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GENERALIZED COORDINATES

  • Generalized coordinates
  • System configuration relative to another

    configuration. The generalized velocities are the time derivatives of the generalized coordinates of the system. The adjective "generalized" distinguishes

    Generalized coordinates

    Generalized_coordinates

  • Barycentric coordinate system
  • Coordinate system that is defined by points instead of vectors

    point not having unique generalized barycentric coordinates except when P is a simplex. Dual to generalized barycentric coordinates are slack variables,

    Barycentric coordinate system

    Barycentric coordinate system

    Barycentric_coordinate_system

  • Lagrangian mechanics
  • Formulation of classical mechanics

    this vk, the kinetic energy in generalized coordinates depends on the generalized velocities, generalized coordinates, and time if the position vectors

    Lagrangian mechanics

    Lagrangian mechanics

    Lagrangian_mechanics

  • Canonical coordinates
  • Sets of coordinates on phase space which can be used to describe a physical system

    details. As Hamiltonian mechanics are generalized by symplectic geometry and canonical transformations are generalized by contact transformations, so the

    Canonical coordinates

    Canonical_coordinates

  • Analytical mechanics
  • Overview of mechanics based on the least action principle

    the generalized coordinates and velocities (q, q̇) with (q, p); the generalized coordinates and the generalized momentums conjugate to the generalized coordinates:

    Analytical mechanics

    Analytical_mechanics

  • Momentum
  • Property of a mass in motion

    symbol Π. In this mathematical framework, a generalized momentum is associated with the generalized coordinates. Its components are defined as p j = ∂ L

    Momentum

    Momentum

    Momentum

  • Generalized forces
  • Concept in Lagrangian mechanics

    mechanics (particularly Lagrangian mechanics), generalized forces are conjugate to generalized coordinates. They are obtained from the applied forces Fi

    Generalized forces

    Generalized_forces

  • Coordinate system
  • Method for specifying point positions

    Plücker coordinates are a way of representing lines in 3D Euclidean space using a six-tuple of numbers as homogeneous coordinates. Generalized coordinates are

    Coordinate system

    Coordinate system

    Coordinate_system

  • Action-angle coordinates
  • Method of solution for certain mechanical problems

    coordinates, which we denote as w {\displaystyle \mathbf {w} } (the action angles, which are the generalized coordinates) and their new generalized momenta

    Action-angle coordinates

    Action-angle_coordinates

  • Generalized filtering
  • formulated in generalized coordinates of motion. Note that "generalized coordinates of motion" are related to—but distinct from—generalized coordinates as used

    Generalized filtering

    Generalized_filtering

  • Noether's theorem
  • Statement relating differentiable symmetries to conserved quantities

    = 1. Taking δθ as the ε parameter and the Cartesian coordinates r as the generalized coordinates q, the corresponding Q variables are given by Q = n ×

    Noether's theorem

    Noether's theorem

    Noether's_theorem

  • Hamiltonian optics
  • Formulation of geometrical optics

    q_{N}{\left(\sigma \right)}\right)} described by N {\displaystyle N} generalized coordinates between two specified states at two specified parameters σA and

    Hamiltonian optics

    Hamiltonian_optics

  • Hamilton–Jacobi equation
  • Formulation of classical mechanics

    choice of generalized coordinates. For orthogonal coordinates and Hamiltonians that have no time dependence and are quadratic in the generalized momenta

    Hamilton–Jacobi equation

    Hamilton–Jacobi_equation

  • Configuration space (physics)
  • Space of possible positions for all objects in a physical system

    the configuration of a system are called generalized coordinates, and the space defined by these coordinates is called the configuration space of the

    Configuration space (physics)

    Configuration_space_(physics)

  • Frame of reference
  • Abstract coordinate system

    perspective, the formulation of many problems in physics employs generalized coordinates, normal modes or eigenvectors, which are only indirectly related

    Frame of reference

    Frame_of_reference

  • Projective plane
  • Geometric concept of a 2D space with "points at infinity" adjoined

    (geometric) plane through the origin in the 3-space. This idea can be generalized and made more precise as follows. Let K be any division ring (skewfield)

    Projective plane

    Projective plane

    Projective_plane

  • Centrifugal force
  • Type of inertial force

    Retrieved 2020-11-09. For a description of generalized coordinates, see Ahmed A. Shabana (2003). "Generalized coordinates and kinematic constraints". Dynamics

    Centrifugal force

    Centrifugal force

    Centrifugal_force

  • Holonomic constraints
  • Type of constraints for mechanical systems

    n } {\displaystyle \{u_{1},u_{2},u_{3},\ldots ,u_{n}\}} are n generalized coordinates that describe the system (in unconstrained configuration space)

    Holonomic constraints

    Holonomic_constraints

  • Equations of motion
  • Equations that describe the behavior of a physical system

    are usually spatial coordinates and time, but may include momentum components. The most general choice are generalized coordinates which can be any convenient

    Equations of motion

    Equations of motion

    Equations_of_motion

  • Canonical transformation
  • Coordinate transformation that preserves the form of Hamilton's equations

    mechanics). Since Lagrangian mechanics is based on generalized coordinates, transformations of the coordinates q → Q do not affect the form of Lagrange's equations

    Canonical transformation

    Canonical_transformation

  • Classical mechanics
  • Description of large objects' physics

    mechanics are Lagrangian mechanics, which uses generalized coordinates and corresponding generalized velocities in tangent bundle space (the tangent

    Classical mechanics

    Classical mechanics

    Classical_mechanics

  • Scientific law
  • Statement based on repeated empirical observations that describes some natural phenomenon

    freedom is defined by generalized coordinates q = (q1, q2, ... qN). There are generalized momenta conjugate to these coordinates, p = (p1, p2, ..., pN)

    Scientific law

    Scientific_law

  • Virtual work
  • Work done by a force to move a particle along a virtual displacement

    virtual displacements. This can be generalized to an arbitrary mechanical system defined by the generalized coordinates q i {\displaystyle q_{i}} , i = 1

    Virtual work

    Virtual_work

  • Action (physics)
  • Physical quantity of dimension energy × time

    the action-angle coordinates, called the "action" of the generalized coordinate qk, is defined by integrating a single generalized momentum around a

    Action (physics)

    Action_(physics)

  • Rigid body dynamics
  • Study of the effects of forces on undeformable bodies

    {q}}}}\right),} is the generalized force acting on this one degree of freedom system. If the mechanical system is defined by m generalized coordinates, qj, j = 1

    Rigid body dynamics

    Rigid body dynamics

    Rigid_body_dynamics

  • Euler–Lagrange equation
  • Second-order partial differential equation describing motion of mechanical system

    has the advantage that it takes the same form in any system of generalized coordinates, and it is better suited to generalizations. In classical field

    Euler–Lagrange equation

    Euler–Lagrange_equation

  • Hamilton's principle
  • Formulation of the principle of stationary action

    states that the true evolution q(t) of a system described by N generalized coordinates q = (q1, q2, ..., qN) between two specified states q1 = q(t1) and

    Hamilton's principle

    Hamilton's principle

    Hamilton's_principle

  • Maupertuis's principle
  • Principle of least length in physics

    involve the generalized velocities. By defining a normalized distance or metric d s {\displaystyle ds} in the space of generalized coordinates d s 2 = d

    Maupertuis's principle

    Maupertuis's_principle

  • Appell's equation of motion
  • Formulation of classical mechanics

    _{r}={\ddot {q}}_{r}} is an arbitrary generalized acceleration, or the second time derivative of the generalized coordinates q r {\displaystyle q_{r}} , and

    Appell's equation of motion

    Appell's_equation_of_motion

  • Relativistic Lagrangian mechanics
  • Mathematical formulation of special and general relativity

    differential of r obtains the transformation of velocity v to the generalized coordinates, generalized velocities, and coordinate time v = ∑ j = 1 n ∂ r ∂ q j q

    Relativistic Lagrangian mechanics

    Relativistic Lagrangian mechanics

    Relativistic_Lagrangian_mechanics

  • Rayleigh dissipation function
  • Function used in Lagrangian mechanics

    potential. This relationship is represented in terms of the set of generalized coordinates q i = { q 1 , q 2 , … q n } {\displaystyle q_{i}=\left\{q_{1},q_{2}

    Rayleigh dissipation function

    Rayleigh_dissipation_function

  • Elliptic coordinate system
  • 2D coordinate system whose coordinate lines are confocal ellipses and hyperbolae

    the momenta). Curvilinear coordinates Ellipsoidal coordinates Generalized coordinates Bipolar coordinates "Elliptic coordinates", Encyclopedia of Mathematics

    Elliptic coordinate system

    Elliptic coordinate system

    Elliptic_coordinate_system

  • Mechanical equilibrium
  • When the net force on a particle is zero

    where the gradient of the potential energy with respect to the generalized coordinates is zero. If a particle in equilibrium has zero velocity, that particle

    Mechanical equilibrium

    Mechanical equilibrium

    Mechanical_equilibrium

  • Mass matrix
  • Matrix relating a system's generalized coordinate vector and kinetic energy

    describes the evolution of a system in terms of an arbitrary vector of generalized coordinates that completely defines the position of every particle in the system

    Mass matrix

    Mass_matrix

  • Lagrangian (field theory)
  • Application of Lagrangian mechanics to field theories

    bundles. In Lagrangian field theory, the Lagrangian as a function of generalized coordinates is replaced by a Lagrangian density, a function of the fields in

    Lagrangian (field theory)

    Lagrangian_(field_theory)

  • Action principles
  • Fundamental mechanical principles

    p2,…,pN) are the particle momenta or the conjugate momenta of generalized coordinates, defined by the equation p k   = def   ∂ L ∂ q ˙ k , {\displaystyle

    Action principles

    Action_principles

  • Scleronomous
  • Mechanical system whose constraints are independent of time

    explicit variable and the equation of constraints can be described by generalized coordinates. Such constraints are called scleronomic constraints. The opposite

    Scleronomous

    Scleronomous

  • Derivative (multivariable calculus)
  • Type of derivative in mathematics

    time derivative of a function of time and the n {\displaystyle n} generalized coordinates lead to the same equations of motion. An interesting example concerns

    Derivative (multivariable calculus)

    Derivative_(multivariable_calculus)

  • Routhian mechanics
  • Formulation of classical mechanics

    generalized velocity dqi/dt is to be expressed as a function of generalized momentum pi via its defining relation. The choice of which n coordinates are

    Routhian mechanics

    Routhian mechanics

    Routhian_mechanics

  • Phase space
  • Space of all possible states that a system can take

    mechanics, any choice of generalized coordinates qi for the position (i.e. coordinates on configuration space) defines conjugate generalized momenta pi, which

    Phase space

    Phase space

    Phase_space

  • Nonholonomic system
  • Type of optimization problem

    generalized coordinates and is the foundation of Lagrangian mechanics. Nonholonomic constraints cannot be eliminated by using generalized coordinates

    Nonholonomic system

    Nonholonomic_system

  • Position and momentum spaces
  • Physical spaces representing position and momentum, Fourier-transform duals

    n-tuple of the generalized momenta. A Legendre transformation is performed to change the variables in the total differential of the generalized coordinate

    Position and momentum spaces

    Position_and_momentum_spaces

  • Schrödinger equation
  • Description of a quantum-mechanical system

    {\displaystyle H} is the Hamiltonian function (not operator). Here the generalized coordinates q i {\displaystyle q_{i}} for i = 1 , 2 , 3 {\displaystyle i=1

    Schrödinger equation

    Schrödinger_equation

  • Manifold
  • Topological space that locally resembles Euclidean space

    freedom of the system and where the points are specified by their generalized coordinates. For an unconstrained movement of free particles the manifold is

    Manifold

    Manifold

    Manifold

  • Multibody system
  • Tool to study dynamic behavior of interconnected rigid or flexible bodies

    redundant coordinates, because the equations use more coordinates than degrees of freedom of the underlying system. The generalized coordinates are denoted

    Multibody system

    Multibody_system

  • Hamiltonian (quantum mechanics)
  • Quantum operator for the sum of energies of a system

    Hamilton's equations, with the a n {\displaystyle a_{n}} s as the generalized coordinates, the π n {\displaystyle \pi _{n}} s as the conjugate momenta, and

    Hamiltonian (quantum mechanics)

    Hamiltonian_(quantum_mechanics)

  • Motion
  • Change in the position of an object

    are usually spatial coordinates and time, but may include momentum components. The most general choice are generalized coordinates which can be any convenient

    Motion

    Motion

    Motion

  • Conserved quantity
  • Value remaining constant in a dynamical system

    {\displaystyle {\mathcal {H}}} , a function f of the generalized coordinates q and generalized momenta p has time evolution d f d t = { f , H } + ∂ f

    Conserved quantity

    Conserved_quantity

  • Joseph-Louis Lagrange
  • Italian-French scientist (1736–1813)

    its configuration by a sufficient number of variables x, called generalized coordinates, whose number is the same as that of the degrees of freedom possessed

    Joseph-Louis Lagrange

    Joseph-Louis Lagrange

    Joseph-Louis_Lagrange

  • Double pendulum
  • Pendulum with another pendulum attached to its end

    convenient to use the angles between each limb and the vertical as the generalized coordinates defining the configuration of the system. These angles are denoted

    Double pendulum

    Double pendulum

    Double_pendulum

  • Microstate (statistical mechanics)
  • Specific microscopic configuration of a thermodynamic system

    space, whose coordinate axes consist of the F generalized coordinates qi of the system, and its F generalized momenta pi. The microstate of such a system

    Microstate (statistical mechanics)

    Microstate (statistical mechanics)

    Microstate_(statistical_mechanics)

  • Inverted pendulum
  • Pendulum with center of mass above pivot

    {\theta }}^{2}.} The generalized coordinates of the system are θ {\displaystyle \theta } and x {\displaystyle x} , each has a generalized force. On the x {\displaystyle

    Inverted pendulum

    Inverted pendulum

    Inverted_pendulum

  • Hamiltonian system
  • Dynamical system governed by Hamilton's equations

    described by the generalized coordinates p {\displaystyle {\boldsymbol {p}}} and q {\displaystyle {\boldsymbol {q}}} , corresponding to generalized momentum and

    Hamiltonian system

    Hamiltonian system

    Hamiltonian_system

  • List of common physics notations
  • Power volt-ampere reactive (var) q {\displaystyle \mathbf {q} } Generalized coordinates varied depending on context (sometimes meter (m) or radian (rad))

    List of common physics notations

    List_of_common_physics_notations

  • Angular momentum
  • Conserved physical quantity; rotational analogue of linear momentum

    angles around the three axes cannot be treated simultaneously as generalized coordinates, since they are not independent; in particular, two angles per

    Angular momentum

    Angular momentum

    Angular_momentum

  • Tautological one-form
  • Canonical differential form

    {\displaystyle g,} then corresponding definitions can be made in terms of generalized coordinates. Specifically, if we take the metric to be a map g : T Q → T ∗

    Tautological one-form

    Tautological_one-form

  • Grand canonical ensemble
  • Statistical ensemble of particles in thermodynamic equilibrium

    the p1, … pn and q1, … qn are the canonical coordinates (generalized momenta and generalized coordinates) of the system's internal degrees of freedom

    Grand canonical ensemble

    Grand_canonical_ensemble

  • Josephson junction
  • Superconducting circuit element

    oscillator. In circuit quantization, flux and charge are treated as generalized coordinates. The quantization step promotes ϕ {\displaystyle \phi } (dimensionless

    Josephson junction

    Josephson junction

    Josephson_junction

  • Hamiltonian mechanics
  • Formulation of classical mechanics using momenta

    mechanics replaces (generalized) velocities q ˙ i {\displaystyle {\dot {q}}^{i}} used in Lagrangian mechanics with (generalized) momenta. Both theories

    Hamiltonian mechanics

    Hamiltonian mechanics

    Hamiltonian_mechanics

  • Stress–energy tensor
  • Tensor describing energy momentum density in spacetime

    spacetime coordinates, we can construct the canonical stress–energy tensor by looking at the total derivative with respect to one of the generalized coordinates

    Stress–energy tensor

    Stress–energy tensor

    Stress–energy_tensor

  • Hamiltonian field theory
  • Formalism in classical field theory based on Hamiltonian mechanics

    Hamiltonian for a system of discrete particles is a function of their generalized coordinates and conjugate momenta, and possibly, time. For continua and fields

    Hamiltonian field theory

    Hamiltonian_field_theory

  • Poisson bracket
  • Operation in Hamiltonian mechanics

    _{j}]=-\delta _{ij}} Note that the summation here involves generalized coordinates as well as generalized momentum. The invariance of Poisson bracket can be expressed

    Poisson bracket

    Poisson bracket

    Poisson_bracket

  • Constraint (computational chemistry)
  • Method for satisfying the Newtonian motion of a rigid body which consists of mass points

    represents the generalized forces and the scalar V(q) represents the potential energy, both of which are functions of the generalized coordinates q. If M constraints

    Constraint (computational chemistry)

    Constraint_(computational_chemistry)

  • Generalized function
  • Objects extending the notion of functions

    theory of generalized functions in order to define weak solutions of partial differential equations (i.e. solutions which are generalized functions,

    Generalized function

    Generalized_function

  • Cartesian coordinate system
  • Coordinate system using perpendicular axes

    later generalized into the concept of vector spaces. Many other coordinate systems have been developed since Descartes, such as the polar coordinates for

    Cartesian coordinate system

    Cartesian coordinate system

    Cartesian_coordinate_system

  • D'Alembert's principle
  • Statement in classical mechanics

    Q j {\displaystyle Q_{j}} being a generalized applied force and Q j ∗ {\displaystyle Q_{j}^{*}} being a generalized inertia force. This condition yields

    D'Alembert's principle

    D'Alembert's principle

    D'Alembert's_principle

  • Ensemble (mathematical physics)
  • Idealization of a large number of atomic-sized systems

    mechanical system with a defined number of parts, the phase space has n generalized coordinates called q1, ... qn, and n associated canonical momenta called p1

    Ensemble (mathematical physics)

    Ensemble_(mathematical_physics)

  • Hypercube
  • Convex polytope, the n-dimensional analogue of a square and a cube

    generates a 4-dimensional unit hypercube (a unit tesseract). This can be generalized to any number of dimensions. This process of sweeping out volumes can

    Hypercube

    Hypercube

    Hypercube

  • Ellipsoidal coordinates
  • Three-dimensional coordinate system

    Ellipsoidal coordinates are a three-dimensional orthogonal coordinate system ( λ , μ , ν ) {\displaystyle (\lambda ,\mu ,\nu )} that generalizes the two-dimensional

    Ellipsoidal coordinates

    Ellipsoidal_coordinates

  • Christoffel symbols
  • Array of numbers describing a metric connection

    x i {\displaystyle x^{i}} be the generalized coordinates and x ˙ i {\displaystyle {\dot {x}}^{i}} be the generalized velocities, then the kinetic energy

    Christoffel symbols

    Christoffel_symbols

  • Canonical ensemble
  • Ensemble of states at a constant temperature

    the p1, … pn and q1, … qn are the canonical coordinates (generalized momenta and generalized coordinates) of the system's internal degrees of freedom

    Canonical ensemble

    Canonical_ensemble

  • Paul Flory
  • American chemist (1910–1985)

    _{i}} . Applying a vector conversion from the Cartesian coordinates to the generalized coordinates will describe the same three-dimensional structure using

    Paul Flory

    Paul Flory

    Paul_Flory

  • ADM formalism
  • Hamiltonian formulation of general relativity

    ( 4 ) g i j {\displaystyle g_{ij}={^{(4)}}g_{ij}} will be the generalized coordinates for a Hamiltonian formulation. The conjugate momenta can then be

    ADM formalism

    ADM formalism

    ADM_formalism

  • Computational anatomy
  • Interdisciplinary field of biology

    generally, the Euler–Lagrange equations can be derived for systems of generalized coordinates. The Euler–Lagrange equation in computational anatomy describes

    Computational anatomy

    Computational_anatomy

  • Perturbation theory (quantum mechanics)
  • Mathematical approach to quantum physics

    are considered as generalized coordinates, then Fμ should be identified as the generalized force operators related to those coordinates. Different indices

    Perturbation theory (quantum mechanics)

    Perturbation_theory_(quantum_mechanics)

  • Classical Mechanics (Goldstein)
  • Advanced undergraduate or graduate textbook

    concepts, then introduces the principle of virtual work, constraints, generalized coordinates, and Lagrangian mechanics. Scattering is treated in the same chapter

    Classical Mechanics (Goldstein)

    Classical_Mechanics_(Goldstein)

  • Vlasov equation
  • Description of the time-evolution of plasma

    equation, though anachronistically in this context—expressed in generalized coordinates: d d t f ( r , p , t ) = 0 {\displaystyle {\frac {\mathrm {d} }{\mathrm

    Vlasov equation

    Vlasov_equation

  • Seakeeping
  • Response of a vessel to sea conditions

    ^{2}=gk\tanh(kh)} The vessel response is commonly represented by six generalized coordinates corresponding to surge, sway, heave, roll, pitch and yaw. In the

    Seakeeping

    Seakeeping

    Seakeeping

  • Kozai mechanism
  • Phenomenon affecting the orbit of a binary system

    {\mathcal {H}}} , of canonical coordinates in phase space. The canonical coordinates consist of the generalized coordinates x k {\displaystyle x_{k}} in

    Kozai mechanism

    Kozai_mechanism

  • Laplace–Runge–Lenz vector
  • Vector used in astronomy

    direction. A generalized conserved LRL vector A {\displaystyle {\mathcal {A}}} can be defined for all central forces, but this generalized vector is a

    Laplace–Runge–Lenz vector

    Laplace–Runge–Lenz_vector

  • List of equations in classical mechanics
  • E_{p}={\frac {1}{2}}k(r_{2}-r_{1})^{2}} where r2 and r1 are collinear coordinates of the free end of the spring, in the direction of the extension/compression

    List of equations in classical mechanics

    List_of_equations_in_classical_mechanics

  • Operator (physics)
  • Function acting on the space of physical states in physics

    , p , t ) {\displaystyle H(q,p,t)} , a function of the generalized coordinates q, generalized velocities q ˙ = d q / d t {\displaystyle {\dot {q}}=\mathrm

    Operator (physics)

    Operator_(physics)

  • Four-momentum
  • 4D relativistic energy and momentum

    from the action S. Given that in general for a closed system with generalized coordinates qi and canonical momenta pi, p i = ∂ S ∂ q i = ∂ S ∂ x i , E =

    Four-momentum

    Four-momentum

  • Émilie du Châtelet
  • French mathematician, physicist, and author (1706–1749)

    true for all problems where the initial state is symmetric in generalized coordinates. E.g., mechanical energy, either kinetic or potential, may be lost

    Émilie du Châtelet

    Émilie du Châtelet

    Émilie_du_Châtelet

  • Partition function (mathematics)
  • Generalization of the concept from statistical mechanics

    X} . The word conjugate here is used in the sense of conjugate generalized coordinates in Lagrangian mechanics, thus, properly β {\displaystyle \beta

    Partition function (mathematics)

    Partition_function_(mathematics)

  • Fictitious force
  • Frame-dependent apparent force in Physics

    motion equation Frenet–Serret formulas General relativity Generalized coordinates Generalized force Gravity Inertial reference frame Kinematics Kinetics

    Fictitious force

    Fictitious force

    Fictitious_force

  • Homogeneous coordinates
  • Coordinate system used in projective geometry

    coordinates or projective coordinates, introduced by August Ferdinand Möbius in his 1827 work Der barycentrische Calcul, are a system of coordinates used

    Homogeneous coordinates

    Homogeneous coordinates

    Homogeneous_coordinates

  • Stochastic Eulerian Lagrangian method
  • been introduced allowing for descriptions of structures involving generalized coordinates and additional translational or rotational degrees of freedom.

    Stochastic Eulerian Lagrangian method

    Stochastic_Eulerian_Lagrangian_method

  • Type locality (biology)
  • Place where a name-bearing type specimen was collected

    publishing a broader verbal locality, rounding or generalizing coordinates, or withholding exact coordinates from public datasets while retaining the full

    Type locality (biology)

    Type_locality_(biology)

  • Intensive and extensive properties
  • Properties independent of system size, and proportional to system size

    care is needed to distinguish generalized coordinates (often extensive, such as total charge) from their conjugate generalized forces (often intensive, such

    Intensive and extensive properties

    Intensive and extensive properties

    Intensive_and_extensive_properties

  • Lagrangian and Eulerian specification of the flow field
  • Computational fluid dynamics tools

    Contour advection Displacement field (mechanics) Equivalent latitude Generalized Lagrangian mean Trajectory (fluid mechanics) Liouville's theorem (Hamiltonian)

    Lagrangian and Eulerian specification of the flow field

    Lagrangian and Eulerian specification of the flow field

    Lagrangian_and_Eulerian_specification_of_the_flow_field

  • Herglotz's variational principle
  • Principle in mathematical physics

    its generalized coordinates, and let u = ( u 1 , u 2 , … , u n ) {\displaystyle {\boldsymbol {u}}=(u_{1},u_{2},\dots ,u_{n})} be its generalized velocity

    Herglotz's variational principle

    Herglotz's_variational_principle

  • First-class constraint
  • switch to generalized coordinates that manifestly solve the constraint, or one can use a Lagrange multiplier while retaining the redundant coordinates so constrained

    First-class constraint

    First-class_constraint

  • Curvilinear coordinates
  • Coordinate system whose directions vary in space

    geometry, curvilinear coordinates are a coordinate system for Euclidean space in which the coordinate lines may be curved. These coordinates may be derived from

    Curvilinear coordinates

    Curvilinear coordinates

    Curvilinear_coordinates

  • Spherical pendulum
  • 3-Dimensional analogue of a pendulum

    of the Lagrangian L = T − V {\displaystyle L=T-V} in arbitrary generalized coordinates the position of the mass is expressed along Cartesian axes. Here

    Spherical pendulum

    Spherical pendulum

    Spherical_pendulum

  • Moving frame
  • Generalization of an ordered basis of a vector space

    automorphisms is G. A smooth manifold Σ which serves as a space of (generalized) coordinates for X. A collection of frames ƒ each of which determines a coordinate

    Moving frame

    Moving frame

    Moving_frame

  • Pfaffian constraint
  • {\displaystyle \{u_{1},u_{2},u_{3},\ldots ,u_{n}\}} are the n generalized coordinates that describe the system, and where L {\displaystyle L} is the

    Pfaffian constraint

    Pfaffian_constraint

  • Bohr–Van Leeuwen theorem
  • Theorem on magnetism

    {p} _{N};\mathbf {r} _{1},\ldots ,\mathbf {r} _{N})} of these generalized coordinates is then ⟨ f ⟩ = ∫ f d P ∫ d P . {\displaystyle \langle f\rangle

    Bohr–Van Leeuwen theorem

    Bohr–Van_Leeuwen_theorem

  • Electromechanical modeling
  • systems is mainly based on the Lagrangian which is a function of the generalized coordinates and the associated velocities. If all forces are derivable from

    Electromechanical modeling

    Electromechanical_modeling

  • Microcanonical ensemble
  • Ensemble of states with an exactly specified total energy

    qn) defined over the system's phase space. The phase space has n generalized coordinates called q1, ... qn, and n associated canonical momenta called p1

    Microcanonical ensemble

    Microcanonical_ensemble

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  • Squire
  • Surname or Lastname

    English

    Squire

    English : status name from Middle English squyer ‘esquire’, ‘a man belonging to the feudal rank immediately below that of knight’ (from Old French esquier ‘shield bearer’). At first it denoted a young man of good birth attendant on a knight, or by extension any attendant or servant, but by the 14th century the meaning had been generalized, and referred to social status rather than age. By the 17th century, the term denoted any member of the landed gentry, but this is unlikely to have influenced the development of the surname.

    Squire

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Online names & meanings

  • Daylam
  • Boy/Male

    Arabic, Muslim

    Daylam

    Name of a Companion of the Prophet PBUH

  • Charukesi
  • Girl/Female

    Hindu, Indian

    Charukesi

    Name of a Raga of Carnatic Music

  • Turhan
  • Boy/Male

    Muslim/Islamic

    Turhan

    Of mercy

  • Iman
  • Girl/Female

    African, American, Arabic, French, Indian, Iranian, Kannada, Muslim, Parsi, Punjabi, Sikh, Sindhi, Telugu

    Iman

    Faith; Belief; Faithful; Believer of Faith

  • Kashaf
  • Boy/Male

    Arabic, Muslim

    Kashaf

    Opener; Untier; One who Opens

  • Kerensa
  • Girl/Female

    British, Christian, English, Indian

    Kerensa

    Beautiful

  • Yogadevan
  • Boy/Male

    Hindu

    Yogadevan

    Lord of Yoga

  • Samuela
  • Girl/Female

    Hebrew

    Samuela

    Asked of God.

  • Rosemond
  • Girl/Female

    Australian, German, Teutonic

    Rosemond

    Famous Defender

  • Linet
  • Girl/Female

    Australian, French, Indian, Malayalam, Welsh

    Linet

    Idol; Image; A Small Bird

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GENERALIZED COORDINATES

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GENERALIZED COORDINATES

  • Mineralized
  • imp. & p. p.

    of Mineralize

  • Mineralize
  • v. t.

    To impregnate with a mineral; as, mineralized water.

  • Federalized
  • imp. & p. p.

    of Federalize

  • Centralism
  • n.

    The system by which power is centralized, as in a government.

  • Generalizing
  • p. pr. & vb. n.

    of Generalize

  • Generalize
  • v. t.

    To derive or deduce (a general conception, or a general principle) from particulars.

  • Generalizer
  • n.

    One who takes general or comprehensive views.

  • Generalizable
  • a.

    Capable of being generalized, or reduced to a general form of statement, or brought under a general rule.

  • Manifoldness
  • n.

    A generalized concept of magnitude.

  • Induce
  • v. t.

    To generalize or conclude as an inference from all the particulars; -- the opposite of deduce.

  • Generalize
  • v. t.

    To bring under a genus or under genera; to view in relation to a genus or to genera.

  • Amphioxus
  • n.

    A fishlike creature (Amphioxus lanceolatus), two or three inches long, found in temperature seas; -- also called the lancelet. Its body is pointed at both ends. It is the lowest and most generalized of the vertebrates, having neither brain, skull, vertebrae, nor red blood. It forms the type of the group Acrania, Leptocardia, etc.

  • Unicursal
  • a.

    That can be passed over in a single course; -- said of a curve when the coordinates of the point on the curve can be expressed as rational algebraic functions of a single parameter /.

  • Centralization
  • n.

    The act or process of centralizing, or the state of being centralized; the act or process of combining or reducing several parts into a whole; as, the centralization of power in the general government; the centralization of commerce in a city.

  • Generalized
  • a.

    Comprising structural characters which are separated in more specialized forms; synthetic; as, a generalized type.

  • Generalize
  • v. t.

    To apply to other genera or classes; to use with a more extensive application; to extend so as to include all special cases; to make universal in application, as a formula or rule.

  • Generalized
  • imp. & p. p.

    of Generalize

  • Generalize
  • v. i.

    To form into a genus; to view objects in their relations to a genus or class; to take general or comprehensive views.

  • Centralized
  • imp. & p. p.

    of Centralize

  • Universalize
  • v. t.

    To make universal; to generalize.