} 4511: 8667:. When formulated in terms of generalized coordinates, this is equivalent to the requirement that the generalized forces for any virtual displacement are zero, that is 4787: 5820: 814:
of the generalized coordinates of the system. The adjective "generalized" distinguishes these parameters from the traditional use of the term "coordinate" to refer to
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states that if a system is in static equilibrium, the virtual work of the applied forces is zero for all virtual movements of the system from this state, that is,
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are the generalized forces acting on the system. Kane shows that these generalized forces can also be formulated in terms of the ratio of time derivatives,
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which illustrates the kinetic energy is in general a function of the generalized velocities, coordinates, and time if the constraints also vary with time, so
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In the case the constraints on the particles are time-independent, then all partial derivatives with respect to time are zero, and the kinetic energy is a
8488: 1754: 5052:{\displaystyle T={\frac {1}{2}}m\mathbf {v} \cdot \mathbf {v} ={\frac {1}{2}}m({\dot {x}}^{2}+{\dot {y}}^{2})={\frac {1}{2}}mL^{2}{\dot {\theta }}^{2}.} 489: 1507:
will appear explicitly in the constraint equations. At any instant of time, any one coordinate will be determined from the other coordinates, e.g. if
6453: 462: 3017:. Thus for time-independent constraints it is sufficient to know the line element to quickly obtain the kinetic energy of particles and hence the 1503:
which connects all the 3 spatial coordinates of that particle together, so they are not independent. The constraint may change with time, so time
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of the system. They are all independent of one other, and each is a function of time. Geometrically they can be lengths along straight lines, or
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for the system. If the coordinates are independent of one another, the number of independent generalized coordinates is defined by the number of
1621: 9571: 3846: 736: 10007: 9805: 9530:{\displaystyle F_{i}=\sum _{j=1}^{m}\mathbf {F} _{j}\cdot {\frac {\partial \mathbf {v} _{j}}{\partial {\dot {q}}_{i}}},\quad i=1,\ldots ,n,} 4611: 1789: 3522: 3486:{\displaystyle \left({\frac {ds}{dt}}\right)^{2}={\dot {r}}^{2}+r^{2}{\dot {\theta }}^{2}+r^{2}\sin ^{2}\theta \,{\dot {\varphi }}^{2}\,.} 6130:{\displaystyle f_{2}(x_{1},y_{1},x_{2},y_{2})=(\mathbf {r} _{2}-\mathbf {r} _{1})\cdot (\mathbf {r} _{2}-\mathbf {r} _{1})-L_{2}^{2}=0.} 4262: 444: 2032:{\displaystyle {\dot {\mathbf {q} }}={\frac {d\mathbf {q} }{dt}}=({\dot {q}}_{1}(t),\ {\dot {q}}_{2}(t),\ \ldots ,\ {\dot {q}}_{n}(t))} 10097: 10052: 9565:
In order for the virtual work to be zero for an arbitrary virtual displacement, each of the generalized forces must be zero, that is
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Suppose the wire changes its shape with time, by flexing. Then the constraint equation and position of the particle are respectively
3736:{\displaystyle {\frac {\partial L}{\partial q_{i}}}={\frac {d}{dt}}{\frac {\partial L}{\partial {\dot {q}}_{i}}}={\dot {p}}_{i}=0\,.} 10130: 10033: 9929: 9776: 3776:
For a bead sliding on a frictionless wire subject only to gravity in 2d space, the constraint on the bead can be stated in the form
774: 9385:{\displaystyle F_{i}=\sum _{j=1}^{m}\mathbf {F} _{j}\cdot {\frac {\partial \mathbf {r} _{j}}{\partial q_{i}}},\quad i=1,\ldots ,n,} 8389: 5584:{\displaystyle {\frac {d}{dt}}{\frac {\partial T}{\partial {\dot {\theta }}}}-{\frac {\partial T}{\partial \theta }}=F_{\theta },} 4148: 2286: 995: 5600: 110: 47: 7137:{\displaystyle \delta W=-(m_{1}+m_{2})gL_{1}\sin \theta _{1}\delta \theta _{1}-m_{2}gL_{2}\sin \theta _{2}\delta \theta _{2},} 6564:
is the acceleration due to gravity. Therefore, the virtual work of gravity on the two masses as they follow the trajectories
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that define the angular position of each mass of the double pendulum from the vertical direction. In this case, we have
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It is instructive to see the various cases of polar coordinates in 2D and 3D, owing to their frequent appearance. In 2D
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free to swing in any angular direction subject to gravity, the constraint on the pendulum bob can be stated in the form
7310:{\displaystyle F_{\theta _{1}}=-(m_{1}+m_{2})gL_{1}\sin \theta _{1},\quad F_{\theta _{2}}=-m_{2}gL_{2}\sin \theta _{2}.} 1065: 868: 767: 754: 515: 438: 7698: 203: 3821:
along the curve from some point on the wire. This is a suitable choice of generalized coordinate for the system. Only
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coordinates can be eliminated, one coordinate from each constraint equation. The number of independent coordinates is
434: 235: 6668:{\displaystyle \delta W=\mathbf {F} _{1}\cdot \delta \mathbf {r} _{1}+\mathbf {F} _{2}\cdot \delta \mathbf {r} _{2}.} 10154: 9999: 4723: 4415: 654: 543: 469: 329: 262: 3951:
due to the changing coordinates as the wire changes its shape. Notice time appears implicitly via the coordinates
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along the curve is a legitimate generalized coordinate since the position is uniquely determined, but the angle
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The formulation of Lagrange's equations for this system yields six equations in the four Cartesian coordinates
2477:{\displaystyle T={\frac {1}{2}}\sum _{k=1}^{N}m_{k}{\dot {\mathbf {r} }}_{k}\cdot {\dot {\mathbf {r} }}_{k}\,,} 1049: 684: 528: 8367: 3998: 1453: 9674: 3302:{\displaystyle \left({\frac {ds}{dt}}\right)^{2}={\dot {r}}^{2}+r^{2}{\dot {\theta }}^{2}+{\dot {z}}^{2}\,,} 3156: 674: 634: 398: 4361: 806:. These parameters must uniquely define the configuration of the system relative to a reference state. The 10070: 9669: 3967:
Simple pendulum. Since the rod is rigid, the position of the bob is constrained according to the equation
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coordinate is needed instead of two, because the position of the bead can be parameterized by one number,
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to define the configuration of this system avoids the constraint provided by the equation of the circle.
10159: 9659: 9654: 8596: 5459:{\displaystyle m{\ddot {x}}=\lambda (2x),\quad m{\ddot {y}}=-mg+\lambda (2y),\quad x^{2}+y^{2}-L^{2}=0,} 3506: 3313: 1179: 1167: 1138: 836: 815: 689: 664: 350: 168: 10021: 8722:, then the virtual work generated by a virtual displacement from the equilibrium position is given by 1137:
are needed to specify the points on the curve, one possibility is shown for each case. The full three
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This formulation yields one equation because there is a single parameter and no constraint equation.
3018: 2771: 1436: 1041: 795: 709: 704: 669: 577: 573: 565: 555: 345: 338: 94: 4595:{\displaystyle \delta \mathbf {r} =(\delta x,\delta y)=(L\cos \theta ,L\sin \theta )\delta \theta .} 4886:{\displaystyle \mathbf {v} =({\dot {x}},{\dot {y}})=(L\cos \theta ,L\sin \theta ){\dot {\theta }},} 825: 484: 425: 403: 148: 143: 138: 38: 10107: 9689: 8376: 5946:{\displaystyle f_{1}(x_{1},y_{1},x_{2},y_{2})=\mathbf {r} _{1}\cdot \mathbf {r} _{1}-L_{1}^{2}=0} 3607: 614: 355: 230: 198: 158: 9945: 1857:
and the generalized coordinates can be thought of as parameters associated with the constraint.
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are not necessary because any two determines the third according to the equations of the curves.
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Two generalized coordinates, two degrees of freedom, on curved surfaces in 3D. Only two numbers
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in this case is gravity. Notice the initial position of the wire can lead to different motions.
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T. R. Kane and D. A. Levinson, Dynamics: theory and applications, McGraw-Hill, New York, 1985
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provides an alternative to the Cartesian formulation of the dynamics of the double pendulum.
3145:{\displaystyle \left({\frac {ds}{dt}}\right)^{2}={\dot {r}}^{2}+r^{2}{\dot {\theta }}^{2}\,,} 9684: 2058: 719: 699: 644: 639: 585: 560: 415: 273: 218: 193: 1044:
of motion. However, it can also occur that a useful set of generalized coordinates may be
10125:. HRW Series in Mechanical Engineering. United States of America: CBS College Publishing. 5767: 5760: 5739:
is a generalized coordinate that can be used in the same way as the Cartesian coordinates
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is related to the other by the equations of the curves. They can also be parameterized by
714: 659: 609: 604: 523: 3610:, because the time derivative is zero implying the momentum is a constant of the motion; 3756: 8606: 2365: 741: 649: 550: 267: 213: 9712:, as shown here, as the condition for the constraint on that particle to be holonomic. 8798:{\displaystyle \delta W=\sum _{j=1}^{m}\mathbf {F} _{j}\cdot \delta \mathbf {r} _{j}.} 17: 10143: 9708:
Some authors e.g. Hand & Finch take the form of the position vector for particle
629: 456: 8609:. A logical choice of generalized coordinates to describe the motion are the angles 8573:{\displaystyle \mathbf {r} =(x(\theta ,\phi ),y(\theta ,\phi ),z(\theta ,\phi ))\,,} 5814:
define their two trajectories. These vectors satisfy the two constraint equations,
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hanging from a pivot point so that it is constrained to move on a circle of radius
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Bead constrained to move on a frictionless wire. The wire exerts a reaction force
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Still for the time-independent case, this expression is equivalent to taking the
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along curves, or angles; not necessarily Cartesian coordinates or other standard
9679: 2488: 840: 6550:{\displaystyle \mathbf {F} _{1}=(0,-m_{1}g),\quad \mathbf {F} _{2}=(0,-m_{2}g)} 5766:
The benefits of generalized coordinates become apparent with the analysis of a
10062: 5755: 3815: 1746: 811: 479: 153: 501: 1729:{\displaystyle \mathbf {q} (t)=(q_{1}(t),\ q_{2}(t),\ \ldots ,\ q_{n}(t))} 4011: 420: 303: 278: 9638:{\displaystyle \delta W=0\quad \Rightarrow \quad F_{i}=0,i=1,\ldots ,n.} 4142:. This equation also provides a constraint on the velocity components, 3937:{\displaystyle f(\mathbf {r} ,t)=0\,,\quad \mathbf {r} =(x(s,t),y(s,t))} 4248:
from the vertical direction. It can be used to define the coordinates
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Generalized coordinates are paired with generalized momenta to provide
393: 246: 163: 4702:-component of the applied force. In the same way, the coefficient of 8605:
is measured along the suspension point to the bob, here treated as a
4681:{\displaystyle \delta W=-mg\delta y=-mgL\sin(\theta )\delta \theta .} 1847:{\displaystyle \mathbf {r} _{k}=\mathbf {r} _{k}(\mathbf {q} (t))\,,} 802:
are a set of parameters used to represent the state of a system in a
452: 298: 208: 3581:{\displaystyle p_{i}={\frac {\partial L}{\partial {\dot {q}}_{i}}}.} 5754: 4334:{\displaystyle \mathbf {r} =(x,y)=(L\sin \theta ,-L\cos \theta ).} 3997: 1613: 1175: 288: 283: 225: 4022:. The position of the mass is defined by the coordinate vector 1030:
is not since there are multiple positions for a single value of
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because the bob moves in the surface of a sphere. The position
5722:{\displaystyle {\ddot {\theta }}+{\frac {g}{L}}\sin \theta =0.} 4476:{\displaystyle \delta W=\mathbf {F} \cdot \delta \mathbf {r} .} 2368:
of the system is the energy of the system's motion, defined as
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on the bead to keep it on the wire. The non-constraint force
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denote the virtual displacements of each point in the body.
8472:{\displaystyle f(\mathbf {r} )=x^{2}+y^{2}+z^{2}-l^{2}=0\,,} 4230:{\displaystyle {\dot {f}}(x,y)=2x{\dot {x}}+2y{\dot {y}}=0.} 2340:{\displaystyle g(\mathbf {q} ,{\dot {\mathbf {q} }},t)=0\,,} 9769:
Fundamentals of multibody dynamics: theory and applications
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yield two equations in the unknown generalized coordinates
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is the tension in the rod. Again the non-constraint force
2491:. The kinetic energy is a function only of the velocities 9752:
p. 397,  §7.2.1 Selection of generalized coordinates
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is the velocity of the point of application of the force
5659:{\displaystyle mL^{2}{\ddot {\theta }}=-mgL\sin \theta ,} 86:{\displaystyle {\textbf {F}}={\frac {d\mathbf {p} }{dt}}} 6447:
The force of gravity acting on the masses is given by,
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where the position of the pendulum bob can be written
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generalized coordinates (and, through them, of time),
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So far, the configuration of the system is defined by
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so any one of them is determined from the other two.
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To complete the analysis consider the kinetic energy
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Mechanics: From Newton's Laws to Deterministic Chaos
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Notice that the force of gravity acting on the mass
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themselves. By contrast an important observation is
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coordinates, and the reduction by constraints means
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constraints, each has an equation, so there will be
10028:(3rd ed.). San Francisco, CA: Addison Wesley. 9895: 9859: 9820: 1048:, which means that they are related by one or more 9637: 9529: 9384: 9244: 9006: 8797: 8572: 8471: 8334: 8038: 7687: 7309: 7136: 6972: 6667: 6549: 6436: 6129: 5945: 5721: 5658: 5583: 5458: 5304: 5063:D'Alembert's form of the principle of virtual work 5051: 4885: 4766: 4680: 4594: 4475: 4399: 4355:is formulated in the usual Cartesian coordinates, 4333: 4229: 4127: 3936: 3735: 3580: 3485: 3301: 3144: 2996: 2726: 2476: 2339: 2235: 2031: 1846: 1728: 1572:dimensions, the original configuration would need 1492: 1402: 85: 3007:and dividing by the square differential in time, 8702:be applied to points with Cartesian coordinates 7320:Compute the kinetic energy of this system to be 3787:, where the position of the bead can be written 9835: 4041:is in the vertical direction. The coordinates 9907: 6175:that arise from the two constraint equations. 4037:measured in the plane of the circle such that 2355:Physical quantities in generalized coordinates 5065:for the pendulum in terms of the coordinates 4767:{\displaystyle F_{\theta }=-mgL\sin \theta .} 3013:, to obtain the velocity squared of particle 989:. Multiple intersections of radius with path. 775: 8: 4493:can be computed in terms of the coordinates 9794:"§5.1 Manifolds of generalized coordinates" 4128:{\displaystyle f(x,y)=x^{2}+y^{2}-L^{2}=0,} 2774:of degree 2 in the generalized velocities. 1608:. It is convenient to collect them into an 1413:Any of the position vectors can be denoted 929:. Having both of the Cartesian coordinates 10112:: CS1 maint: location missing publisher ( 8371:Spherical pendulum: angles and velocities. 6178:Now introduce the generalized coordinates 4049:are related by the equation of the circle 782: 768: 29: 10047:. Cambridge: Cambridge University Press. 9871: 9596: 9573: 9490: 9479: 9478: 9466: 9461: 9454: 9445: 9440: 9433: 9422: 9409: 9403: 9345: 9330: 9325: 9318: 9309: 9304: 9297: 9286: 9273: 9267: 9233: 9228: 9210: 9195: 9190: 9183: 9174: 9169: 9162: 9151: 9127: 9122: 9104: 9089: 9084: 9077: 9068: 9063: 9056: 9045: 9025: 8995: 8990: 8977: 8962: 8957: 8950: 8935: 8930: 8917: 8902: 8897: 8890: 8881: 8876: 8870: 8786: 8781: 8768: 8763: 8756: 8745: 8730: 8566: 8492: 8490: 8465: 8453: 8440: 8427: 8414: 8399: 8391: 8323: 8307: 8294: 8275: 8262: 8243: 8231: 8225: 8224: 8217: 8207: 8197: 8181: 8168: 8149: 8138: 8137: 8130: 8120: 8110: 8097: 8086: 8085: 8078: 8073: 8063: 8057: 8027: 8011: 7995: 7982: 7960: 7947: 7928: 7916: 7910: 7909: 7902: 7892: 7882: 7866: 7853: 7834: 7823: 7822: 7815: 7805: 7795: 7782: 7771: 7770: 7763: 7758: 7745: 7732: 7723: 7676: 7665: 7664: 7657: 7646: 7645: 7635: 7622: 7603: 7593: 7583: 7570: 7565: 7554: 7553: 7546: 7541: 7531: 7517: 7508: 7503: 7492: 7491: 7484: 7479: 7466: 7453: 7436: 7427: 7422: 7412: 7407: 7400: 7386: 7377: 7372: 7362: 7357: 7350: 7336: 7328: 7298: 7282: 7269: 7251: 7246: 7232: 7216: 7200: 7187: 7166: 7161: 7155: 7125: 7112: 7096: 7083: 7070: 7057: 7041: 7025: 7012: 6991: 6964: 6948: 6932: 6919: 6903: 6887: 6871: 6855: 6842: 6826: 6810: 6805: 6791: 6775: 6759: 6746: 6730: 6714: 6709: 6703: 6656: 6651: 6638: 6633: 6623: 6618: 6605: 6600: 6588: 6535: 6510: 6505: 6488: 6463: 6458: 6455: 6422: 6406: 6390: 6374: 6355: 6339: 6323: 6307: 6291: 6286: 6272: 6256: 6240: 6224: 6208: 6203: 6200: 6115: 6110: 6094: 6089: 6079: 6074: 6058: 6053: 6043: 6038: 6022: 6009: 5996: 5983: 5970: 5964: 5931: 5926: 5913: 5908: 5898: 5893: 5880: 5867: 5854: 5841: 5828: 5822: 5694: 5680: 5679: 5677: 5618: 5617: 5611: 5602: 5572: 5545: 5528: 5527: 5513: 5498: 5496: 5441: 5428: 5415: 5366: 5365: 5329: 5328: 5323: 5279: 5267: 5240: 5223: 5222: 5208: 5193: 5169: 5157: 5130: 5113: 5112: 5098: 5083: 5081: 5040: 5029: 5028: 5021: 5004: 4992: 4981: 4980: 4970: 4959: 4958: 4941: 4933: 4925: 4912: 4904: 4869: 4868: 4818: 4817: 4803: 4802: 4791: 4789: 4731: 4725: 4613: 4518: 4513: 4465: 4454: 4443: 4365: 4363: 4266: 4264: 4210: 4209: 4189: 4188: 4153: 4152: 4150: 4110: 4097: 4084: 4057: 3881: 3876: 3856: 3848: 3729: 3717: 3706: 3705: 3692: 3681: 3680: 3665: 3650: 3638: 3620: 3618: 3566: 3555: 3554: 3539: 3530: 3524: 3479: 3473: 3462: 3461: 3459: 3447: 3437: 3424: 3413: 3412: 3405: 3392: 3381: 3380: 3370: 3346: 3339: 3295: 3289: 3278: 3277: 3267: 3256: 3255: 3248: 3235: 3224: 3223: 3213: 3189: 3182: 3138: 3132: 3121: 3120: 3113: 3100: 3089: 3088: 3078: 3054: 3047: 2990: 2984: 2971: 2950: 2935: 2930: 2923: 2911: 2896: 2891: 2884: 2873: 2856: 2843: 2838: 2825: 2820: 2807: 2802: 2793: 2715: 2704: 2703: 2696: 2685: 2684: 2669: 2654: 2649: 2642: 2630: 2615: 2610: 2603: 2592: 2575: 2562: 2551: 2549: 2548: 2538: 2527: 2525: 2524: 2521: 2470: 2464: 2453: 2451: 2450: 2440: 2429: 2427: 2426: 2419: 2409: 2398: 2384: 2376: 2333: 2307: 2305: 2304: 2296: 2288: 2229: 2223: 2212: 2211: 2201: 2186: 2181: 2174: 2168: 2157: 2133: 2128: 2121: 2112: 2101: 2099: 2098: 2088: 2083: 2080: 2011: 2000: 1999: 1968: 1957: 1956: 1934: 1923: 1922: 1899: 1893: 1879: 1877: 1876: 1874: 1840: 1823: 1814: 1809: 1799: 1794: 1791: 1708: 1674: 1649: 1625: 1623: 1469: 1464: 1455: 1387: 1374: 1361: 1345: 1340: 1310: 1297: 1284: 1268: 1263: 1245: 1232: 1219: 1203: 1198: 1192: 1190: 67: 61: 52: 51: 49: 10043:Hand, Louis N.; Finch, Janet D. (1998). 9747: 8641:Generalized coordinates and virtual work 8366: 3962: 3955:explicitly in the constraint equations. 3755: 2042:(each dot over a quantity indicates one 27:System configuration relative to another 10121:Torby, Bruce (1984). "Energy Methods". 9800:(5th ed.). Springer. p. 286. 9740: 9720: 9701: 8844:depends on the generalized coordinates 8345:The use of the generalized coordinates 4244:, that defines the angular position of 2781:squared of the trajectory for particle 1493:{\displaystyle f(\mathbf {r} _{k},t)=0} 1174:of each particle can be written as a 3- 101: 37: 10105: 10088:Landau, L. D.; Lifshitz, E.M. (1976). 1860:The corresponding time derivatives of 9970: 9883: 9847: 4400:{\displaystyle \mathbf {F} =(0,-mg),} 464:Newton's law of universal gravitation 7: 1528:. One constraint equation counts as 6983:Thus, the virtual work is given by 4605:Thus, the virtual work is given by 4002:Dynamic model of a simple pendulum. 445:Mechanics of planar particle motion 53: 9474: 9457: 9338: 9321: 9203: 9186: 9097: 9080: 8970: 8953: 8910: 8893: 5556: 5548: 5524: 5516: 5290: 5282: 5251: 5243: 5219: 5211: 5180: 5172: 5141: 5133: 5109: 5101: 3676: 3668: 3631: 3623: 3550: 3542: 2943: 2926: 2904: 2887: 2662: 2645: 2623: 2606: 2194: 2177: 847:Constraints and degrees of freedom 25: 9896:Goldstein, Poole & Safko 2002 9860:Goldstein, Poole & Safko 2002 9821:Goldstein, Poole & Safko 2002 6161:and the two Lagrange multipliers 4781:of the mass, using the velocity, 9988:Bibliography of cited references 9961:, scienceworld.wolfram.com. 2007 9462: 9441: 9326: 9305: 9191: 9170: 9085: 9064: 8958: 8898: 8877: 8782: 8764: 8682:Let the forces on the system be 8493: 8400: 7423: 7408: 7373: 7358: 6806: 6710: 6652: 6634: 6619: 6601: 6506: 6459: 6287: 6204: 6090: 6075: 6054: 6039: 5909: 5894: 5488:, those equations take the form 5315:This yields the three equations 4934: 4926: 4792: 4519: 4466: 4455: 4366: 4267: 4138:that constrains the movement of 3882: 3857: 2931: 2892: 2839: 2821: 2650: 2611: 2552: 2528: 2454: 2430: 2308: 2297: 2182: 2129: 2102: 2084: 1900: 1880: 1866:are the generalized velocities, 1824: 1810: 1795: 1626: 1465: 1341: 1264: 1199: 1094: 1064: 994: 967: 893: 867: 855: 749: 748: 735: 68: 10123:Advanced Dynamics for Engineers 10069:(5th ed.). River Edge NJ: 9924:(2nd ed.). Prentice Hall. 9765:"§2.4: Generalized coordinates" 9591: 9587: 9502: 9357: 7241: 7147:and the generalized forces are 6800: 6503: 6284: 5410: 5361: 5192: 4691:Notice that the coefficient of 4501:, or in terms of the parameter 3880: 1330: 1329: 9998:(3rd ed.). Cambridge UK: 9763:Farid M. L. Amirouche (2006). 9588: 8563: 8560: 8548: 8539: 8527: 8518: 8506: 8500: 8404: 8396: 8281: 8255: 8187: 8161: 8001: 7975: 7966: 7940: 7872: 7846: 7751: 7725: 7641: 7615: 7472: 7446: 7206: 7180: 7031: 7005: 6954: 6896: 6877: 6819: 6781: 6723: 6544: 6519: 6497: 6472: 6428: 6367: 6361: 6300: 6278: 6217: 6100: 6070: 6064: 6034: 6028: 5976: 5886: 5834: 5735:This shows that the parameter 5404: 5395: 5355: 5346: 4998: 4954: 4865: 4835: 4829: 4799: 4666: 4660: 4580: 4550: 4544: 4526: 4391: 4373: 4325: 4292: 4286: 4274: 4176: 4164: 4074: 4062: 3947:which now both depend on time 3931: 3928: 3916: 3907: 3895: 3889: 3867: 3853: 2324: 2293: 2026: 2023: 2017: 1980: 1974: 1946: 1940: 1918: 1837: 1834: 1828: 1820: 1723: 1720: 1714: 1686: 1680: 1661: 1655: 1642: 1636: 1630: 1481: 1460: 1393: 1354: 1316: 1277: 1251: 1212: 1: 9920:Greenwood, Donald T. (1987). 4713:along generalized coordinate 4429:as it follows the trajectory 941:are unnecessary since either 371:Koopman–von Neumann mechanics 4240:Now introduce the parameter 1016:. Self-intersection of path. 439:Non-inertial reference frame 9994:Ginsberg, Jerry H. (2008). 9836:Kibble & Berkshire 2004 9728:the derivatives are needed. 4416:acceleration due to gravity 366:Appell's equation of motion 236:Inertial frame of reference 10181: 10092:(Third ed.). Oxford. 10065:; Berkshire, F.H. (2004). 10000:Cambridge University Press 9908:Landau & Lifshitz 1976 3599:depend on some coordinate 5747:to analyze the pendulum. 2275:Non-holonomic constraints 1779:is a function of all the 1594:in this context, denoted 1532:constraint. If there are 1444:of the form for particle 9771:. Springer. p. 46. 3994:in this case is gravity. 1753:. There is one for each 1739:which is a point in the 1434:labels the particles. A 529:Rotating reference frame 361:Hamilton–Jacobi equation 9792:Florian Scheck (2010). 9675:Curvilinear coordinates 7699:Euler–Lagrange equation 5469:in the three unknowns, 4425:of gravity on the mass 3982:, the constraint force 3157:cylindrical coordinates 2046:). The velocity vector 1592:generalized coordinates 800:generalized coordinates 470:Newton's laws of motion 330:Newton's laws of motion 10071:Imperial College Press 10024:; Safko, John (2002). 9922:Principles of Dynamics 9670:Orthogonal coordinates 9639: 9531: 9438: 9386: 9302: 9246: 9167: 9061: 9008: 8799: 8761: 8597:spherical polar angles 8574: 8473: 8372: 8336: 8040: 7689: 7311: 7138: 6974: 6695:can be computed to be 6669: 6551: 6438: 6131: 5947: 5763: 5723: 5660: 5585: 5460: 5306: 5053: 4887: 4768: 4682: 4596: 4477: 4401: 4335: 4231: 4129: 4003: 3995: 3938: 3773: 3737: 3582: 3487: 3303: 3146: 2998: 2878: 2728: 2597: 2502:, not the coordinates 2478: 2414: 2341: 2237: 2173: 2033: 1848: 1751:orthogonal coordinates 1730: 1521:are given, then so is 1494: 1404: 1101:Closed curved surface 808:generalized velocities 497:Simple harmonic motion 410:Euler's laws of motion 204:D'Alembert's principle 87: 18:Generalized coordinate 10165:Mechanical quantities 9944:Richard Fitzpatrick, 9872:Hand & Finch 1998 9660:Hamiltonian mechanics 9655:Canonical coordinates 9640: 9532: 9418: 9387: 9282: 9247: 9147: 9041: 9009: 8832:Now assume that each 8800: 8741: 8575: 8474: 8379:with constant length 8370: 8337: 8041: 7690: 7312: 7139: 6975: 6670: 6552: 6439: 6132: 5948: 5770:. For the two masses 5758: 5724: 5661: 5586: 5461: 5307: 5054: 4888: 4769: 4683: 4597: 4478: 4402: 4336: 4232: 4130: 4001: 3966: 3939: 3759: 3738: 3583: 3507:canonically conjugate 3488: 3314:spherical coordinates 3304: 3147: 2999: 2852: 2729: 2571: 2479: 2394: 2342: 2269:independent variables 2238: 2153: 2072:with respect to time 2034: 1849: 1731: 1495: 1405: 1180:Cartesian coordinates 1168:real coordinate space 1139:Cartesian coordinates 1056:Holonomic constraints 837:canonical coordinates 816:Cartesian coordinates 351:Hamiltonian mechanics 169:Statistical mechanics 88: 10150:Lagrangian mechanics 10045:Analytical mechanics 9996:Engineering dynamics 9572: 9402: 9266: 9024: 8869: 8729: 8489: 8390: 8375:For a 3D example, a 8056: 7722: 7327: 7154: 6990: 6702: 6587: 6454: 6199: 5963: 5821: 5676: 5601: 5495: 5484:Using the parameter 5322: 5080: 4903: 4788: 4724: 4612: 4512: 4442: 4362: 4263: 4149: 4056: 3847: 3814:is a parameter, the 3617: 3523: 3503:generalized momentum 3497:Generalized momentum 3338: 3181: 3046: 2792: 2772:homogeneous function 2520: 2375: 2287: 2079: 1873: 1790: 1622: 1454: 1437:holonomic constraint 1189: 1071:Open curved surface 1042:Lagrange's equations 796:analytical mechanics 574:Angular acceleration 566:Rotational frequency 346:Lagrangian mechanics 339:Analytical mechanics 95:Second law of motion 48: 10067:Classical Mechanics 10026:Classical Mechanics 9957:Eric W. Weisstein, 8083: 7768: 7575: 7551: 7513: 7489: 6120: 5936: 4014:consists of a mass 3509:to" the coordinate 2812: 1742:configuration space 1442:constraint equation 1001:Closed curved path 900:Closed curved path 826:equations of motion 804:configuration space 426:Harmonic oscillator 404:Equations of motion 39:Classical mechanics 33:Part of a series on 10018:Goldstein, Herbert 9946:Newtonian Dynamics 9690:Generalized forces 9635: 9527: 9382: 9242: 9004: 8795: 8660:for any variation 8570: 8469: 8377:spherical pendulum 8373: 8363:Spherical pendulum 8332: 8069: 8036: 7754: 7685: 7552: 7537: 7490: 7475: 7307: 7134: 6970: 6665: 6547: 6434: 6127: 6106: 5943: 5922: 5764: 5719: 5656: 5581: 5456: 5302: 5049: 4883: 4764: 4678: 4592: 4473: 4397: 4331: 4227: 4125: 4004: 3996: 3934: 3774: 3733: 3608:conserved quantity 3591:If the Lagrangian 3578: 3483: 3299: 3142: 2994: 2798: 2724: 2487:in which · is the 2474: 2337: 2267:can be treated as 2233: 2029: 1844: 1726: 1490: 1400: 1398: 862:Open straight path 830:degrees of freedom 742:Physics portal 356:Routhian mechanics 231:Frame of reference 83: 10155:Dynamical systems 10009:978-0-521-88303-0 9807:978-3-642-05369-6 9497: 9487: 9352: 9217: 9111: 8984: 8924: 8240: 8146: 8094: 7925: 7831: 7779: 7673: 7654: 7562: 7525: 7500: 7444: 7394: 7344: 5702: 5688: 5626: 5563: 5540: 5536: 5511: 5374: 5337: 5297: 5258: 5235: 5231: 5206: 5187: 5148: 5125: 5121: 5096: 5037: 5012: 4989: 4967: 4949: 4920: 4877: 4826: 4811: 4711:generalized force 4218: 4197: 4161: 3714: 3699: 3689: 3663: 3645: 3573: 3563: 3470: 3421: 3389: 3364: 3286: 3264: 3232: 3207: 3129: 3097: 3072: 3026:polar coordinates 2957: 2918: 2712: 2693: 2676: 2637: 2559: 2535: 2461: 2437: 2392: 2315: 2220: 2208: 2148: 2109: 2008: 1997: 1988: 1965: 1954: 1931: 1913: 1887: 1755:degree of freedom 1703: 1694: 1669: 974:Open curved path 874:Open curved path 792: 791: 539:Centrifugal force 534:Centripetal force 490:Euler's equations 475:Relative velocity 251:Moment of inertia 81: 55: 16:(Redirected from 10172: 10136: 10117: 10111: 10103: 10084: 10058: 10039: 10013: 9982: 9979: 9973: 9968: 9962: 9955: 9949: 9942: 9936: 9935: 9917: 9911: 9905: 9899: 9893: 9887: 9881: 9875: 9869: 9863: 9857: 9851: 9845: 9839: 9833: 9824: 9818: 9812: 9811: 9789: 9783: 9782: 9760: 9754: 9745: 9729: 9725: 9713: 9711: 9706: 9685:Stiffness matrix 9644: 9642: 9641: 9636: 9601: 9600: 9561: 9550: 9536: 9534: 9533: 9528: 9498: 9496: 9495: 9494: 9489: 9488: 9480: 9472: 9471: 9470: 9465: 9455: 9450: 9449: 9444: 9437: 9432: 9414: 9413: 9391: 9389: 9388: 9383: 9353: 9351: 9350: 9349: 9336: 9335: 9334: 9329: 9319: 9314: 9313: 9308: 9301: 9296: 9278: 9277: 9258: 9251: 9249: 9248: 9243: 9238: 9237: 9232: 9223: 9219: 9218: 9216: 9215: 9214: 9201: 9200: 9199: 9194: 9184: 9179: 9178: 9173: 9166: 9161: 9132: 9131: 9126: 9117: 9113: 9112: 9110: 9109: 9108: 9095: 9094: 9093: 9088: 9078: 9073: 9072: 9067: 9060: 9055: 9013: 9011: 9010: 9005: 9000: 8999: 8994: 8985: 8983: 8982: 8981: 8968: 8967: 8966: 8961: 8951: 8940: 8939: 8934: 8925: 8923: 8922: 8921: 8908: 8907: 8906: 8901: 8891: 8886: 8885: 8880: 8861: 8843: 8828: 8804: 8802: 8801: 8796: 8791: 8790: 8785: 8773: 8772: 8767: 8760: 8755: 8721: 8701: 8678: 8666: 8659: 8636: 8620: 8604: 8594: 8579: 8577: 8576: 8571: 8496: 8478: 8476: 8475: 8470: 8458: 8457: 8445: 8444: 8432: 8431: 8419: 8418: 8403: 8382: 8358: 8341: 8339: 8338: 8333: 8328: 8327: 8312: 8311: 8299: 8298: 8280: 8279: 8267: 8266: 8248: 8247: 8242: 8241: 8236: 8235: 8226: 8222: 8221: 8212: 8211: 8202: 8201: 8186: 8185: 8173: 8172: 8154: 8153: 8148: 8147: 8139: 8135: 8134: 8125: 8124: 8115: 8114: 8102: 8101: 8096: 8095: 8087: 8082: 8077: 8068: 8067: 8045: 8043: 8042: 8037: 8032: 8031: 8016: 8015: 8000: 7999: 7987: 7986: 7965: 7964: 7952: 7951: 7933: 7932: 7927: 7926: 7921: 7920: 7911: 7907: 7906: 7897: 7896: 7887: 7886: 7871: 7870: 7858: 7857: 7839: 7838: 7833: 7832: 7824: 7820: 7819: 7810: 7809: 7800: 7799: 7787: 7786: 7781: 7780: 7772: 7767: 7762: 7750: 7749: 7737: 7736: 7714: 7694: 7692: 7691: 7686: 7681: 7680: 7675: 7674: 7666: 7662: 7661: 7656: 7655: 7647: 7640: 7639: 7627: 7626: 7608: 7607: 7598: 7597: 7588: 7587: 7574: 7569: 7564: 7563: 7555: 7550: 7545: 7536: 7535: 7526: 7518: 7512: 7507: 7502: 7501: 7493: 7488: 7483: 7471: 7470: 7458: 7457: 7445: 7437: 7432: 7431: 7426: 7417: 7416: 7411: 7405: 7404: 7395: 7387: 7382: 7381: 7376: 7367: 7366: 7361: 7355: 7354: 7345: 7337: 7316: 7314: 7313: 7308: 7303: 7302: 7287: 7286: 7274: 7273: 7258: 7257: 7256: 7255: 7237: 7236: 7221: 7220: 7205: 7204: 7192: 7191: 7173: 7172: 7171: 7170: 7143: 7141: 7140: 7135: 7130: 7129: 7117: 7116: 7101: 7100: 7088: 7087: 7075: 7074: 7062: 7061: 7046: 7045: 7030: 7029: 7017: 7016: 6979: 6977: 6976: 6971: 6969: 6968: 6953: 6952: 6937: 6936: 6924: 6923: 6908: 6907: 6892: 6891: 6876: 6875: 6860: 6859: 6847: 6846: 6831: 6830: 6815: 6814: 6809: 6796: 6795: 6780: 6779: 6764: 6763: 6751: 6750: 6735: 6734: 6719: 6718: 6713: 6694: 6674: 6672: 6671: 6666: 6661: 6660: 6655: 6643: 6642: 6637: 6628: 6627: 6622: 6610: 6609: 6604: 6579: 6563: 6556: 6554: 6553: 6548: 6540: 6539: 6515: 6514: 6509: 6493: 6492: 6468: 6467: 6462: 6443: 6441: 6440: 6435: 6427: 6426: 6411: 6410: 6395: 6394: 6379: 6378: 6360: 6359: 6344: 6343: 6328: 6327: 6312: 6311: 6296: 6295: 6290: 6277: 6276: 6261: 6260: 6245: 6244: 6229: 6228: 6213: 6212: 6207: 6191: 6174: 6160: 6136: 6134: 6133: 6128: 6119: 6114: 6099: 6098: 6093: 6084: 6083: 6078: 6063: 6062: 6057: 6048: 6047: 6042: 6027: 6026: 6014: 6013: 6001: 6000: 5988: 5987: 5975: 5974: 5952: 5950: 5949: 5944: 5935: 5930: 5918: 5917: 5912: 5903: 5902: 5897: 5885: 5884: 5872: 5871: 5859: 5858: 5846: 5845: 5833: 5832: 5813: 5783: 5746: 5742: 5738: 5728: 5726: 5725: 5720: 5703: 5695: 5690: 5689: 5681: 5665: 5663: 5662: 5657: 5628: 5627: 5619: 5616: 5615: 5590: 5588: 5587: 5582: 5577: 5576: 5564: 5562: 5554: 5546: 5541: 5539: 5538: 5537: 5529: 5522: 5514: 5512: 5510: 5499: 5487: 5480: 5476: 5472: 5465: 5463: 5462: 5457: 5446: 5445: 5433: 5432: 5420: 5419: 5376: 5375: 5367: 5339: 5338: 5330: 5311: 5309: 5308: 5303: 5298: 5296: 5288: 5280: 5272: 5271: 5259: 5257: 5249: 5241: 5236: 5234: 5233: 5232: 5224: 5217: 5209: 5207: 5205: 5194: 5188: 5186: 5178: 5170: 5162: 5161: 5149: 5147: 5139: 5131: 5126: 5124: 5123: 5122: 5114: 5107: 5099: 5097: 5095: 5084: 5072: 5068: 5058: 5056: 5055: 5050: 5045: 5044: 5039: 5038: 5030: 5026: 5025: 5013: 5005: 4997: 4996: 4991: 4990: 4982: 4975: 4974: 4969: 4968: 4960: 4950: 4942: 4937: 4929: 4921: 4913: 4892: 4890: 4889: 4884: 4879: 4878: 4870: 4828: 4827: 4819: 4813: 4812: 4804: 4795: 4780: 4773: 4771: 4770: 4765: 4736: 4735: 4716: 4709:is known as the 4708: 4701: 4697: 4687: 4685: 4684: 4679: 4601: 4599: 4598: 4593: 4522: 4504: 4500: 4496: 4492: 4482: 4480: 4479: 4474: 4469: 4458: 4434: 4428: 4413: 4406: 4404: 4403: 4398: 4369: 4354: 4347: 4340: 4338: 4337: 4332: 4270: 4255: 4251: 4247: 4243: 4236: 4234: 4233: 4228: 4220: 4219: 4211: 4199: 4198: 4190: 4163: 4162: 4154: 4141: 4134: 4132: 4131: 4126: 4115: 4114: 4102: 4101: 4089: 4088: 4048: 4044: 4040: 4036: 4021: 4017: 3993: 3987: 3981: 3950: 3943: 3941: 3940: 3935: 3885: 3860: 3836: 3832: 3828: 3820: 3813: 3809: 3786: 3771: 3765: 3742: 3740: 3739: 3734: 3722: 3721: 3716: 3715: 3707: 3700: 3698: 3697: 3696: 3691: 3690: 3682: 3674: 3666: 3664: 3662: 3651: 3646: 3644: 3643: 3642: 3629: 3621: 3605: 3594: 3587: 3585: 3584: 3579: 3574: 3572: 3571: 3570: 3565: 3564: 3556: 3548: 3540: 3535: 3534: 3515: 3492: 3490: 3489: 3484: 3478: 3477: 3472: 3471: 3463: 3452: 3451: 3442: 3441: 3429: 3428: 3423: 3422: 3414: 3410: 3409: 3397: 3396: 3391: 3390: 3382: 3375: 3374: 3369: 3365: 3363: 3355: 3347: 3330: 3308: 3306: 3305: 3300: 3294: 3293: 3288: 3287: 3279: 3272: 3271: 3266: 3265: 3257: 3253: 3252: 3240: 3239: 3234: 3233: 3225: 3218: 3217: 3212: 3208: 3206: 3198: 3190: 3173: 3151: 3149: 3148: 3143: 3137: 3136: 3131: 3130: 3122: 3118: 3117: 3105: 3104: 3099: 3098: 3090: 3083: 3082: 3077: 3073: 3071: 3063: 3055: 3038: 3016: 3012: 3003: 3001: 3000: 2995: 2989: 2988: 2976: 2975: 2963: 2959: 2958: 2956: 2955: 2954: 2941: 2940: 2939: 2934: 2924: 2919: 2917: 2916: 2915: 2902: 2901: 2900: 2895: 2885: 2877: 2872: 2848: 2847: 2842: 2830: 2829: 2824: 2811: 2806: 2784: 2766: 2733: 2731: 2730: 2725: 2720: 2719: 2714: 2713: 2705: 2701: 2700: 2695: 2694: 2686: 2682: 2678: 2677: 2675: 2674: 2673: 2660: 2659: 2658: 2653: 2643: 2638: 2636: 2635: 2634: 2621: 2620: 2619: 2614: 2604: 2596: 2591: 2567: 2566: 2561: 2560: 2555: 2550: 2543: 2542: 2537: 2536: 2531: 2526: 2512: 2501: 2483: 2481: 2480: 2475: 2469: 2468: 2463: 2462: 2457: 2452: 2445: 2444: 2439: 2438: 2433: 2428: 2424: 2423: 2413: 2408: 2393: 2385: 2346: 2344: 2343: 2338: 2317: 2316: 2311: 2306: 2300: 2266: 2253: 2242: 2240: 2239: 2234: 2228: 2227: 2222: 2221: 2213: 2209: 2207: 2206: 2205: 2192: 2191: 2190: 2185: 2175: 2172: 2167: 2149: 2147: 2139: 2138: 2137: 2132: 2122: 2117: 2116: 2111: 2110: 2105: 2100: 2093: 2092: 2087: 2071: 2059:total derivative 2056: 2038: 2036: 2035: 2030: 2016: 2015: 2010: 2009: 2001: 1995: 1986: 1973: 1972: 1967: 1966: 1958: 1952: 1939: 1938: 1933: 1932: 1924: 1914: 1912: 1904: 1903: 1894: 1889: 1888: 1883: 1878: 1865: 1853: 1851: 1850: 1845: 1827: 1819: 1818: 1813: 1804: 1803: 1798: 1782: 1778: 1774: 1760: 1735: 1733: 1732: 1727: 1713: 1712: 1701: 1692: 1679: 1678: 1667: 1654: 1653: 1629: 1611: 1607: 1589: 1575: 1571: 1567: 1553: 1550:quantities, but 1549: 1539: 1535: 1527: 1520: 1513: 1506: 1499: 1497: 1496: 1491: 1474: 1473: 1468: 1447: 1433: 1423: 1409: 1407: 1406: 1401: 1399: 1392: 1391: 1379: 1378: 1366: 1365: 1350: 1349: 1344: 1337: 1325: 1315: 1314: 1302: 1301: 1289: 1288: 1273: 1272: 1267: 1260: 1250: 1249: 1237: 1236: 1224: 1223: 1208: 1207: 1202: 1195: 1166:particles in 3D 1165: 1162:For a system of 1155: 1136: 1119: 1098: 1089: 1068: 1033: 1029: 1025: 1015: 998: 988: 971: 956: 952: 948: 944: 940: 928: 924: 914: 897: 888: 871: 859: 784: 777: 770: 757: 752: 751: 744: 740: 739: 645:Johann Bernoulli 640:Daniel Bernoulli 561:Tangential speed 465: 441: 416:Fictitious force 411: 263:Mechanical power 253: 194:Angular momentum 92: 90: 89: 84: 82: 80: 72: 71: 62: 57: 56: 30: 21: 10180: 10179: 10175: 10174: 10173: 10171: 10170: 10169: 10140: 10139: 10133: 10120: 10104: 10100: 10087: 10081: 10061: 10055: 10042: 10036: 10016: 10010: 9993: 9990: 9985: 9980: 9976: 9969: 9965: 9959:Double Pendulum 9956: 9952: 9943: 9939: 9932: 9919: 9918: 9914: 9906: 9902: 9894: 9890: 9882: 9878: 9870: 9866: 9858: 9854: 9846: 9842: 9834: 9827: 9819: 9815: 9808: 9791: 9790: 9786: 9779: 9762: 9761: 9757: 9746: 9742: 9738: 9733: 9732: 9726: 9722: 9717: 9716: 9709: 9707: 9703: 9698: 9651: 9592: 9570: 9569: 9560: 9552: 9549: 9541: 9477: 9473: 9460: 9456: 9439: 9405: 9400: 9399: 9341: 9337: 9324: 9320: 9303: 9269: 9264: 9263: 9256: 9227: 9206: 9202: 9189: 9185: 9168: 9146: 9142: 9121: 9100: 9096: 9083: 9079: 9062: 9040: 9036: 9022: 9021: 8989: 8973: 8969: 8956: 8952: 8929: 8913: 8909: 8896: 8892: 8875: 8867: 8866: 8850: 8845: 8842: 8833: 8818: 8809: 8780: 8762: 8727: 8726: 8711: 8703: 8691: 8683: 8676: 8668: 8661: 8653: 8643: 8622: 8610: 8600: 8584: 8487: 8486: 8449: 8436: 8423: 8410: 8388: 8387: 8380: 8365: 8351: 8346: 8319: 8303: 8290: 8271: 8258: 8227: 8223: 8213: 8203: 8193: 8177: 8164: 8136: 8126: 8116: 8106: 8084: 8059: 8054: 8053: 8023: 8007: 7991: 7978: 7956: 7943: 7912: 7908: 7898: 7888: 7878: 7862: 7849: 7821: 7811: 7801: 7791: 7769: 7741: 7728: 7720: 7719: 7707: 7702: 7663: 7644: 7631: 7618: 7599: 7589: 7579: 7527: 7462: 7449: 7421: 7406: 7396: 7371: 7356: 7346: 7325: 7324: 7294: 7278: 7265: 7247: 7242: 7228: 7212: 7196: 7183: 7162: 7157: 7152: 7151: 7121: 7108: 7092: 7079: 7066: 7053: 7037: 7021: 7008: 6988: 6987: 6960: 6944: 6928: 6915: 6899: 6883: 6867: 6851: 6838: 6822: 6804: 6787: 6771: 6755: 6742: 6726: 6708: 6700: 6699: 6688: 6679: 6678:The variations 6650: 6632: 6617: 6599: 6585: 6584: 6573: 6565: 6561: 6531: 6504: 6484: 6457: 6452: 6451: 6418: 6402: 6386: 6370: 6351: 6335: 6319: 6303: 6285: 6268: 6252: 6236: 6220: 6202: 6197: 6196: 6184: 6179: 6167: 6162: 6153: 6146: 6141: 6088: 6073: 6052: 6037: 6018: 6005: 5992: 5979: 5966: 5961: 5960: 5907: 5892: 5876: 5863: 5850: 5837: 5824: 5819: 5818: 5806: 5799: 5793: 5785: 5776: 5771: 5768:double pendulum 5761:double pendulum 5753: 5751:Double pendulum 5744: 5740: 5736: 5674: 5673: 5607: 5599: 5598: 5594:which becomes, 5568: 5555: 5547: 5523: 5515: 5503: 5493: 5492: 5485: 5478: 5474: 5470: 5437: 5424: 5411: 5320: 5319: 5289: 5281: 5263: 5250: 5242: 5218: 5210: 5198: 5179: 5171: 5153: 5140: 5132: 5108: 5100: 5088: 5078: 5077: 5070: 5066: 5027: 5017: 4979: 4957: 4901: 4900: 4786: 4785: 4778: 4727: 4722: 4721: 4714: 4703: 4699: 4692: 4610: 4609: 4510: 4509: 4502: 4498: 4494: 4487: 4440: 4439: 4430: 4426: 4411: 4360: 4359: 4352: 4345: 4261: 4260: 4253: 4249: 4245: 4241: 4147: 4146: 4139: 4106: 4093: 4080: 4054: 4053: 4046: 4042: 4038: 4023: 4019: 4015: 3989: 3983: 3968: 3961: 3959:Simple pendulum 3948: 3845: 3844: 3834: 3830: 3826: 3818: 3811: 3788: 3777: 3767: 3761: 3754: 3749: 3704: 3679: 3675: 3667: 3655: 3634: 3630: 3622: 3615: 3614: 3604: 3600: 3592: 3553: 3549: 3541: 3526: 3521: 3520: 3514: 3510: 3499: 3460: 3443: 3433: 3411: 3401: 3379: 3356: 3348: 3342: 3341: 3336: 3335: 3316: 3276: 3254: 3244: 3222: 3199: 3191: 3185: 3184: 3179: 3178: 3159: 3119: 3109: 3087: 3064: 3056: 3050: 3049: 3044: 3043: 3028: 3014: 3008: 2980: 2967: 2946: 2942: 2929: 2925: 2907: 2903: 2890: 2886: 2883: 2879: 2837: 2819: 2790: 2789: 2782: 2738: 2702: 2683: 2665: 2661: 2648: 2644: 2626: 2622: 2609: 2605: 2602: 2598: 2547: 2523: 2518: 2517: 2511: 2503: 2500: 2492: 2449: 2425: 2415: 2373: 2372: 2362: 2357: 2285: 2284: 2277: 2260: 2255: 2254:and velocities 2252: 2248: 2210: 2197: 2193: 2180: 2176: 2140: 2127: 2123: 2097: 2082: 2077: 2076: 2070: 2062: 2055: 2047: 2044:time derivative 1998: 1955: 1921: 1905: 1895: 1871: 1870: 1861: 1808: 1793: 1788: 1787: 1780: 1776: 1773: 1765: 1758: 1704: 1670: 1645: 1620: 1619: 1609: 1600: 1595: 1577: 1573: 1569: 1555: 1551: 1544: 1537: 1533: 1526: 1522: 1519: 1515: 1512: 1508: 1504: 1463: 1452: 1451: 1445: 1425: 1422: 1414: 1397: 1396: 1383: 1370: 1357: 1339: 1335: 1334: 1323: 1322: 1306: 1293: 1280: 1262: 1258: 1257: 1241: 1228: 1215: 1197: 1187: 1186: 1172:position vector 1163: 1160: 1159: 1158: 1157: 1141: 1126: 1122: 1121: 1120: 1102: 1099: 1091: 1090: 1072: 1069: 1058: 1038: 1037: 1036: 1035: 1031: 1027: 1023: 1022:The arc length 1019: 1018: 1017: 1002: 999: 991: 990: 975: 972: 961: 960: 959: 958: 954: 950: 946: 942: 930: 926: 922: 917: 916: 915: 901: 898: 890: 889: 875: 872: 864: 863: 860: 849: 832:of the system. 788: 747: 734: 733: 726: 725: 724: 599: 591: 590: 570: 524:Circular motion 518: 508: 507: 506: 463: 433: 430: 409: 388: 380: 379: 376: 375: 333: 323: 315: 314: 313: 272: 268:Mechanical work 261: 245: 183: 175: 174: 173: 128: 120: 97: 73: 63: 46: 45: 28: 23: 22: 15: 12: 11: 5: 10178: 10176: 10168: 10167: 10162: 10157: 10152: 10142: 10141: 10138: 10137: 10131: 10118: 10099:978-0750628969 10098: 10085: 10079: 10059: 10054:978-0521575720 10053: 10040: 10034: 10022:Poole, Charles 10014: 10008: 9989: 9986: 9984: 9983: 9974: 9963: 9950: 9937: 9930: 9912: 9900: 9888: 9876: 9864: 9852: 9840: 9825: 9813: 9806: 9784: 9777: 9755: 9739: 9737: 9734: 9731: 9730: 9719: 9718: 9715: 9714: 9700: 9699: 9697: 9694: 9693: 9692: 9687: 9682: 9677: 9672: 9667: 9662: 9657: 9650: 9647: 9646: 9645: 9634: 9631: 9628: 9625: 9622: 9619: 9616: 9613: 9610: 9607: 9604: 9599: 9595: 9590: 9586: 9583: 9580: 9577: 9556: 9545: 9538: 9537: 9526: 9523: 9520: 9517: 9514: 9511: 9508: 9505: 9501: 9493: 9486: 9483: 9476: 9469: 9464: 9459: 9453: 9448: 9443: 9436: 9431: 9428: 9425: 9421: 9417: 9412: 9408: 9393: 9392: 9381: 9378: 9375: 9372: 9369: 9366: 9363: 9360: 9356: 9348: 9344: 9340: 9333: 9328: 9323: 9317: 9312: 9307: 9300: 9295: 9292: 9289: 9285: 9281: 9276: 9272: 9253: 9252: 9241: 9236: 9231: 9226: 9222: 9213: 9209: 9205: 9198: 9193: 9188: 9182: 9177: 9172: 9165: 9160: 9157: 9154: 9150: 9145: 9141: 9138: 9135: 9130: 9125: 9120: 9116: 9107: 9103: 9099: 9092: 9087: 9082: 9076: 9071: 9066: 9059: 9054: 9051: 9048: 9044: 9039: 9035: 9032: 9029: 9015: 9014: 9003: 8998: 8993: 8988: 8980: 8976: 8972: 8965: 8960: 8955: 8949: 8946: 8943: 8938: 8933: 8928: 8920: 8916: 8912: 8905: 8900: 8895: 8889: 8884: 8879: 8874: 8848: 8838: 8814: 8806: 8805: 8794: 8789: 8784: 8779: 8776: 8771: 8766: 8759: 8754: 8751: 8748: 8744: 8740: 8737: 8734: 8707: 8687: 8672: 8642: 8639: 8607:point particle 8581: 8580: 8569: 8565: 8562: 8559: 8556: 8553: 8550: 8547: 8544: 8541: 8538: 8535: 8532: 8529: 8526: 8523: 8520: 8517: 8514: 8511: 8508: 8505: 8502: 8499: 8495: 8480: 8479: 8468: 8464: 8461: 8456: 8452: 8448: 8443: 8439: 8435: 8430: 8426: 8422: 8417: 8413: 8409: 8406: 8402: 8398: 8395: 8364: 8361: 8349: 8343: 8342: 8331: 8326: 8322: 8318: 8315: 8310: 8306: 8302: 8297: 8293: 8289: 8286: 8283: 8278: 8274: 8270: 8265: 8261: 8257: 8254: 8251: 8246: 8239: 8234: 8230: 8220: 8216: 8210: 8206: 8200: 8196: 8192: 8189: 8184: 8180: 8176: 8171: 8167: 8163: 8160: 8157: 8152: 8145: 8142: 8133: 8129: 8123: 8119: 8113: 8109: 8105: 8100: 8093: 8090: 8081: 8076: 8072: 8066: 8062: 8047: 8046: 8035: 8030: 8026: 8022: 8019: 8014: 8010: 8006: 8003: 7998: 7994: 7990: 7985: 7981: 7977: 7974: 7971: 7968: 7963: 7959: 7955: 7950: 7946: 7942: 7939: 7936: 7931: 7924: 7919: 7915: 7905: 7901: 7895: 7891: 7885: 7881: 7877: 7874: 7869: 7865: 7861: 7856: 7852: 7848: 7845: 7842: 7837: 7830: 7827: 7818: 7814: 7808: 7804: 7798: 7794: 7790: 7785: 7778: 7775: 7766: 7761: 7757: 7753: 7748: 7744: 7740: 7735: 7731: 7727: 7705: 7696: 7695: 7684: 7679: 7672: 7669: 7660: 7653: 7650: 7643: 7638: 7634: 7630: 7625: 7621: 7617: 7614: 7611: 7606: 7602: 7596: 7592: 7586: 7582: 7578: 7573: 7568: 7561: 7558: 7549: 7544: 7540: 7534: 7530: 7524: 7521: 7516: 7511: 7506: 7499: 7496: 7487: 7482: 7478: 7474: 7469: 7465: 7461: 7456: 7452: 7448: 7443: 7440: 7435: 7430: 7425: 7420: 7415: 7410: 7403: 7399: 7393: 7390: 7385: 7380: 7375: 7370: 7365: 7360: 7353: 7349: 7343: 7340: 7335: 7332: 7318: 7317: 7306: 7301: 7297: 7293: 7290: 7285: 7281: 7277: 7272: 7268: 7264: 7261: 7254: 7250: 7245: 7240: 7235: 7231: 7227: 7224: 7219: 7215: 7211: 7208: 7203: 7199: 7195: 7190: 7186: 7182: 7179: 7176: 7169: 7165: 7160: 7145: 7144: 7133: 7128: 7124: 7120: 7115: 7111: 7107: 7104: 7099: 7095: 7091: 7086: 7082: 7078: 7073: 7069: 7065: 7060: 7056: 7052: 7049: 7044: 7040: 7036: 7033: 7028: 7024: 7020: 7015: 7011: 7007: 7004: 7001: 6998: 6995: 6981: 6980: 6967: 6963: 6959: 6956: 6951: 6947: 6943: 6940: 6935: 6931: 6927: 6922: 6918: 6914: 6911: 6906: 6902: 6898: 6895: 6890: 6886: 6882: 6879: 6874: 6870: 6866: 6863: 6858: 6854: 6850: 6845: 6841: 6837: 6834: 6829: 6825: 6821: 6818: 6813: 6808: 6803: 6799: 6794: 6790: 6786: 6783: 6778: 6774: 6770: 6767: 6762: 6758: 6754: 6749: 6745: 6741: 6738: 6733: 6729: 6725: 6722: 6717: 6712: 6707: 6684: 6676: 6675: 6664: 6659: 6654: 6649: 6646: 6641: 6636: 6631: 6626: 6621: 6616: 6613: 6608: 6603: 6598: 6595: 6592: 6569: 6558: 6557: 6546: 6543: 6538: 6534: 6530: 6527: 6524: 6521: 6518: 6513: 6508: 6502: 6499: 6496: 6491: 6487: 6483: 6480: 6477: 6474: 6471: 6466: 6461: 6445: 6444: 6433: 6430: 6425: 6421: 6417: 6414: 6409: 6405: 6401: 6398: 6393: 6389: 6385: 6382: 6377: 6373: 6369: 6366: 6363: 6358: 6354: 6350: 6347: 6342: 6338: 6334: 6331: 6326: 6322: 6318: 6315: 6310: 6306: 6302: 6299: 6294: 6289: 6283: 6280: 6275: 6271: 6267: 6264: 6259: 6255: 6251: 6248: 6243: 6239: 6235: 6232: 6227: 6223: 6219: 6216: 6211: 6206: 6182: 6165: 6151: 6144: 6138: 6137: 6126: 6123: 6118: 6113: 6109: 6105: 6102: 6097: 6092: 6087: 6082: 6077: 6072: 6069: 6066: 6061: 6056: 6051: 6046: 6041: 6036: 6033: 6030: 6025: 6021: 6017: 6012: 6008: 6004: 5999: 5995: 5991: 5986: 5982: 5978: 5973: 5969: 5954: 5953: 5942: 5939: 5934: 5929: 5925: 5921: 5916: 5911: 5906: 5901: 5896: 5891: 5888: 5883: 5879: 5875: 5870: 5866: 5862: 5857: 5853: 5849: 5844: 5840: 5836: 5831: 5827: 5804: 5797: 5789: 5774: 5752: 5749: 5730: 5729: 5718: 5715: 5712: 5709: 5706: 5701: 5698: 5693: 5687: 5684: 5667: 5666: 5655: 5652: 5649: 5646: 5643: 5640: 5637: 5634: 5631: 5625: 5622: 5614: 5610: 5606: 5592: 5591: 5580: 5575: 5571: 5567: 5561: 5558: 5553: 5550: 5544: 5535: 5532: 5526: 5521: 5518: 5509: 5506: 5502: 5467: 5466: 5455: 5452: 5449: 5444: 5440: 5436: 5431: 5427: 5423: 5418: 5414: 5409: 5406: 5403: 5400: 5397: 5394: 5391: 5388: 5385: 5382: 5379: 5373: 5370: 5364: 5360: 5357: 5354: 5351: 5348: 5345: 5342: 5336: 5333: 5327: 5313: 5312: 5301: 5295: 5292: 5287: 5284: 5278: 5275: 5270: 5266: 5262: 5256: 5253: 5248: 5245: 5239: 5230: 5227: 5221: 5216: 5213: 5204: 5201: 5197: 5191: 5185: 5182: 5177: 5174: 5168: 5165: 5160: 5156: 5152: 5146: 5143: 5138: 5135: 5129: 5120: 5117: 5111: 5106: 5103: 5094: 5091: 5087: 5073:are given by, 5060: 5059: 5048: 5043: 5036: 5033: 5024: 5020: 5016: 5011: 5008: 5003: 5000: 4995: 4988: 4985: 4978: 4973: 4966: 4963: 4956: 4953: 4948: 4945: 4940: 4936: 4932: 4928: 4924: 4919: 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4298: 4295: 4289: 4283: 4280: 4277: 4271: 4259: 4258: 4257: 4224: 4221: 4215: 4212: 4206: 4203: 4200: 4194: 4191: 4185: 4182: 4179: 4173: 4170: 4167: 4158: 4155: 4145: 4144: 4143: 4122: 4119: 4116: 4111: 4107: 4103: 4098: 4094: 4090: 4085: 4081: 4077: 4071: 4068: 4065: 4059: 4052: 4051: 4050: 4034: 4030: 4026: 4013: 4008: 4000: 3992: 3986: 3979: 3975: 3971: 3965: 3958: 3956: 3954: 3925: 3922: 3919: 3913: 3910: 3904: 3901: 3898: 3892: 3886: 3877: 3873: 3870: 3864: 3861: 3850: 3843: 3842: 3841: 3838: 3824: 3817: 3807: 3803: 3799: 3795: 3791: 3784: 3780: 3770: 3764: 3758: 3751: 3746: 3730: 3726: 3723: 3718: 3711: 3708: 3701: 3693: 3686: 3683: 3671: 3659: 3656: 3652: 3647: 3639: 3635: 3626: 3613: 3612: 3611: 3609: 3598: 3575: 3567: 3560: 3557: 3545: 3536: 3531: 3527: 3519: 3518: 3517: 3508: 3504: 3496: 3480: 3474: 3467: 3464: 3456: 3453: 3448: 3444: 3438: 3434: 3430: 3425: 3418: 3415: 3406: 3402: 3398: 3393: 3386: 3383: 3376: 3371: 3366: 3360: 3357: 3352: 3349: 3343: 3334: 3333: 3332: 3328: 3324: 3320: 3315: 3296: 3290: 3283: 3280: 3273: 3268: 3261: 3258: 3249: 3245: 3241: 3236: 3229: 3226: 3219: 3214: 3209: 3203: 3200: 3195: 3192: 3186: 3177: 3176: 3175: 3171: 3167: 3163: 3158: 3139: 3133: 3126: 3123: 3114: 3110: 3106: 3101: 3094: 3091: 3084: 3079: 3074: 3068: 3065: 3060: 3057: 3051: 3042: 3041: 3040: 3036: 3032: 3027: 3022: 3020: 3011: 2991: 2985: 2981: 2977: 2972: 2968: 2964: 2960: 2951: 2947: 2936: 2920: 2912: 2908: 2897: 2880: 2874: 2869: 2866: 2863: 2860: 2857: 2853: 2849: 2844: 2834: 2831: 2826: 2816: 2813: 2808: 2803: 2799: 2795: 2788: 2787: 2786: 2780: 2775: 2773: 2768: 2764: 2760: 2756: 2753: 2749: 2745: 2741: 2721: 2716: 2709: 2706: 2697: 2690: 2687: 2679: 2670: 2666: 2655: 2639: 2631: 2627: 2616: 2599: 2593: 2588: 2585: 2582: 2579: 2576: 2572: 2568: 2563: 2556: 2544: 2539: 2532: 2516: 2515: 2514: 2510: 2506: 2499: 2495: 2490: 2471: 2465: 2458: 2446: 2441: 2434: 2420: 2416: 2410: 2405: 2402: 2399: 2395: 2389: 2386: 2381: 2378: 2371: 2370: 2369: 2367: 2359: 2354: 2352: 2334: 2330: 2327: 2321: 2318: 2312: 2301: 2290: 2283: 2282: 2281: 2274: 2272: 2270: 2265: 2261: 2230: 2224: 2217: 2214: 2202: 2198: 2187: 2169: 2164: 2161: 2158: 2154: 2150: 2144: 2141: 2134: 2124: 2118: 2113: 2106: 2094: 2089: 2075: 2074: 2073: 2069: 2065: 2060: 2054: 2050: 2045: 2020: 2012: 2005: 2002: 1992: 1989: 1983: 1977: 1969: 1962: 1959: 1949: 1943: 1935: 1928: 1925: 1915: 1909: 1906: 1896: 1890: 1884: 1869: 1868: 1867: 1864: 1858: 1841: 1831: 1815: 1805: 1800: 1786: 1785: 1784: 1772: 1768: 1762: 1756: 1752: 1748: 1744: 1743: 1717: 1709: 1705: 1698: 1695: 1689: 1683: 1675: 1671: 1664: 1658: 1650: 1646: 1639: 1633: 1618: 1617: 1616: 1615: 1605: 1601: 1593: 1588: 1584: 1580: 1566: 1562: 1558: 1548: 1541: 1531: 1487: 1484: 1478: 1475: 1470: 1457: 1450: 1449: 1448: 1443: 1439: 1438: 1432: 1428: 1421: 1417: 1388: 1384: 1380: 1375: 1371: 1367: 1362: 1358: 1351: 1346: 1331: 1327: 1319: 1311: 1307: 1303: 1298: 1294: 1290: 1285: 1281: 1274: 1269: 1254: 1246: 1242: 1238: 1233: 1229: 1225: 1220: 1216: 1209: 1204: 1185: 1184: 1183: 1181: 1177: 1173: 1169: 1153: 1149: 1145: 1140: 1134: 1130: 1117: 1113: 1109: 1105: 1097: 1087: 1083: 1079: 1075: 1067: 1055: 1053: 1051: 1047: 1043: 1013: 1009: 1005: 997: 986: 982: 978: 970: 938: 934: 912: 908: 904: 896: 886: 882: 878: 870: 858: 846: 844: 842: 838: 833: 831: 827: 822: 819: 817: 813: 810:are the time 809: 805: 801: 797: 785: 780: 778: 773: 771: 766: 765: 763: 762: 756: 746: 743: 738: 732: 731: 730: 729: 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: 606: 603: 602: 595: 594: 587: 583: 579: 575: 572: 571: 567: 564: 562: 559: 557: 554: 552: 549: 545: 542: 541: 540: 537: 535: 532: 530: 527: 525: 522: 521: 517: 512: 511: 503: 500: 498: 495: 491: 488: 486: 483: 482: 481: 478: 476: 473: 471: 468: 466: 461: 458: 454: 451: 450: 446: 443: 440: 436: 432: 431: 427: 424: 422: 419: 417: 414: 412: 407: 405: 402: 400: 397: 395: 392: 391: 384: 383: 372: 369: 367: 364: 362: 359: 357: 354: 352: 349: 347: 344: 343: 341: 340: 335: 332: 331: 326: 325: 319: 318: 310: 307: 305: 302: 300: 297: 295: 292: 290: 287: 285: 282: 280: 277: 275: 271: 269: 266: 264: 260: 258: 255: 252: 248: 244: 242: 239: 237: 234: 232: 229: 227: 224: 220: 217: 215: 212: 211: 210: 207: 205: 202: 200: 197: 195: 192: 190: 187: 186: 179: 178: 170: 167: 165: 162: 160: 157: 155: 152: 150: 147: 145: 142: 140: 137: 135: 132: 131: 124: 123: 117: 114: 112: 109: 107: 104: 103: 100: 96: 77: 74: 64: 58: 44: 43: 40: 36: 32: 31: 19: 10160:Rigid bodies 10122: 10089: 10066: 10044: 10025: 9995: 9977: 9966: 9953: 9940: 9921: 9915: 9903: 9898:, p. 25 9891: 9879: 9874:, p. 15 9867: 9862:, p. 13 9855: 9843: 9823:, p. 12 9816: 9797: 9787: 9768: 9758: 9743: 9723: 9704: 9665:Virtual work 9564: 9557: 9553: 9546: 9542: 9539: 9394: 9254: 9016: 8857: 8853: 8846: 8839: 8835: 8831: 8824: 8820: 8815: 8811: 8807: 8717: 8713: 8708: 8704: 8697: 8693: 8688: 8684: 8681: 8673: 8669: 8663: 8655: 8649:virtual work 8646: 8644: 8632: 8628: 8624: 8616: 8612: 8601: 8590: 8586: 8582: 8481: 8374: 8354: 8347: 8344: 8048: 7710: 7703: 7697: 7319: 7146: 6982: 6690: 6685: 6681: 6677: 6580:is given by 6575: 6570: 6566: 6559: 6446: 6187: 6180: 6177: 6170: 6163: 6156: 6149: 6142: 6139: 5955: 5809: 5802: 5795: 5790: 5786: 5779: 5772: 5765: 5734: 5731: 5668: 5593: 5483: 5468: 5314: 5061: 4895: 4776: 4705: 4694: 4690: 4604: 4489: 4485: 4435:is given by 4431: 4423:virtual work 4420: 4409: 4350: 4343: 4256:, such that 4239: 4137: 4032: 4028: 4024: 4009: 4005: 3990: 3984: 3977: 3973: 3969: 3952: 3946: 3839: 3822: 3805: 3801: 3797: 3793: 3789: 3782: 3778: 3775: 3768: 3762: 3596: 3590: 3502: 3500: 3326: 3322: 3318: 3311: 3169: 3165: 3161: 3154: 3034: 3030: 3023: 3009: 3006: 2779:line element 2776: 2769: 2762: 2758: 2754: 2751: 2747: 2743: 2739: 2736: 2508: 2504: 2497: 2493: 2486: 2363: 2349: 2278: 2268: 2263: 2256: 2245: 2067: 2063: 2052: 2048: 2041: 1862: 1859: 1856: 1775:of particle 1770: 1766: 1763: 1740: 1738: 1603: 1596: 1591: 1586: 1582: 1578: 1564: 1560: 1556: 1546: 1542: 1529: 1502: 1441: 1435: 1430: 1426: 1419: 1415: 1412: 1161: 1151: 1147: 1143: 1132: 1128: 1115: 1111: 1107: 1103: 1085: 1081: 1077: 1073: 1045: 1039: 1011: 1007: 1003: 984: 980: 976: 936: 932: 910: 906: 902: 884: 880: 876: 834: 823: 820: 807: 799: 793: 584: / 580: / 578:displacement 576: / 437: / 399:Displacement 337: 328: 322:Formulations 309:Virtual work 249: / 189:Acceleration 182:Fundamentals 9910:, p. 8 9680:Mass matrix 8856:= 1, 2, …, 8823:= 1, 2, …, 8716:= 1, 2, …, 8696:= 1, 2, …, 4717:, given by 4344:The use of 3810:, in which 2489:dot product 1747:arc lengths 1429:= 1, 2, …, 1052:equations. 841:phase space 812:derivatives 720:von Neumann 387:Core topics 10144:Categories 10080:1860944248 9971:Torby 1984 9884:Torby 1984 9848:Torby 1984 9736:References 3816:arc length 3019:Lagrangian 2364:The total 1050:constraint 655:d'Alembert 635:Maupertuis 598:Scientists 480:Rigid body 154:Kinematics 10108:cite book 10090:Mechanics 9624:… 9589:⇒ 9576:δ 9516:… 9485:˙ 9475:∂ 9458:∂ 9452:⋅ 9420:∑ 9371:… 9339:∂ 9322:∂ 9316:⋅ 9284:∑ 9225:δ 9204:∂ 9187:∂ 9181:⋅ 9149:∑ 9137:… 9119:δ 9098:∂ 9081:∂ 9075:⋅ 9043:∑ 9028:δ 8987:δ 8971:∂ 8954:∂ 8945:… 8927:δ 8911:∂ 8894:∂ 8873:δ 8778:δ 8775:⋅ 8743:∑ 8733:δ 8583:in which 8558:ϕ 8552:θ 8537:ϕ 8531:θ 8516:ϕ 8510:θ 8447:− 8321:θ 8317:⁡ 8288:− 8273:θ 8269:− 8260:θ 8253:⁡ 8238:˙ 8229:θ 8179:θ 8175:− 8166:θ 8159:⁡ 8144:¨ 8141:θ 8092:¨ 8089:θ 8025:θ 8021:⁡ 7973:− 7958:θ 7954:− 7945:θ 7938:⁡ 7923:˙ 7914:θ 7864:θ 7860:− 7851:θ 7844:⁡ 7829:¨ 7826:θ 7777:¨ 7774:θ 7715:given by 7671:˙ 7668:θ 7652:˙ 7649:θ 7633:θ 7629:− 7620:θ 7613:⁡ 7560:˙ 7557:θ 7498:˙ 7495:θ 7419:⋅ 7369:⋅ 7296:θ 7292:⁡ 7263:− 7249:θ 7230:θ 7226:⁡ 7178:− 7164:θ 7123:θ 7119:δ 7110:θ 7106:⁡ 7077:− 7068:θ 7064:δ 7055:θ 7051:⁡ 7003:− 6994:δ 6962:θ 6958:δ 6946:θ 6942:⁡ 6917:θ 6913:⁡ 6885:θ 6881:δ 6869:θ 6865:⁡ 6840:θ 6836:⁡ 6802:δ 6789:θ 6785:δ 6773:θ 6769:⁡ 6744:θ 6740:⁡ 6706:δ 6648:δ 6645:⋅ 6615:δ 6612:⋅ 6591:δ 6529:− 6482:− 6420:θ 6416:⁡ 6400:− 6388:θ 6384:⁡ 6353:θ 6349:⁡ 6333:− 6321:θ 6317:⁡ 6270:θ 6266:⁡ 6250:− 6238:θ 6234:⁡ 6104:− 6086:− 6068:⋅ 6050:− 5920:− 5905:⋅ 5711:θ 5708:⁡ 5686:¨ 5683:θ 5651:θ 5648:⁡ 5633:− 5624:¨ 5621:θ 5574:θ 5560:θ 5557:∂ 5549:∂ 5543:− 5534:˙ 5531:θ 5525:∂ 5517:∂ 5435:− 5393:λ 5381:− 5372:¨ 5344:λ 5335:¨ 5291:∂ 5283:∂ 5277:λ 5252:∂ 5244:∂ 5238:− 5229:˙ 5220:∂ 5212:∂ 5181:∂ 5173:∂ 5167:λ 5142:∂ 5134:∂ 5128:− 5119:˙ 5110:∂ 5102:∂ 5035:˙ 5032:θ 4987:˙ 4965:˙ 4931:⋅ 4875:˙ 4872:θ 4863:θ 4860:⁡ 4848:θ 4845:⁡ 4824:˙ 4809:˙ 4759:θ 4756:⁡ 4741:− 4733:θ 4673:θ 4670:δ 4664:θ 4658:⁡ 4643:− 4634:δ 4625:− 4616:δ 4587:θ 4584:δ 4578:θ 4575:⁡ 4563:θ 4560:⁡ 4539:δ 4530:δ 4516:δ 4463:δ 4460:⋅ 4446:δ 4383:− 4323:θ 4320:⁡ 4311:− 4305:θ 4302:⁡ 4216:˙ 4195:˙ 4159:˙ 4104:− 4010:A simple 3712:˙ 3687:˙ 3677:∂ 3669:∂ 3632:∂ 3624:∂ 3561:˙ 3551:∂ 3543:∂ 3468:˙ 3465:φ 3457:θ 3454:⁡ 3419:˙ 3416:θ 3387:˙ 3284:˙ 3262:˙ 3259:θ 3230:˙ 3127:˙ 3124:θ 3095:˙ 2944:∂ 2927:∂ 2921:⋅ 2905:∂ 2888:∂ 2854:∑ 2832:⋅ 2710:˙ 2691:˙ 2663:∂ 2646:∂ 2640:⋅ 2624:∂ 2607:∂ 2573:∑ 2557:˙ 2545:⋅ 2533:˙ 2459:˙ 2447:⋅ 2435:˙ 2396:∑ 2313:˙ 2218:˙ 2195:∂ 2178:∂ 2155:∑ 2107:˙ 2006:˙ 1990:… 1963:˙ 1929:˙ 1885:˙ 1696:… 1332:⋮ 1046:dependent 925:or angle 700:Liouville 582:frequency 502:Vibration 219:potential 144:Continuum 139:Celestial 116:Textbooks 9649:See also 8595:are the 4012:pendulum 3747:Examples 755:Category 680:Hamilton 665:Lagrange 660:Clairaut 625:Horrocks 586:velocity 556:Pendulum 544:reactive 516:Rotation 485:dynamics 435:Inertial 421:Friction 304:Velocity 279:Momentum 159:Kinetics 149:Dynamics 127:Branches 111:Timeline 8357:= 1, 2) 7713:= 1, 2) 6693:= 1, 2) 6578:= 1, 2) 6190:= 1, 2) 6173:= 1, 2) 6159:= 1, 2) 5782:= 1, 2) 4698:is the 4414:is the 2057:is the 715:Koopman 675:Poisson 670:Laplace 615:Huygens 610:Galileo 455: ( 394:Damping 247:Inertia 241:Impulse 214:kinetic 164:Statics 134:Applied 106:History 10129:  10096:  10077:  10051:  10032:  10006:  9928:  9804:  9775:  9540:where 9259:terms 8808:where 6560:where 5812:= 1, 2 5784:, let 4410:where 3312:in 3D 3155:in 3D 1996:  1987:  1953:  1702:  1693:  1668:  1568:. (In 1424:where 1170:, the 753:  705:Appell 690:Cauchy 685:Jacobi 630:Halley 620:Newton 605:Kepler 457:linear 453:Motion 299:Torque 274:Moment 209:Energy 199:Couple 9696:Notes 8862:then 3980:) = 0 3785:) = 0 3595:does 1614:tuple 1440:is a 1176:tuple 1118:) = 0 1088:) = 0 1014:) = 0 987:) = 0 913:) = 0 887:) = 0 710:Gibbs 695:Routh 650:Euler 289:Speed 284:Space 226:Force 10127:ISBN 10114:link 10094:ISBN 10075:ISBN 10049:ISBN 10030:ISBN 10004:ISBN 9926:ISBN 9802:ISBN 9773:ISBN 9255:The 9017:and 8645:The 8049:and 5956:and 5743:and 5477:and 5069:and 4896:so, 4497:and 4421:The 4252:and 4045:and 3833:and 3501:The 1514:and 294:Time 257:Mass 8677:= 0 8658:= 0 8314:sin 8250:sin 8156:cos 8018:sin 7935:sin 7841:cos 7610:cos 7289:sin 7223:sin 7103:sin 7048:sin 6939:sin 6910:cos 6862:sin 6833:cos 6766:sin 6737:cos 6413:cos 6381:sin 6346:cos 6314:sin 6263:cos 6231:sin 5808:), 5794:= ( 5705:sin 5669:or 5645:sin 4857:sin 4842:cos 4753:sin 4655:sin 4572:sin 4557:cos 4317:cos 4299:sin 4027:= ( 3953:and 3823:one 3800:), 3792:= ( 3597:not 3445:sin 2061:of 1559:= 3 1530:one 1178:in 953:or 945:or 839:on 794:In 10146:: 10110:}} 10106:{{ 10073:. 10020:; 10002:. 9828:^ 9796:. 9767:. 9750:, 9562:. 8679:. 8631:, 8627:, 8615:, 8589:, 6148:, 6125:0. 5801:, 5759:A 5717:0. 5481:. 5473:, 4505:, 4418:. 4225:0. 4031:, 3976:, 3808:)) 3331:, 3325:, 3321:, 3174:, 3168:, 3164:, 3039:, 3033:, 3021:. 3010:dt 2785:, 2767:. 2761:, 2759:dt 2750:, 2742:= 2271:. 2264:dt 2257:dq 1585:− 1583:ND 1581:= 1574:ND 1563:− 1182:: 1150:, 1146:, 1131:, 1114:, 1110:, 1084:, 1080:, 1010:, 983:, 935:, 909:, 883:, 843:. 818:. 798:, 10135:. 10116:) 10102:. 10083:. 10057:. 10038:. 10012:. 9948:. 9934:. 9810:. 9781:. 9710:k 9633:. 9630:n 9627:, 9621:, 9618:1 9615:= 9612:i 9609:, 9606:0 9603:= 9598:i 9594:F 9585:0 9582:= 9579:W 9558:j 9554:F 9547:j 9543:v 9525:, 9522:n 9519:, 9513:, 9510:1 9507:= 9504:i 9500:, 9492:i 9482:q 9468:j 9463:v 9447:j 9442:F 9435:m 9430:1 9427:= 9424:j 9416:= 9411:i 9407:F 9380:, 9377:n 9374:, 9368:, 9365:1 9362:= 9359:i 9355:, 9347:i 9343:q 9332:j 9327:r 9311:j 9306:F 9299:m 9294:1 9291:= 9288:j 9280:= 9275:i 9271:F 9257:n 9240:. 9235:n 9230:q 9221:) 9212:n 9208:q 9197:j 9192:r 9176:j 9171:F 9164:m 9159:1 9156:= 9153:j 9144:( 9140:+ 9134:+ 9129:1 9124:q 9115:) 9106:1 9102:q 9091:j 9086:r 9070:j 9065:F 9058:m 9053:1 9050:= 9047:j 9038:( 9034:= 9031:W 9002:, 8997:n 8992:q 8979:n 8975:q 8964:j 8959:r 8948:+ 8942:+ 8937:1 8932:q 8919:1 8915:q 8904:j 8899:r 8888:= 8883:j 8878:r 8860:) 8858:n 8854:i 8852:( 8849:i 8847:q 8840:j 8836:r 8834:δ 8827:) 8825:m 8821:j 8819:( 8816:j 8812:r 8810:δ 8793:. 8788:j 8783:r 8770:j 8765:F 8758:m 8753:1 8750:= 8747:j 8739:= 8736:W 8720:) 8718:m 8714:j 8712:( 8709:j 8705:r 8700:) 8698:m 8694:j 8692:( 8689:j 8685:F 8674:i 8670:F 8664:r 8662:δ 8656:W 8654:δ 8635:) 8633:z 8629:y 8625:x 8623:( 8619:) 8617:φ 8613:θ 8611:( 8602:r 8593:) 8591:φ 8587:θ 8585:( 8568:, 8564:) 8561:) 8555:, 8549:( 8546:z 8543:, 8540:) 8534:, 8528:( 8525:y 8522:, 8519:) 8513:, 8507:( 8504:x 8501:( 8498:= 8494:r 8467:, 8463:0 8460:= 8455:2 8451:l 8442:2 8438:z 8434:+ 8429:2 8425:y 8421:+ 8416:2 8412:x 8408:= 8405:) 8401:r 8397:( 8394:f 8381:l 8355:i 8353:( 8350:i 8348:θ 8330:. 8325:2 8309:2 8305:L 8301:g 8296:2 8292:m 8285:= 8282:) 8277:1 8264:2 8256:( 8245:2 8233:1 8219:2 8215:L 8209:1 8205:L 8199:2 8195:m 8191:+ 8188:) 8183:1 8170:2 8162:( 8151:1 8132:2 8128:L 8122:1 8118:L 8112:2 8108:m 8104:+ 8099:2 8080:2 8075:2 8071:L 8065:2 8061:m 8034:, 8029:1 8013:1 8009:L 8005:g 8002:) 7997:2 7993:m 7989:+ 7984:1 7980:m 7976:( 7970:= 7967:) 7962:2 7949:1 7941:( 7930:2 7918:2 7904:2 7900:L 7894:1 7890:L 7884:2 7880:m 7876:+ 7873:) 7868:1 7855:2 7847:( 7836:2 7817:2 7813:L 7807:1 7803:L 7797:2 7793:m 7789:+ 7784:1 7765:2 7760:1 7756:L 7752:) 7747:2 7743:m 7739:+ 7734:1 7730:m 7726:( 7711:i 7709:( 7706:i 7704:θ 7683:. 7678:2 7659:1 7642:) 7637:1 7624:2 7616:( 7605:2 7601:L 7595:1 7591:L 7585:2 7581:m 7577:+ 7572:2 7567:2 7548:2 7543:2 7539:L 7533:2 7529:m 7523:2 7520:1 7515:+ 7510:2 7505:1 7486:2 7481:1 7477:L 7473:) 7468:2 7464:m 7460:+ 7455:1 7451:m 7447:( 7442:2 7439:1 7434:= 7429:2 7424:v 7414:2 7409:v 7402:2 7398:m 7392:2 7389:1 7384:+ 7379:1 7374:v 7364:1 7359:v 7352:1 7348:m 7342:2 7339:1 7334:= 7331:T 7305:. 7300:2 7284:2 7280:L 7276:g 7271:2 7267:m 7260:= 7253:2 7244:F 7239:, 7234:1 7218:1 7214:L 7210:g 7207:) 7202:2 7198:m 7194:+ 7189:1 7185:m 7181:( 7175:= 7168:1 7159:F 7132:, 7127:2 7114:2 7098:2 7094:L 7090:g 7085:2 7081:m 7072:1 7059:1 7043:1 7039:L 7035:g 7032:) 7027:2 7023:m 7019:+ 7014:1 7010:m 7006:( 7000:= 6997:W 6966:2 6955:) 6950:2 6934:2 6930:L 6926:, 6921:2 6905:2 6901:L 6897:( 6894:+ 6889:1 6878:) 6873:1 6857:1 6853:L 6849:, 6844:1 6828:1 6824:L 6820:( 6817:= 6812:2 6807:r 6798:, 6793:1 6782:) 6777:1 6761:1 6757:L 6753:, 6748:1 6732:1 6728:L 6724:( 6721:= 6716:1 6711:r 6691:i 6689:( 6686:i 6682:r 6680:δ 6663:. 6658:2 6653:r 6640:2 6635:F 6630:+ 6625:1 6620:r 6607:1 6602:F 6597:= 6594:W 6576:i 6574:( 6571:i 6567:r 6562:g 6545:) 6542:g 6537:2 6533:m 6526:, 6523:0 6520:( 6517:= 6512:2 6507:F 6501:, 6498:) 6495:g 6490:1 6486:m 6479:, 6476:0 6473:( 6470:= 6465:1 6460:F 6432:. 6429:) 6424:2 6408:2 6404:L 6397:, 6392:2 6376:2 6372:L 6368:( 6365:+ 6362:) 6357:1 6341:1 6337:L 6330:, 6325:1 6309:1 6305:L 6301:( 6298:= 6293:2 6288:r 6282:, 6279:) 6274:1 6258:1 6254:L 6247:, 6242:1 6226:1 6222:L 6218:( 6215:= 6210:1 6205:r 6188:i 6186:( 6183:i 6181:θ 6171:i 6169:( 6166:i 6164:λ 6157:i 6155:( 6152:i 6150:y 6145:i 6143:x 6122:= 6117:2 6112:2 6108:L 6101:) 6096:1 6091:r 6081:2 6076:r 6071:( 6065:) 6060:1 6055:r 6045:2 6040:r 6035:( 6032:= 6029:) 6024:2 6020:y 6016:, 6011:2 6007:x 6003:, 5998:1 5994:y 5990:, 5985:1 5981:x 5977:( 5972:2 5968:f 5941:0 5938:= 5933:2 5928:1 5924:L 5915:1 5910:r 5900:1 5895:r 5890:= 5887:) 5882:2 5878:y 5874:, 5869:2 5865:x 5861:, 5856:1 5852:y 5848:, 5843:1 5839:x 5835:( 5830:1 5826:f 5810:i 5805:i 5803:y 5798:i 5796:x 5791:i 5787:r 5780:i 5778:( 5775:i 5773:m 5745:y 5741:x 5737:θ 5714:= 5700:L 5697:g 5692:+ 5654:, 5642:L 5639:g 5636:m 5630:= 5613:2 5609:L 5605:m 5579:, 5570:F 5566:= 5552:T 5520:T 5508:t 5505:d 5501:d 5486:θ 5479:λ 5475:y 5471:x 5454:, 5451:0 5448:= 5443:2 5439:L 5430:2 5426:y 5422:+ 5417:2 5413:x 5408:, 5405:) 5402:y 5399:2 5396:( 5390:+ 5387:g 5384:m 5378:= 5369:y 5363:m 5359:, 5356:) 5353:x 5350:2 5347:( 5341:= 5332:x 5326:m 5300:. 5294:y 5286:f 5274:+ 5269:y 5265:F 5261:= 5255:y 5247:T 5226:y 5215:T 5203:t 5200:d 5196:d 5190:, 5184:x 5176:f 5164:+ 5159:x 5155:F 5151:= 5145:x 5137:T 5116:x 5105:T 5093:t 5090:d 5086:d 5071:y 5067:x 5047:. 5042:2 5023:2 5019:L 5015:m 5010:2 5007:1 5002:= 4999:) 4994:2 4984:y 4977:+ 4972:2 4962:x 4955:( 4952:m 4947:2 4944:1 4939:= 4935:v 4927:v 4923:m 4918:2 4915:1 4910:= 4907:T 4881:, 4866:) 4854:L 4851:, 4839:L 4836:( 4833:= 4830:) 4821:y 4815:, 4806:x 4800:( 4797:= 4793:v 4779:T 4762:. 4750:L 4747:g 4744:m 4738:= 4729:F 4715:θ 4706:θ 4704:δ 4700:y 4695:y 4693:δ 4676:. 4667:) 4661:( 4652:L 4649:g 4646:m 4640:= 4637:y 4631:g 4628:m 4622:= 4619:W 4590:. 4581:) 4569:L 4566:, 4554:L 4551:( 4548:= 4545:) 4542:y 4536:, 4533:x 4527:( 4524:= 4520:r 4503:θ 4499:y 4495:x 4490:r 4488:δ 4471:. 4467:r 4456:F 4452:= 4449:W 4432:r 4427:m 4412:g 4395:, 4392:) 4389:g 4386:m 4380:, 4377:0 4374:( 4371:= 4367:F 4353:m 4346:θ 4329:. 4326:) 4314:L 4308:, 4296:L 4293:( 4290:= 4287:) 4284:y 4281:, 4278:x 4275:( 4272:= 4268:r 4254:y 4250:x 4246:M 4242:θ 4222:= 4213:y 4207:y 4204:2 4201:+ 4192:x 4186:x 4183:2 4180:= 4177:) 4174:y 4171:, 4168:x 4165:( 4156:f 4140:M 4123:, 4120:0 4117:= 4112:2 4108:L 4099:2 4095:y 4091:+ 4086:2 4082:x 4078:= 4075:) 4072:y 4069:, 4066:x 4063:( 4060:f 4047:y 4043:x 4039:y 4035:) 4033:y 4029:x 4025:r 4020:L 4016:M 3991:N 3985:C 3978:y 3974:x 3972:( 3970:f 3949:t 3932:) 3929:) 3926:t 3923:, 3920:s 3917:( 3914:y 3911:, 3908:) 3905:t 3902:, 3899:s 3896:( 3893:x 3890:( 3887:= 3883:r 3878:, 3874:0 3871:= 3868:) 3865:t 3862:, 3858:r 3854:( 3851:f 3835:y 3831:x 3827:s 3819:s 3812:s 3806:s 3804:( 3802:y 3798:s 3796:( 3794:x 3790:r 3783:r 3781:( 3779:f 3769:N 3763:C 3731:. 3727:0 3724:= 3719:i 3709:p 3702:= 3694:i 3684:q 3672:L 3660:t 3657:d 3653:d 3648:= 3640:i 3636:q 3627:L 3603:i 3601:q 3593:L 3576:. 3568:i 3558:q 3546:L 3537:= 3532:i 3528:p 3513:i 3511:q 3505:" 3481:. 3475:2 3449:2 3439:2 3435:r 3431:+ 3426:2 3407:2 3403:r 3399:+ 3394:2 3384:r 3377:= 3372:2 3367:) 3361:t 3358:d 3353:s 3350:d 3344:( 3329:) 3327:φ 3323:θ 3319:r 3317:( 3297:, 3291:2 3281:z 3274:+ 3269:2 3250:2 3246:r 3242:+ 3237:2 3227:r 3220:= 3215:2 3210:) 3204:t 3201:d 3196:s 3193:d 3187:( 3172:) 3170:z 3166:θ 3162:r 3160:( 3140:, 3134:2 3115:2 3111:r 3107:+ 3102:2 3092:r 3085:= 3080:2 3075:) 3069:t 3066:d 3061:s 3058:d 3052:( 3037:) 3035:θ 3031:r 3029:( 3015:k 2992:, 2986:j 2982:q 2978:d 2973:i 2969:q 2965:d 2961:) 2952:j 2948:q 2937:k 2932:r 2913:i 2909:q 2898:k 2893:r 2881:( 2875:n 2870:1 2867:= 2864:j 2861:, 2858:i 2850:= 2845:k 2840:r 2835:d 2827:k 2822:r 2817:d 2814:= 2809:2 2804:k 2800:s 2796:d 2783:k 2765:) 2763:t 2757:/ 2755:q 2752:d 2748:q 2746:( 2744:T 2740:T 2722:, 2717:j 2707:q 2698:i 2688:q 2680:) 2671:j 2667:q 2656:k 2651:r 2632:i 2628:q 2617:k 2612:r 2600:( 2594:n 2589:1 2586:= 2583:j 2580:, 2577:i 2569:= 2564:k 2553:r 2540:k 2529:r 2509:k 2505:r 2498:k 2494:v 2472:, 2466:k 2455:r 2442:k 2431:r 2421:k 2417:m 2411:N 2406:1 2403:= 2400:k 2390:2 2387:1 2382:= 2379:T 2335:, 2331:0 2328:= 2325:) 2322:t 2319:, 2309:q 2302:, 2298:q 2294:( 2291:g 2262:/ 2259:j 2251:j 2249:q 2231:. 2225:j 2215:q 2203:j 2199:q 2188:k 2183:r 2170:n 2165:1 2162:= 2159:j 2151:= 2145:t 2142:d 2135:k 2130:r 2125:d 2119:= 2114:k 2103:r 2095:= 2090:k 2085:v 2068:k 2064:r 2053:k 2049:v 2027:) 2024:) 2021:t 2018:( 2013:n 2003:q 1993:, 1984:, 1981:) 1978:t 1975:( 1970:2 1960:q 1950:, 1947:) 1944:t 1941:( 1936:1 1926:q 1919:( 1916:= 1910:t 1907:d 1901:q 1897:d 1891:= 1881:q 1863:q 1842:, 1838:) 1835:) 1832:t 1829:( 1825:q 1821:( 1816:k 1811:r 1806:= 1801:k 1796:r 1781:n 1777:k 1771:k 1767:r 1759:n 1724:) 1721:) 1718:t 1715:( 1710:n 1706:q 1699:, 1690:, 1687:) 1684:t 1681:( 1676:2 1672:q 1665:, 1662:) 1659:t 1656:( 1651:1 1647:q 1643:( 1640:= 1637:) 1634:t 1631:( 1627:q 1612:- 1610:n 1606:) 1604:t 1602:( 1599:j 1597:q 1587:C 1579:n 1570:D 1565:C 1561:N 1557:n 1552:C 1547:N 1545:3 1538:C 1534:C 1525:k 1523:y 1518:k 1516:z 1511:k 1509:x 1505:t 1488:0 1485:= 1482:) 1479:t 1476:, 1471:k 1466:r 1461:( 1458:f 1446:k 1431:N 1427:k 1420:k 1416:r 1394:) 1389:N 1385:z 1381:, 1376:N 1372:y 1368:, 1363:N 1359:x 1355:( 1352:= 1347:N 1342:r 1320:, 1317:) 1312:2 1308:z 1304:, 1299:2 1295:y 1291:, 1286:2 1282:x 1278:( 1275:= 1270:2 1265:r 1255:, 1252:) 1247:1 1243:z 1239:, 1234:1 1230:y 1226:, 1221:1 1217:x 1213:( 1210:= 1205:1 1200:r 1164:N 1154:) 1152:z 1148:y 1144:x 1142:( 1135:) 1133:v 1129:u 1127:( 1116:z 1112:y 1108:x 1106:( 1104:S 1086:z 1082:y 1078:x 1076:( 1074:F 1034:. 1032:θ 1028:θ 1024:s 1012:y 1008:x 1006:( 1004:C 985:y 981:x 979:( 977:F 957:. 955:θ 951:s 947:y 943:x 939:) 937:y 933:x 931:( 927:θ 923:s 911:y 907:x 905:( 903:C 885:y 881:x 879:( 877:F 783:e 776:t 769:v 459:) 78:t 75:d 69:p 65:d 59:= 54:F 20:)

Index

Generalized coordinate
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
Mechanical work

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