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The angular velocity tensor is a skew-symmetric matrix defined by: Ω = ( 0 − ω z ω y ω z 0 − ω x − ω y ω x 0 ) {\displaystyle \Omega ={\begin{pmatrix}0&-\omega
Angular_velocity_tensor
Direction and rate of rotation
kinematics, angular velocity (symbol ω or ω → {\displaystyle {\vec {\omega }}} , the lowercase Greek letter omega), also known as the angular frequency
Angular_velocity
Scalar measure of the rotational inertia with respect to a fixed axis of rotation
change its angular momentum. The amount of torque needed to cause any given angular acceleration (the rate of change in angular velocity) is proportional
Moment_of_inertia
Conserved physical quantity; rotational analogue of linear momentum
L_{ij}=x_{i}p_{j}-x_{j}p_{i}\,.} The angular velocity can also be defined as an anti-symmetric second order tensor, with components ωij. The relation between
Angular_momentum
Angular momentum in special and general relativity
corresponding components for other objects and fields. The angular momentum tensor M is indeed a tensor, the components change according to a Lorentz transformation
Relativistic_angular_momentum
Physical object which does not deform when forces or moments are exerted on it
velocity. The angular momentum with respect to the center of mass is the same as without translation: at any time it is equal to the inertia tensor times
Rigid_body
Tensor used in continuum mechanics
The viscous stress tensor is a tensor used in continuum mechanics to model the part of the stress at a point within some material that can be attributed
Viscous_stress_tensor
Quasilinear first-order ordinary differential equation
{\displaystyle \mathbf {Q} } is the rotation tensor (not rotation matrix), an orthogonal tensor related to the angular velocity vector by ω × u = Q ˙ Q − 1 u {\displaystyle
Euler's equations (rigid body dynamics)
Euler's_equations_(rigid_body_dynamics)
Equations that describe the behavior of a physical system
rotational motion is described by the relativistic angular momentum tensor, including the spin tensor, which enter the equations of motion under covariant
Equations_of_motion
Assignment of a tensor continuously varying across a region of space
In mathematics and physics, a tensor field is a function assigning a tensor to each point of a region of a mathematical space (typically a Euclidean space
Tensor_field
Intrinsic quantum property of particles
theorem, the angular velocity is equal to the derivative of the Hamiltonian to its conjugate momentum, which is the total angular momentum operator J =
Spin_(physics)
Concept in physics
are torque-free. These concepts—the balance of angular momentum, the symmetry of the Cauchy stress tensor, and the Boltzmann Axiom—are interconnected, as
Balance_of_angular_momentum
Sum of directed areas in exterior algebra
bivectors such as the angular velocity tensor and the electromagnetic tensor, respectively a 3×3 and 4×4 skew-symmetric matrix or tensor. Real bivectors in
Bivector
Type of matrix
_{x}(t)&0\\\end{pmatrix}}} Dividing it by the time difference yields the angular velocity tensor: Ω = d Φ ( t ) d t = ( 0 − ω z ( t ) ω y ( t ) ω z ( t ) 0 − ω
Infinitesimal_rotation_matrix
Family of linear transformations
the bilinearity of the tensor product and the last step defines a 2-tensor on component form, or rather, it just renames the tensor u ⊗ v. These observations
Lorentz_transformation
Representation of mechanical stress at every point within a deformed 3D object
Cauchy stress tensor (symbol σ {\displaystyle {\boldsymbol {\sigma }}} , named after Augustin-Louis Cauchy), also called true stress tensor or simply stress
Cauchy_stress_tensor
Equations of motion for viscous fluids
stress tensor through a constitutive relation. By expressing the deviatoric (shear) stress tensor in terms of viscosity and the fluid velocity gradient
Navier–Stokes_equations
Physical quantity that expresses internal forces in a continuous material
the first and second Piola–Kirchhoff stress tensors, the Biot stress tensor, and the Kirchhoff stress tensor. Bending Compressive strength Critical plane
Stress_(mechanics)
Tensor describing energy momentum density in spacetime
stress-energy tensor The stress–energy tensor, sometimes called the stress–energy–momentum tensor or the energy–momentum tensor, is a tensor field quantity
Stress–energy_tensor
Exact solution for the Einstein field equations
admits a remarkable Killing tensor. There is a pair of principal null congruences (one ingoing and one outgoing). The Weyl tensor is algebraically special
Kerr_metric
Tensor in differential geometry
converge. Formally, it is a symmetric rank-two tensor obtained by taking a trace of the Riemann curvature tensor of a Riemannian or pseudo-Riemannian metric
Ricci_curvature
field. Tensors also have extensive applications in physics: Electromagnetic tensor (or Faraday's tensor) in electromagnetism Finite deformation tensors for
Introduction to the mathematics of general relativity
Introduction_to_the_mathematics_of_general_relativity
Rate of change in the linear deformation of a material with respect to time
some region are moving with the same velocity (same speed and direction) and/or rotating with the same angular velocity, as if that part of the medium were
Strain_rate
Model of rotating physical systems
frame—the normalized eigenvectors of the inertia tensor, which always can be chosen orthonormal, since the tensor is symmetric. When the rotor possesses a symmetry-axis
Rigid_rotor
Physical quantity that changes sign with improper rotation
compared to a true scalar or tensor. Physical examples of pseudovectors include angular velocity, angular acceleration, angular momentum, torque, magnetic
Pseudovector
Ways of writing certain laws of physics
t^{2}}-\nabla ^{2}.} The signs in the following tensor analysis depend on the convention used for the metric tensor. The convention used here is (+ − − −), corresponding
Covariant formulation of classical electromagnetism
Covariant_formulation_of_classical_electromagnetism
Formulation of classical mechanics
pearl sliding inside, the time-varying constraint forces like the angular velocity of the torus and the motion of the pearl in relation to the torus made
Lagrangian_mechanics
Concept in physics
In continuum mechanics, the strain-rate tensor or rate-of-strain tensor is a physical quantity that describes the rate of change of the strain (i.e.,
Strain-rate_tensor
Force acting on charged particles in electric and magnetic fields
{\boldsymbol {\sigma }}} is the Maxwell stress tensor, ∇ ⋅ {\displaystyle \nabla \cdot } denotes the tensor divergence, c {\displaystyle c} is the speed
Lorentz_force
Laws in physics about force and motion
t)-s(t)}{\Delta t}}.} Acceleration is to velocity as velocity is to position: it is the derivative of the velocity with respect to time. Acceleration can
Newton's_laws_of_motion
Study of the effects of forces on undeformable bodies
acceleration A of the reference particle as well as the angular velocity vector ω and angular acceleration vector α of the rigid system of particles as
Rigid_body_dynamics
Rate of change of acceleration with time
If its angular position as a function of time is θ(t), the angular velocity, acceleration, and jerk can be expressed as follows: Angular velocity, ω ( t
Jerk_(physics)
velocity and acceleration in another frame F' moving at translational velocity V or angular velocity Ω relative to F. Conversely F moves at velocity (—V
List of equations in classical mechanics
List_of_equations_in_classical_mechanics
Component of stress coplanar with a material cross section
shear tensor (a second-order tensor) is proportional to the flow velocity gradient (the velocity is a vector, so its gradient is a second-order tensor): τ
Shear_stress
Representation of a tensor in Euclidean space
a Cartesian tensor uses an orthonormal basis to represent a tensor in a Euclidean space in the form of components. Converting a tensor's components from
Cartesian_tensor
Equations describing classical electromagnetism
one formalism. In the tensor calculus formulation, the electromagnetic tensor Fαβ is an antisymmetric covariant order 2 tensor; the four-potential, Aα
Maxwell's_equations
Effect of a material on light
different velocities. Group-velocity dispersion is quantified as the derivative of the reciprocal of the group velocity with respect to angular frequency
Dispersion_(optics)
Geometric object that has length and direction
example of a pseudovector is angular velocity. Driving in a car, and looking forward, each of the wheels has an angular velocity vector pointing to the left
Euclidean_vector
Array of numbers describing a metric connection
corresponding gravitational potential being the metric tensor. When the coordinate system and the metric tensor share some symmetry, many of the Γijk are zero
Christoffel_symbols
Mathematical operation on vectors in 3D space
seen as the (1,2)-tensor (a mixed tensor, specifically a bilinear map) obtained from the 3-dimensional volume form, a (0,3)-tensor, by raising an index
Cross_product
Proposed theories of gravity
Minkowski metric. g μ ν {\displaystyle g_{\mu \nu }\;} is a tensor, usually the metric tensor. These have signature (−,+,+,+). Partial differentiation is
Alternatives to general relativity
Alternatives_to_general_relativity
Solution of Einstein field equations
}}}={\frac {a\left(2r-Q^{2}\right)}{\chi }}} is the frame dragging induced angular velocity. The shorthand term χ {\displaystyle \chi } is defined by χ = ( a 2
Kerr–Newman_metric
Frame-dependent apparent force in Physics
force, which arises when a rotating system changes its angular velocity (i.e., due to angular acceleration). While these forces are not real in the sense
Fictitious_force
Movement of an object which leaves at least one point unchanged
type of angular velocity (spin angular velocity and orbital angular velocity) and angular momentum (spin angular momentum and orbital angular momentum)
Rotation
Influence that can change motion of an object
the tensor) as well as shear terms associated with forces that act parallel to the cross-sectional area (the off-diagonal elements). The stress tensor accounts
Force
Movement of an object's magnetic moment axis about a magnetic field
and the angular momentum. The angular momentum vector J → {\displaystyle {\vec {J}}} precesses about the external field axis with an angular frequency
Larmor_precession
Solution of Einstein field equations
Riemann tensor can be computed into three pieces, the tidal or electrogravitic tensor (which represents tidal forces), the magnetogravitic tensor (which
Gödel_metric
Pseudovector field describing the local rotation of a continuum near some point
is the three-dimensional Levi-Civita tensor. The vorticity tensor is simply the antisymmetric part of the tensor ∇ v {\displaystyle \nabla \mathbf {v}
Vorticity
circular orbits are permissible and valid. The Ricci curvature tensor is a special curvature tensor given by the contraction R α β ≡ R ν α ν β {\displaystyle
Theoretical motivation for general relativity
Theoretical_motivation_for_general_relativity
Physical quantities taking values at each point in space and time
example of a vector field. Strain tensor, representing the deformation of matter caused by stress, is an example of a tensor field. Field theories, mathematical
Field_(physics)
Measurable property of a material or system
for its velocity are u, u, or u → {\displaystyle {\vec {u}}} . Scalar and vector quantities are the simplest tensor quantities, which are tensors that can
Physical_quantity
for determining the complete elastic tensor, c i j k l {\displaystyle c_{ijkl}} , of solids. The elastic tensor is an 81 component 3x3x3x3 matrix which
Brillouin_spectroscopy
Branch of physics which studies the behavior of materials modeled as continuous media
stress tensor, and ρ 0 {\displaystyle \rho _{0}} is the mass density in the reference configuration. The first Piola-Kirchhoff stress tensor is related
Continuum_mechanics
Rigid body equations in classical mechanics
velocity of the center of mass τ = total torque acting about the center of mass Icm = moment of inertia about the center of mass ω = angular velocity
Newton–Euler_equations
Algebraic operation on coordinate vectors
(single-) dot product between a tensor of order n {\displaystyle n} and a tensor of order m {\displaystyle m} is a tensor of order n + m − 2 {\displaystyle
Dot_product
Geometric method for visualizing a rotating rigid body
expressed in terms of the moment of inertia tensor I {\displaystyle \mathbf {I} } and the angular velocity vector ω {\displaystyle {\boldsymbol {\omega
Poinsot's_ellipsoid
Algebra associated to any vector space
alternating tensor subspace. On the other hand, the image A ( T ( V ) ) {\displaystyle {\mathcal {A}}(\mathrm {T} (V))} is always the alternating tensor graded
Exterior_algebra
Polish physicist (born 1975)
the four-angular momentum is related to a generator of rotation in the Lorentz group. From the covariant conservation laws for the spin tensor and energy–momentum
Nikodem_Popławski
transformation properties (i.e. whether the quantity is a scalar, vector, matrix or tensor), and whether the quantity is conserved. List of photometric quantities
List_of_physical_quantities
Type of fluid flow
}{|\mathbf {r} |^{3}}}\right)} is a second-rank tensor (or more accurately tensor field) known as the Oseen tensor (after Carl Wilhelm Oseen). Here, r r is a
Stokes_flow
Fluid dynamics theory on gravity waves
wave energy density flux, S is the radiation stress tensor and ∇U is the mean-velocity shear rate tensor. In this equation in non-conservation form, the Frobenius
Airy_wave_theory
fluid dynamics, Faxén's laws relate a sphere's velocity U {\displaystyle \mathbf {U} } and angular velocity Ω {\displaystyle \mathbf {\Omega } } to the forces
Faxén's_law
Type of derivative in differential geometry
differentiable manifold. Functions, tensor fields and forms can be differentiated with respect to a vector field. If T is a tensor field and X is a vector field
Lie_derivative
Description of the orientation of a rigid body
principal axes) in which the moment of inertia tensor has only three components. The angular velocity of a rigid body takes a simple form using Euler
Euler_angles
Figure formed by two rays meeting at a common point
metric tensor is used to define the angle between two tangents. Where U and V are tangent vectors and gij are the components of the metric tensor G, cos
Angle
Calculus of vector-valued functions
(p,q)} tensor can be formed by taking a tensor product of a ( p , 0 ) {\displaystyle (p,0)} tensor and a ( 0 , q ) {\displaystyle (0,q)} tensor, which
Vector_calculus
Property of a mass in motion
of both linear momentum and angular momentum. To distinguish it from generalized momentum, the product of mass and velocity is also referred to as mechanical
Momentum
Equation
specifying the stress tensor through a constitutive relation. By expressing the shear tensor in terms of viscosity and fluid velocity, and assuming constant
Cauchy_momentum_equation
Theory of motion and forces for objects close to the speed of light
collected into four vectors, or four-dimensional tensors. The six-component angular momentum tensor is sometimes called a bivector because in the 3D viewpoint
Relativistic_mechanics
Branch of mechanics concerned with balance of forces in nonmoving systems
dynamics, describing the relationship between angular momentum and angular velocity, torque and angular acceleration, and several other quantities. The
Statics
Dynamic disturbance in a medium or field
is a number; for a vector field it is a vector; in general a tensor field has a tensor value. The value of x {\displaystyle x} is a point of space, specifically
Wave
Equation describing the evolution of the vorticity of a fluid particle as it flows
derivative operator, u is the flow velocity, ρ is the local fluid density, p is the local pressure, τ is the viscous stress tensor and B represents the sum of
Vorticity_equation
Mathematical description of spacetime used in relativity
provide a basis for the cotangent space at p. The tensor product (denoted by the symbol ⊗) yields a tensor field of type (0, 2), i.e. the type that expects
Minkowski_spacetime
Analogies between Maxwell's and Einstein's field equations
second order stress–energy tensor, as opposed to the source of the electromagnetic field being the first order four-current tensor. This difference becomes
Gravitoelectromagnetism
Superseded theory of electromagnetism
Gauss and Wilhelm Eduard Weber. In this theory, Coulomb's law becomes velocity and acceleration dependent. Weber electrodynamics is only applicable for
Weber_electrodynamics
Physical system that responds to a restoring force proportional to displacement
on the amplitude). If a frictional force (damping) proportional to the velocity is also present, the harmonic oscillator is described as a damped oscillator
Harmonic_oscillator
Term in physical oceanography
mean flow. The radiation stresses behave as a second-order tensor. The radiation stress tensor describes the additional forcing due to the presence of the
Radiation_stress
Specification of a derivative along a tangent vector of a manifold
fields) and to arbitrary tensor fields, in a unique way that ensures compatibility with the tensor product and trace operations (tensor contraction). Given
Covariant_derivative
Mathematical theory of the geometry of space and time
instead characterized by the Riemann curvature tensor. In flat spaces, the components of the curvature tensor vanish even when the metric coefficients and
Curved_spacetime
Physical theory describing classical fields
formulation using tensor fields was found. Instead of using two vector fields describing the electric and magnetic fields, a tensor field representing
Classical_field_theory
Subfield of astronomy
astrophysical jets and accretion disks. Chandrasekhar potential energy tensor – Tensor formalism for gravitational stability in self-gravitating systems.
Outline_of_astrophysics
Periodic change in the direction of a rotation axis
fixed internal moment of inertia tensor I0 and fixed external angular momentum L, the instantaneous angular velocity is ω ( R ) = R I 0 − 1 R T L {\displaystyle
Precession
Theory of interwoven space and time by Albert Einstein
macroscopic gyroscope, relating the angular velocity of the spin of a particle following a curvilinear orbit to the angular velocity of the orbital motion. Thomas
Special_relativity
Physical constant equal to the speed of light
steady speed but changing velocity v, the effect on the orbit is order v2/c2, and the effect preserves energy and angular momentum, so that orbits do
Speed_of_gravity
Vector used in astronomy
{F} (r)=-k\mathbf {r} ,} the angular momentum vector is conserved and the motion lies in a plane. The conserved dyadic tensor can be written in a simple
Laplace–Runge–Lenz_vector
Tensor formulation of non-relativistic physics
constructed a similar tensor formulation in the context of Newton–Cartan theory. Some other authors also have developed a similar Galilean tensor formalism. The
Galilei-covariant tensor formulation
Galilei-covariant_tensor_formulation
Straight path on a curved surface or a Riemannian manifold
and real trees. In a Riemannian manifold M {\displaystyle M} with metric tensor g {\displaystyle g} , the length L {\displaystyle L} of a continuously differentiable
Geodesic
Physical constant for the strength of gravity induced by a mass
is the Einstein tensor (not the gravitational constant despite the use of G), Λ is the cosmological constant, gμν is the metric tensor, Tμν is the stress–energy
Gravitational_constant
Object with escape velocity exceeding the speed of light
space-time components of general relativity's Riemann curvature tensor, the curvature tensor only contains purely spatial components, and both forms of curvature
Dark star (Newtonian mechanics)
Dark_star_(Newtonian_mechanics)
Quantum mechanical waves describing matter
k}}={\frac {d\nu }{d(1/\lambda )}}} (The modern definition of group velocity uses angular frequency ω and wave number k). By applying the differentials to
Matter_wave
energy–momentum tensor and the Petrov classification of the Weyl tensor. There are various methods of classifying these tensors, some of which use tensor invariants
Mathematics of general relativity
Mathematics_of_general_relativity
Attraction of masses and energy
T_{\mu \nu },} where Gμν is the Einstein tensor, gμν is the metric tensor, Tμν is the stress–energy tensor, Λ is the cosmological constant, G {\displaystyle
Gravity
General relativity equation
V^{\mu }} is the four-velocity of some reference point X μ {\displaystyle X^{\mu }} in the body, and the skew-symmetric tensor S μ ν {\displaystyle S^{\mu
Mathisson–Papapetrou–Dixon equations
Mathisson–Papapetrou–Dixon_equations
Theory of gravitation as curved spacetime
stress–energy tensor, which includes both energy and momentum densities as well as stress: pressure and shear. Using the equivalence principle, this tensor is readily
General_relativity
Constant of motion in the Kerr-Newman spacetime
where u {\displaystyle u} is the four-velocity of the particle in motion. The components of the Killing tensor in Boyer–Lindquist coordinates are: K μ
Carter_constant
Models and algorithms for simulating collision and reaction
(1a) and (1b) Compute new angular velocities ω ′ i {\displaystyle \mathbf {\omega '} _{i}} in terms of old angular velocities ω i {\displaystyle \mathbf
Collision_response
alpha (α). Just like angular velocity, there are two types of angular acceleration: spin angular acceleration and orbital angular acceleration, representing
Glossary_of_physics
Formulation of classical mechanics using momenta
William Rowan Hamilton, Hamiltonian mechanics replaces (generalized) velocities q ˙ i {\displaystyle {\dot {q}}^{i}} used in Lagrangian mechanics with
Hamiltonian_mechanics
Vector in relativity
definition, see tensor. All four-vectors transform in the same way, and this can be generalized to four-dimensional relativistic tensors; see special relativity
Four-vector
Model of electrically conducting fluids
Magnetohydrodynamic sensors are used for precise measurements of angular velocity in inertial navigation systems such as those used in aerospace engineering
Magnetohydrodynamics
ANGULAR VELOCITY-TENSOR
ANGULAR VELOCITY-TENSOR
Girl/Female
Christian & English(British/American/Australian)
Angelic
Girl/Female
Afghan, American, British, Christian, English, Finnish, French, Greek, Indian, Irish, Lebanese, Polish, Portuguese, Romanian, Spanish, Swedish, Tamil
Heavenly Messenger; Angel; Messenger from God
Boy/Male
Muslim/Islamic
Felicity
Girl/Female
French American English Latin
Great happiness.
Boy/Male
Gujarati, Hindu, Indian, Kannada
Spark of Fire
Boy/Male
Arabic, Hindu, Indian, Muslim
Shining
Boy/Male
Hindu
Velocity
Female
English
Feminine form of Latin Angelus, ANGELA means "angel, messenger."
Boy/Male
Tamil
Velocity
Boy/Male
Indian, Sanskrit
Radiant; Bright; Enlightening
Girl/Female
Muslim
Happiness. Bliss. Felicity.
Female
English
English form of French Félicie, FELICITY means "happy" or "lucky."
Girl/Female
American, Australian, British, Chinese, Christian, English, French, Jamaican, Latin
Happy; Good Fortune; Great Happiness; Lucky; Fortunate
Girl/Female
Muslim/Islamic
Bliss felicity
Girl/Female
Indian, Tamil
Lovely; Kind-hearted
Girl/Female
Muslim
Happiness. Bliss. Felicity.
Boy/Male
Hindu, Indian, Kannada, Tamil
Witty; Super
Boy/Male
Indian, Sanskrit
Praising; A Hymn
Girl/Female
French Spanish American Italian Latin Greek
Angel.
Girl/Female
American, Australian, British, English
Beautiful Goddess
ANGULAR VELOCITY-TENSOR
ANGULAR VELOCITY-TENSOR
Male
English
 Anglicized form of Greek Nachor (Hebrew Nachowr), NAHOR means "snoring" or "snorting." In the bible, this is the name of the son of Terah and brother of Abraham. Compare with another form of Nahor.
Girl/Female
Tamil
Lotus flower, Pure and Lovely
Boy/Male
American, Christian, Gaelic, Indian
Unusual Beard; Muddy Place; Ditch
Surname or Lastname
English
English : variant of Blunt.
Male
English
Anglicized form of Greek Sampson (Hebrew Shimshown), SAMSON means "like the sun." In the bible, this is the name of a powerful hero who was betrayed by his mistress Delila.
Girl/Female
Australian, Jamaican
Wild Spirit
Boy/Male
Arabic, Muslim
Reviver of the Faith
Boy/Male
Muslim
The subtle one
Male
Irish
Modern form of Old Irish Coemgen, CAÉMGEN means "little comely one."
Surname or Lastname
English
English : from a Germanic personal name introduced to Britain from France by the Normans, composed of an unexplained first element (possibly akin to Old Norse beinn ‘straight’) + hard ‘brave’, ‘hardy’, ‘strong’.
ANGULAR VELOCITY-TENSOR
ANGULAR VELOCITY-TENSOR
ANGULAR VELOCITY-TENSOR
ANGULAR VELOCITY-TENSOR
ANGULAR VELOCITY-TENSOR
a.
Measured by an angle; as, angular distance.
n.
A pleasing faculty or accomplishment; as, felicity in painting portraits, or in writing or talking.
n.
Savage wildness or fierceness; fury; cruelty; as, ferocity of countenance.
adv.
In an angular manner; with of at angles or corners.
n.
The quality or state of being veracious; habitual observance of truth; truthfulness; truth; as, a man of veracity.
a.
Relating to an angle or to angles; having an angle or angles; forming an angle or corner; sharp-cornered; pointed; as, an angular figure.
a.
Fig.: Lean; lank; raw-boned; ungraceful; sharp and stiff in character; as, remarkably angular in his habits and appearance; an angular female.
a.
Constituted, selected, or conducted in conformity with established usages, rules, or discipline; duly authorized; permanently organized; as, a regular meeting; a regular physican; a regular nomination; regular troops.
a.
Of or pertaining to the jugular vein; as, the jugular foramen.
n.
Quickness of motion; swiftness; speed; celerity; rapidity; as, the velocity of wind; the velocity of a planet or comet in its orbit or course; the velocity of a cannon ball; the velocity of light.
adv.
In an angular manner; angularly.
v. t.
To make angular.
n.
The singular number, or the number denoting one person or thing; a word in the singular number.
a.
Not angular.
a.
Conformed to a rule; agreeable to an established rule, law, principle, or type, or to established customary forms; normal; symmetrical; as, a regular verse in poetry; a regular piece of music; a regular verb; regular practice of law or medicine; a regular building.
a.
Pertaining to, or having the form of, a ring; forming a ring; ringed; ring-shaped; as, annular fibers.
a.
Having the form of a ring; annular.
a.
Thorough; complete; unmitigated; as, a regular humbug.
a.
Having all the parts of the same kind alike in size and shape; as, a regular flower; a regular sea urchin.
pl.
of Ungula