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Equations of motion for viscous fluids
The Navier–Stokes equations generalize the Euler equations in that the latter model only considers inviscid flow. The Navier–Stokes equations are of great
Navier–Stokes_equations
Topics referred to by the same term
Stokes equation may refer to: the Airy equation the equations of Stokes flow, a linearised form of the Navier–Stokes equations in the limit of small Reynolds
Stokes_equation
Law describing the pressure drop in an incompressible and Newtonian fluid
justification of the Poiseuille law was given by George Stokes in 1845. The assumptions of the equation are that the fluid is incompressible and Newtonian;
Hagen–Poiseuille_equation
Equation in Brownian motion
Einstein–Smoluchowski equation, for diffusion of charged particles: D = μ q k B T q {\displaystyle D={\frac {\mu _{q}\,k_{\text{B}}T}{q}}} Stokes–Einstein–Sutherland
Einstein relation (kinetic theory)
Einstein_relation_(kinetic_theory)
Equations of fluid dynamics
the equations, such as Navier–Stokes existence and smoothness, is one of the important unsolved problems in mathematics. The Navier–Stokes equations are
Derivation of the Navier–Stokes equations
Derivation_of_the_Navier–Stokes_equations
Millennium Prize Problem
The Navier–Stokes existence and smoothness problem concerns the mathematical properties of solutions to the Navier–Stokes equations, a system of partial
Navier–Stokes existence and smoothness
Navier–Stokes_existence_and_smoothness
Type of fluid flow
polymers generally. The equations of motion for Stokes flow, called the Stokes equations, are a linearization of the Navier–Stokes equations, and thus can be
Stokes_flow
Equation for the velocity of a body in viscous fluid
derived by George Gabriel Stokes in 1851 by solving the Stokes flow limit for small Reynolds numbers of the Navier–Stokes equations. The force of viscosity
Stokes's_law
Turbulence modeling approach
Reynolds-averaged Navier–Stokes equations (RANS equations) are time-averaged equations of motion for fluid flow. The idea behind the equations is Reynolds decomposition
Reynolds-averaged Navier–Stokes equations
Reynolds-averaged_Navier–Stokes_equations
Type of differential equation
solutions to the Navier–Stokes equations, named as one of the Millennium Prize Problems in 2000. Partial differential equations occur very widely in mathematically
Partial_differential_equation
mechanics, non-dimensionalization of the Navier–Stokes equations is the conversion of the Navier–Stokes equation to a nondimensional form. This technique can
Non-dimensionalization and scaling of the Navier–Stokes equations
Non-dimensionalization_and_scaling_of_the_Navier–Stokes_equations
Branch of physics
was provided by Claude-Louis Navier and George Gabriel Stokes in the Navier–Stokes equations, and boundary layers were investigated (Ludwig Prandtl,
Fluid_mechanics
Subfield of fluid dynamics
hydrodynamic stability problems are the Navier–Stokes equation and the continuity equation. The Navier–Stokes equation is given by: ∂ u ∂ t + ( u ⋅ ∇ ) u − ν
Hydrodynamic_stability
Flow of fluids with zero viscosity (superfluids)
molecular theory, which was further confirmed by Stokes using continuum theory. The Navier–Stokes equations describe the motion of fluids: ρ D v D t = − ∇
Inviscid_flow
Force distributed over an area
kinematic viscosity ν {\displaystyle \nu } in order to compute the Navier–Stokes equation without explicitly showing the density ρ 0 {\displaystyle \rho _{0}}
Pressure
Equations describing behavior of a model
another example, in fluid dynamics, the Navier-Stokes equations are more refined than Euler equations. As the field progresses and our understanding of
Governing_equation
Equation describing the transport of some quantity
Continuity equations underlie more specific transport equations such as the convection–diffusion equation, Boltzmann transport equation, and Navier–Stokes equations
Continuity_equation
Equation describing the flow of a fluid through a porous medium
law is a special case of the Stokes equation for the momentum flux, in turn deriving from the momentum Navier–Stokes equation. Darcy's law is analogous to
Darcy's_law
Class of computational fluid dynamics methods
(CFD) methods for fluid simulation. Instead of solving the Navier–Stokes equations directly, a fluid density on a lattice is simulated with streaming
Lattice_Boltzmann_methods
Set of partial differential equations on fluid flow
momentum equation can be derived from the Navier–Stokes equations that describe fluid motion. The x-component of the Navier–Stokes equations – when expressed
Shallow_water_equations
Finite element method for Navier-Stokes equations
terms in the Navier–Stokes Galerkin formulation. The finite element (FE) numerical computation of incompressible Navier–Stokes equations (NS) suffers from
Streamline_upwind_Petrov–Galerkin_pressure-stabilizing_Petrov–Galerkin_formulation_for_incompressible_Navier–Stokes_equations
Equation describing the evolution of the vorticity of a fluid particle as it flows
vorticity due to flow compressibility. It follows from the Navier-Stokes equation for continuity, namely ∂ ρ ∂ t + ∇ ⋅ ( ρ u ) = 0 ⟺ ∇ ⋅ u = − 1 ρ d
Vorticity_equation
Type of fluid
(2016). "Self-Similar Analytic Solution of the Two-Dimensional Navier-Stokes Equation with a Non-Newtonian Type of Viscosity". Mathematical Modelling and
Non-Newtonian_fluid
Functional equation Functional equation (L-function) Constitutive equation Laws of science Defining equation (physical chemistry) List of equations in classical
List_of_equations
Set of quasilinear hyperbolic equations governing adiabatic and inviscid flow
they correspond to the Navier–Stokes equations with zero viscosity and zero thermal conductivity. The Euler equations can be applied to incompressible
Euler equations (fluid dynamics)
Euler_equations_(fluid_dynamics)
Equation
equation will lead to the Navier–Stokes equations. By assuming inviscid flow, the Navier–Stokes equations can further simplify to the Euler equations
Cauchy_momentum_equation
Principle relating to fluid dynamics
Coandă effect Euler equations – for the flow of an inviscid fluid Hydraulics – applied fluid mechanics for liquids Navier–Stokes equations – for the flow of
Bernoulli's_principle
Combination of the diffusion and convection (advection) equations
convection–diffusion equation is a parabolic partial differential equation that combines the diffusion and convection (advection) equations. It describes physical
Convection–diffusion_equation
Mathematical model in fluid dynamics
Navier–Stokes equations, Math. Comp., 22, 745–762 (1968). Kim, J. and Moin, P., Application of a fractional-step method to incompressible Navier–Stokes equations
Taylor–Green_vortex
Formulae for viscous and incompressible fluid flow at small Reynolds numbers
compared to Stokes flow, with the (partial) inclusion of convective acceleration. Oseen's work is based on the experiments of G.G. Stokes, who had studied
Oseen_equations
System where changes of output are not proportional to changes of input
Ishimori equation Kadomtsev–Petviashvili equation Korteweg–de Vries equation Landau–Lifshitz–Gilbert equation Liénard equation Navier–Stokes equations of fluid
Nonlinear_system
Analysis and solving of problems that involve fluid flows
problems is the Navier–Stokes equations, which define a number of single-phase (gas or liquid, but not both) fluid flows. These equations can be simplified
Computational_fluid_dynamics
British mathematician and physicist (1819–1903)
Lucasian Professor. As a physicist, Stokes made seminal contributions to fluid mechanics, including the Navier–Stokes equations; and to optics, with notable
Sir George Stokes, 1st Baronet
Sir_George_Stokes,_1st_Baronet
Eigenvalue equation
Navier–Stokes equations for a parallel, laminar flow can become unstable if certain conditions on the flow are satisfied, and the Orr–Sommerfeld equation determines
Orr–Sommerfeld_equation
Equation in convective heat transfer
need for the equation arises from the inability to solve the Navier–Stokes equations in the turbulent flow regime, even for a Newtonian fluid. When the
Churchill–Bernstein_equation
Aspects of fluid mechanics involving fluid flow
light, the momentum equations for Newtonian fluids are the Navier–Stokes equations—which is a non-linear set of differential equations that describes the
Fluid_dynamics
Dimensionless number; ratio of a fluid's flow inertia to the external field
theory. Incompressible Navier–Stokes momentum equation is a Cauchy momentum equation with the Pascal law and Stokes's law being the stress constitutive
Froude_number
Partial differential equation with nonlinear terms
existence for a Monge–Ampere equation. The open problem of existence (and smoothness) of solutions to the Navier–Stokes equations is one of the seven Millennium
Nonlinear partial differential equation
Nonlinear_partial_differential_equation
Seven mathematical problems with a US$1 million prize for each solution
Fefferman, Charles L. (2006). "Existence and smoothness of the Navier–Stokes equation" (PDF). In Carlson, James; Jaffe, Arthur; Wiles, Andrew (eds.). The
Millennium_Prize_Problems
Ratio of inertial to viscous forces acting on a liquid
t}},&\nabla '&=L\nabla ,\end{aligned}}} we can rewrite the Navier–Stokes equation without dimensions: D v ′ D t ′ = − ∇ ′ p ′ + μ ρ L V ∇ ′ 2 v ′ + f
Reynolds_number
Oscillating boundary layer over a plate
after Sir George Stokes. This is considered one of the simplest unsteady problems that has an exact solution for the Navier–Stokes equations. In turbulent
Stokes_problem
Fluid dynamics phenomenon
steady-state solution for the Stokes equations around an infinitely long cylinder. This is opposed to the 3-dimensional case, where Stokes' method provides a solution
Stokes'_paradox
Method for numerically solving time-dependent incompressible fluid-flow problems
solving incompressible Navier–Stokes equations. The incompressible Navier-Stokes equation (differential form of momentum equation) may be written as ∂ u ∂
Projection method (fluid dynamics)
Projection_method_(fluid_dynamics)
Discretization of the Navier–Stokes equations of fluid dynamics is a reformulation of the equations in such a way that they can be applied to computational
Discretization of Navier–Stokes equations
Discretization_of_Navier–Stokes_equations
Physics theorem about a swimmer's displacement
mathematical consequences of the linearity of Stokes equations. To summarize, the linearity of Stokes equations allows us to use the reciprocal theorem to
Scallop_theorem
Equation in fluid dynamics
is equivalent to the Hagen–Poiseuille equation, which is analytically derived from the Navier–Stokes equations. The head loss Δh (or hf) expresses the
Darcy–Weisbach_equation
Entropy production in Newtonian fluids
the governing equations for mass conservation and momentum conservation are the continuity equation and the Navier-Stokes equations: ∂ ρ ∂ t = − ∇ ⋅
General equation of heat transfer
General_equation_of_heat_transfer
State of balance between external forces on a fluid and internal pressure gradient
last equation can be derived by solving the three-dimensional Navier–Stokes equations for the equilibrium situation where u = v = ∂ p ∂ x = ∂ p ∂ y = 0 {\displaystyle
Hydrostatic_equilibrium
\nabla ^{2}\mathbf {v} +\mathbf {f} .} The Stokes approximation is developed from the Navier-Stokes equations by omission of the convective term. For small
Stokes approximation and artificial time
Stokes_approximation_and_artificial_time
Mathematical object used in fluid dynamics
analogous to electric field, when the Navier–Stokes equation is compared with Maxwell's equations. The Euler equations written in terms of the Lamb vector is
Lamb_vector
Technique to solve partial differential equations
described by partial differential equations. For example, the Navier–Stokes equations are a set of partial differential equations derived from the conservation
Physics-informed neural networks
Physics-informed_neural_networks
Branch of fluid mechanics that studies fluids at rest
Dynamics Archimedes' principle · Bernoulli's principle Navier–Stokes equations Poiseuille equation · Pascal's law Viscosity (Newtonian · non-Newtonian) Buoyancy ·
Hydrostatics
Statistical mechanics framework
relations appearing in hydrodynamical descriptions such as the Navier–Stokes equations. In doing so, expressions for various transport coefficients such as
Chapman–Enskog_theory
Concept in fluid mechanics
tensor in a fluid obtained from the averaging operation over the Navier–Stokes equations to account for turbulent fluctuations in fluid momentum. The velocity
Reynolds_stress
mechanics problem of Navier–Stokes existence and smoothness, which deals with the mathematical properties of the Navier-Stokes equations. The statement of the
History_of_fluid_mechanics
Equation of statistical mechanics
equation The Vlasov–Poisson equation Landau kinetic equation Fokker–Planck equation Williams–Boltzmann equation Derivation of Navier–Stokes equation from
Boltzmann_equation
Deflection of a spinning object moving through a fluid
Bernoulli's principle Coandă effect Fluid dynamics Kite types Navier–Stokes equations Potential flow around a circular cylinder Reynolds number Tesla turbine
Magnus_effect
Burnett equations are a set of higher-order continuum equations for non-equilibrium flows and the transition regimes where the Navier–Stokes equations do not
Burnett_equations
Differential equation describing pressure distribution of thin viscous fluids
of the Reynolds Equation from the Navier-Stokes equation can be found in numerous lubrication text books. In general, Reynolds equation has to be solved
Reynolds_equation
Mechanism by which a celestial body generates a magnetic field
⋅ u = 0 , {\displaystyle \nabla \cdot \mathbf {u} =0,} The Navier-Stokes equation for conservation of momentum, again in the same approximation, with
Dynamo_theory
Differential equation describing the thickness of a liquid film over time
direction normal to the surface. In the non-dimensional form of the Navier-Stokes equation the requirement is that terms of order ε2 and ε2Re are negligible,
Thin-film_equation
Principle in fluid mechanics
undiminished throughout the fluid. The formula is a specific case of Navier–Stokes equations without inertia and viscosity terms. If an oscillating U-tube is filled
Pascal's_law
Dimensionless number in fluid mechanics
l^{2}\sigma } . The Weber number appears in the incompressible Navier-Stokes equations through a free surface boundary condition. For a fluid of constant
Weber_number
Kinetic energy per unit volume of a fluid
Dynamic pressure can also appear as a term in the incompressible Navier-Stokes equation which may be written: ρ ∂ u ∂ t + ρ ( u ⋅ ∇ ) u − ρ ν ∇ 2 u = − ∇ p
Dynamic_pressure
Korteweg–de Vries equation Modified KdV–Burgers equation Maxwell's equations Navier–Stokes equations Poisson's equation Primitive equations (hydrodynamics)
List of partial differential equation topics
List_of_partial_differential_equation_topics
Topics referred to by the same term
Governor Stokes (disambiguation) Senator Stokes (disambiguation) Stokes (unit), a measure of viscosity Stokes boundary layer Stokes drift Stokes equation (disambiguation)
Stokes
Relation between gas pressure and volume
This law was the first physical law to be expressed in the form of an equation describing the dependence of two variable quantities. The law itself can
Boyle's_law
Terms in a mathematical expression with the largest order of magnitude
Navier–Stokes equations may be considerably simplified by considering only the leading-order components. For example, the Stokes flow equations. Also,
Leading-order_term
Fluid dynamics problem
Sir George Stokes. This is considered as one of the simplest unsteady problems that have an exact solution for the Navier-Stokes equations. The impulse
Rayleigh_problem
Mean kinetic energy per unit mass of eddies in turbulent flow
root-mean-square (RMS) velocity fluctuations. In the Reynolds-averaged Navier Stokes equations, the turbulence kinetic energy can be calculated based on the closure
Turbulence_kinetic_energy
Australian and American mathematician (born 1975)
between Tao's system and the Navier–Stokes equations themselves, it follows that any positive resolution of the Navier–Stokes existence and smoothness problem
Terence_Tao
Solution to the Navier–Stokes equations
Burgers vortex or Burgers–Rott vortex is an exact solution to the Navier–Stokes equations governing viscous flow, named after Jan Burgers and Nicholas Rott.
Burgers_vortex
Special function in the physical sciences
differential equation d 2 y d x 2 − x y = 0 , {\displaystyle {\frac {d^{2}y}{dx^{2}}}-xy=0,} known as the Airy equation or the Stokes equation. Because the
Airy_function
Liquid, gas, or other continuously deforming and flowing material
behavior of fluids can be described by the Navier–Stokes equations—a set of partial differential equations which are based on: continuity (conservation of
Fluid
Algorithm in computational fluid dynamics
dynamics to solve the Navier-Stokes equations. PISO is a pressure-velocity calculation procedure for the Navier-Stokes equations developed originally for
PISO_algorithm
Romanian-American mathematician
differential equations and fluid dynamics. His research focuses on mathematical aspects of hydrodynamics, including the Euler equations, the Navier–Stokes equations
Peter_Constantin
identical. This can be seen from inspection of the underlying Navier-Stokes equation, with geometrically similar bodies, equal Reynolds and Womersley Numbers
Dynamic similarity (Reynolds and Womersley numbers)
Dynamic_similarity_(Reynolds_and_Womersley_numbers)
Buoyancy principle in fluid dynamics
submerged volume (V) times the gravity (g) We can express this relation in the equation: F a = ρ g V {\displaystyle F_{a}=\rho gV} where F a {\displaystyle F_{a}}
Archimedes'_principle
Elliptic partial differential equation
Poisson's equation is an elliptic partial differential equation of broad utility in theoretical physics. For example, the solution to Poisson's equation is the
Poisson's_equation
Hydrodynamic formulation of the Schrödinger equations
hydrodynamical variables, similar to the Navier–Stokes equations of fluid dynamics. The derivation of the Madelung equations is similar to the de Broglie–Bohm formulation
Madelung_equations
French mathematician (born 1973)
concerns partial differential equations such as the Navier–Stokes equations, the wave equation, and the Schrödinger equation, as well as harmonic analysis
Isabelle_Gallagher
Mathematical model of how solid objects deform
independent of the choice of coordinate system, these governing equations are: Cauchy momentum equation, which is an expression of Newton's second law. In convective
Linear_elasticity
State of matter
and time-independent. The Navier-Stokes equations are a well-known example: they are partial differential equations giving the time evolution of density
Liquid
especially useful in studying fluid dynamics, such as in the Navier–Stokes equations that describe how fluids move. It is named after Jean Leray. The basic
Leray_projection
Law of physics and chemistry
related to energy and vice versa by E = m c 2 {\displaystyle E=mc^{2}} , the equation representing mass–energy equivalence, and science now takes the view that
Conservation_of_energy
Computational fluid dynamics algorithm
procedure to solve the Navier–Stokes equations. SIMPLE is an acronym for Semi-Implicit Method for Pressure Linked Equations. The SIMPLE algorithm was developed
SIMPLE_algorithm
American aerodynamicist and mathematician
Navier–Stokes Equations. Springer-Verlag. pp. 247–260. Fernando, B.; Sritharan, S. S. (2013). "Nonlinear Filtering of Stochastic Navier–Stokes Equation with
Sivaguru_S._Sritharan
Tool in computational fluid dynamics
common two-equation turbulence model, that is used as an approximation for the Reynolds-averaged Navier–Stokes equations (RANS equations). The model
K–omega_turbulence_model
Dimensionless quantity in fluid dynamics
around flight (free stream) M = 1 where approximations of the Navier-Stokes equations used for subsonic design no longer apply; the simplest explanation
Mach_number
Laws in physics about force and motion
Incorporating the effect of viscosity turns the Euler equation into a Navier–Stokes equation: ∂ v ∂ t + ( ∇ ⋅ v ) v = − 1 ρ ∇ P + ν ∇ 2 v + f , {\displaystyle
Newton's_laws_of_motion
Equations that describe the behavior of a physical system
In physics, equations of motion are equations that describe the behavior of a physical system in terms of its motion as a function of time. More specifically
Equations_of_motion
Equations to approximate global atmospheric flow
balance equations: A continuity equation: Representing the conservation of mass. Conservation of momentum: Consisting of a form of the Navier–Stokes equations
Primitive_equations
Numerical approximate solution to the Navier–Stokes equations
procedure in the field of computational fluid dynamics to solve the Navier–Stokes equations. This algorithm was developed by Van Doormal and Raithby in 1984. The
SIMPLEC_algorithm
Mathematical equation
the Kármán–Howarth equation (after Theodore von Kármán and Leslie Howarth 1938), which is derived from the Navier–Stokes equations, is used to describe
Kármán–Howarth_equation
Dimensionless quantity associated with free convection of a fluid
where g {\displaystyle g} is acceleration due to gravity. From the Stokes equation, when the volume of fluid is sinking, viscous drag is of the order
Rayleigh_number
Strain caused by an external load
along its length) Only small deflections are considered In this case, the equation describing beam deflection ( w {\displaystyle w} ) can be approximated
Bending
Study of electrically conducting fluids in the presence of electric fields
_{f}}}\right){\Bigr )}} This electrical force is then inserted in Navier-Stokes equation, as a body (volumetric) force. EHD covers the following types of particle
Electrohydrodynamics
Pseudovector field describing the local rotation of a continuum near some point
field in time is described by the vorticity equation, which can be derived from the Navier–Stokes equations. In many real flows where the viscosity can
Vorticity
Relative deformation of a physical body
the engineering strain e by e = λ − 1 {\displaystyle e=\lambda -1} This equation implies that when the normal strain is zero, so that there is no deformation
Strain_(mechanics)
Material property relevant for characterizing fluid flow
{\displaystyle \mu _{v}} . Volume viscosity appears in the classic Navier-Stokes equation if it is written for compressible fluid, as described in most books
Volume_viscosity
STOKES EQUATION
STOKES EQUATION
Surname or Lastname
English
English : variant of Stokes.
Biblical
that stones or is stoned; purple
Surname or Lastname
English
English : habitational name from Stanney in Cheshire, named with Old English stÄn ‘stone’, ‘rock’ + Ä“g ‘island’.
Surname or Lastname
English
English : habitational name from a minor place such as Stockey in Meeth, Devon, named from Old English stocc ‘stump’ + (ge)hæg ‘enclosure’, or a topographic name with the same meaning.
Surname or Lastname
English
English : variant of Stoke.
Surname or Lastname
English
English : topographic name for someone who lived by a prominent post or stake, for example a boundary marker, from Middle English stake ‘post’, ‘stake’, or from the same word used as a nickname for a tall, thin person.
Surname or Lastname
English
English : variant of Stone.
Surname or Lastname
English and German
English and German : variant of Stock.Probably an Americanized form of Stokke.
Surname or Lastname
English
English : unexplained; possibly a variant of Stocken, a topographic name for someone who lived by ‘(the) stumps’, from the weak plural of stocc ‘stump’.
Surname or Lastname
English
English : topographic name from Old Norse storð ‘brushwood’ or ‘young plantation’. There is a place so named in Cumbria (formerly in Lancashire), as well as a High Storrs in Sheffield, South Yorkshire, both named from this word.
Surname or Lastname
English
English : variant of Stokes.
Boy/Male
English
Stiles.
Surname or Lastname
English
English : habitational name from any of the numerous places throughout England named from Middle English stoke. The exact sense in individual cases is not clear; it seems to have meant originally merely ‘place’, and to have been used mainly for an outlying hamlet or dependent settlement.
Boy/Male
Biblical
That stones or is stoned, purple.
Boy/Male
English
From the village.
Surname or Lastname
English
English : habitational name for someone from any of the numerous places called Stoke.Dutch : occupational name for a stoker, Middle Dutch stokere, or from the same word in the sense ‘fire raiser’, ‘arsonist’.Scottish : occupational name for a trumpeter, Gaelic stocaire, an agent derivative of stoc ‘Gaelic trumpet’. The name is borne by a sept of the McFarlanes.
Surname or Lastname
English and Scottish
English and Scottish : from an agent derivative of Middle English stor ‘provisions’, ‘supplies’, hence an occupational name for an official in charge of dispensing provisions in a great house or monastery, or who collected rents paid in kind. The word stor was also used in the Middle Ages for livestock, and the surname may sometimes have denoted a keeper of animals.South German : from a Bavarian dialect word, storer, denoting an unskilled workman, i.e. someone who was not a member of a craft guild.
Surname or Lastname
English
English : variant spelling of Stiles.
Surname or Lastname
English
English : occupational name for someone who made and drove in stakes, or a topographic name for someone who lived near a boundary post for example, from a derivative of Middle English stake ‘post’, ‘stake’.
Boy/Male
English
Village
STOKES EQUATION
STOKES EQUATION
Boy/Male
Muslim
Lion
Girl/Female
Australian, Irish
From the Pure Pool
Girl/Female
Indian
Born of a mountain, Goddess Parvati, Daughter of Himalaya
Boy/Male
Indian, Sanskrit
Thunder
Girl/Female
Indian
Safe, Healthy, Happy
Boy/Male
Muslim
Servant of the Truth.
Boy/Male
Tamil
Souparno | ஸோஉஂபரà¯à®¨à¯‹Â
Jewel of jewels
Girl/Female
Muslim
Bright, White, Fair
Boy/Male
Muslim
A prophet of Allah
Boy/Male
Arabic, Muslim
Gift of the Merciful Allah
STOKES EQUATION
STOKES EQUATION
STOKES EQUATION
STOKES EQUATION
STOKES EQUATION
n.
One who makes or fits stocks, as of guns or gun carriages, etc.
n.
To wall or face with stones; to line or fortify with stones; as, to stone a well; to stone a cellar.
v. t.
To fasten, support, or defend with stakes; as, to stake vines or plants.
n.
One who walls with stones.
n.
One who strokes; also, one who pretends to cure by stroking.
n.
One who stones; one who makes an assault with stones.
v. t.
To mark the limits of by stakes; -- with out; as, to stake out land; to stake out a new road.
n.
One who smokes tobacco or the like.
a.
Characterized by a certain manner or style in speaking; -- often in composition; as, a pleasant-spoken man.
a.
Spoken with propriety; as, well-spoken words.
v. t.
To excavate in the form of stopes.
a.
Speaking with plain, unreserved sincerity; also, spoken sincerely; as, plain-spoken words.
a.
Spoken or speaking prettily.
v. t.
To furnish with spokes, as a wheel.
n.
To pelt, beat, or kill with stones.
a.
Speaking with directness; plain-spoken.
v. t.
Hence, by extension, an addition or amandment to a written composition; a touch; as, to give some finishing strokes to an essay.
a.
Collected or accumulated as a reserve supply; as, stored electricity.
a.
Uttered in speech; delivered by word of mouth; oral; as, a spoken narrative; the spoken word.
p. p.
Alt. of Stopen