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The partial specific volume v i ¯ , {\displaystyle {\bar {v_{i}}},} express the variation of the extensive volume of a mixture in respect to composition
Partial_specific_volume
Volume occupied per unit mass
{V}{m}}={\frac {RT}{PM}}} Specific volume is commonly applied to: Molar volume Volume (thermodynamics) Partial molar volume Imagine a variable-volume, airtight chamber
Specific_volume
Heat required to raise the temperature of a given unit of mass of a substance
constant volume, respectively. The specific heat capacity of a material on a per-mass basis is c = ∂ C ∂ m , {\displaystyle c={\frac {\partial C}{\partial m}}
Specific_heat_capacity
Change in a property of a mixture component with respect to amount
partial molar property. The partial molar volume is broadly understood as the contribution that a component of a mixture makes to the overall volume of
Partial_molar_property
Thermodynamic quantity
ratio of specific heats, or Laplace's coefficient, is the ratio of the heat capacity at constant pressure (CP) to heat capacity at constant volume (CV).
Heat_capacity_ratio
Physical property of matter
dQ=\left({\frac {\partial U}{\partial T}}\right)_{V}dT+\left({\frac {\partial U}{\partial V}}\right)_{T}dV+pdV} For a constant volume ( d V = 0 {\displaystyle
Heat_capacity
Mass per unit volume
Density (volumetric mass density or specific mass) is the ratio of a substance's mass to its volume. The symbol most often used for density is ρ (the
Density
Derivative of a function with multiple variables
{\partial ^{2}f}{\partial y\,\partial x}}={\frac {\partial }{\partial y}}\left({\frac {\partial f}{\partial x}}\right)=(f'_{x})'_{y}=f''_{xy}=\partial _{yx}f=\partial
Partial_derivative
Topics referred to by the same term
PSV may refer to: Papa Stour Airstrip (IATA code PSV) Partial specific volume Peak systolic velocity Petit Saint Vincent, an island south of St. Vincent
PSV
Properties independent of system size, and proportional to system size
(or electrical conductivity) specific heat capacity, cp specific internal energy, u specific rotation, [α] specific volume, v standard reduction potential
Intensive and extensive properties
Intensive_and_extensive_properties
Serum albumin protein derived from cows
(monomer), 6.7 (dimer) Diffusion constant, D20,W × 10−7 cm2/s: 5.9 Partial specific volume, V20: 0.733 Intrinsic viscosity, η: 0.0413 Frictional ratio, f/f0:
Bovine_serum_albumin
Parameter used to calculate the volume change of a fluid or solid in response to pressure
V ∂ p {\displaystyle \beta =-{\frac {1}{V}}{\frac {\partial V}{\partial p}}} , where V is volume and p is pressure. The choice to define compressibility
Compressibility
Extensive parameter used to describe a thermodynamic system's state
thermodynamics, the volume of a system is an important extensive parameter for describing its thermodynamic state. The specific volume, an intensive property
Volume_(thermodynamics)
Equation of the state of a hypothetical ideal gas
written in terms of the specific volume v, the reciprocal of density, as p v = R specific T . {\displaystyle pv=R_{\text{specific}}T.} It is common, especially
Ideal_gas_law
Tendency of matter to change volume in response to a change in temperature
{\frac {1}{V}}\left({\frac {\partial V}{\partial T}}\right)_{p}={\frac {1}{V_{m}}}\left({\frac {\partial V_{m}}{\partial T}}\right)_{p}={\frac {1}{V_{m}}}\left({\frac
Thermal_expansion
Thermodynamic cycle for spark ignition piston engines
giving the terms units of joules/kg (specific energy), meters3/kg (specific volume), or joules/(kelvin·kg) (specific entropy, heat capacity) etc. and would
Otto_cycle
Force distributed over an area
conjugate to volume. It is defined as a derivative of the internal energy of a system: p = − ( ∂ U ∂ V ) S , N , {\displaystyle p=-\left({\frac {\partial U}{\partial
Pressure
Energy contained within a system
T\left({\frac {\partial S}{\partial T}}\right)_{V}} is the heat capacity at constant volume C V . {\displaystyle C_{V}.} The partial derivative of S {\displaystyle
Internal_energy
Partial differential relations in thermodynamics
{\frac {\partial }{\partial x_{j}}}\left({\frac {\partial \Phi }{\partial x_{i}}}\right)={\frac {\partial }{\partial x_{i}}}\left({\frac {\partial \Phi }{\partial
Maxwell_relations
Mathematical model which approximates the behavior of real gases
where U is the internal energy ĉV is the dimensionless specific heat capacity at constant volume, approximately 3/2 for a monatomic gas, 5/2 for diatomic
Ideal_gas
Measure of energy in a thermodynamic system
(mass per unit volume), h is the specific enthalpy (enthalpy per unit mass), ρh represents the enthalpy density (enthalpy per unit volume), dV denotes an
Enthalpy
Protein without a fixed 3D structure
also be a sign of disorder. Folded proteins have a high density (partial specific volume of 0.72-0.74 mL/g) and commensurately small radius of gyration
Intrinsically disordered proteins
Intrinsically_disordered_proteins
Thermodynamic process in which no mass or heat is exchanged with surroundings
expressed as E = γP, where γ is the ratio of specific heats at constant pressure and at constant volume ( γ = Cp/Cv) and P is the pressure of the gas
Adiabatic_process
Thermodynamic process in which pressure remains constant
the molar specific heat capacity at constant pressure (cp) is 7/2R or 29.1006 J mol−1 deg−1. The molar heat capacity at constant volume (cv) is 5/2R
Isobaric_process
Thermodynamic cycle
changes with an increase in pressure ratio. Figure 2 indicates how the specific power output changes with an increase in the gas turbine inlet temperature
Brayton_cycle
Thermodynamic process of a closed system in which volume remains constant
U = d Q {\displaystyle dU=dQ} Using the definition of specific heat capacity at constant volume, cv = (dQ/dT)/m, where m is the mass of the gas, we get
Isochoric_process
Equations in thermodynamics
\over V}\left({\partial V \over \partial p}\right)_{T,N{\text{ or }}S,N}} Specific heat (per-particle) at constant pressure or constant volume c p or V =
Thermodynamic_equations
Type of differential equation
mathematics, a partial differential equation (PDE) is an equation which involves a multivariable function and one or more of its partial derivatives. The
Partial_differential_equation
Thermodynamic process
exactly define intensive quantities (such as pressure, temperature, specific volume, specific entropy) of the system at any instant during the whole process;
Quasistatic_process
Number and arrangement of multiple folded protein subunits in a multi-subunit complex
mass can be inferred from its volume using the partial specific volume of 0.73 ml/g. However, volume measurements are less certain than mass measurements
Protein_quaternary_structure
Method of separating particles in a mixture
pellets.[citation needed] Sedimentation depends on mass, shape, and partial specific volume of a macromolecule, as well as solvent density, rotor size and
Differential_centrifugation
Observational basis of thermodynamics
Continuum Mechanics and Partial Differential Equations. Proceedings of the International Symposium on Continuum Mechanics and Partial Differential Equations
Laws_of_thermodynamics
Phenomenon of non-ideal fluids changing temperature
gas. Combined with the specific heat capacity at constant pressure c P = ( ∂ h / ∂ T ) P {\displaystyle c_{P}=(\partial h/\partial T)_{P}} it allows the
Joule–Thomson_effect
Performance measure of a device that uses thermal energy
heat engine due to temperature, called the Carnot efficiency. Second, specific types of engines have lower limits on the ideal efficiency of the engine
Thermal_efficiency
Thermodynamic cycle
issued 1886-02-16 Clerk, Dugald (1913). The gas, petrol, and oil engine, Volume 2. J. Wiley. p. 210. Heywood, John B. Internal Combustion Engine Fundamentals
Atkinson_cycle
Relations between flows and forces, or gradients, in thermodynamic systems
{\partial s}{\partial t}}+\nabla \cdot \mathbf {J} _{s}={\frac {\partial s_{c}}{\partial t}}} where ∂ s c / ∂ t {\textstyle {\partial s_{c}}/{\partial t}}
Onsager_reciprocal_relations
Thermodynamic process with no change in enthalpy
H; or specific enthalpy, h. If a steady-state, steady-flow process is analysed using a control volume, everything outside the control volume is considered
Isenthalpic_process
Mass fraction of a saturated mixture which is vapor
either specific enthalpy, specific entropy, specific volume or specific internal energy, y f {\displaystyle y_{f}} is the value of the specific property
Vapor_quality
State variables for near-critical fluids
the Peng–Robinson equation of state. The reduced specific volume (or "pseudo-reduced specific volume") of a fluid is computed from the ideal gas law at
Reduced_properties
Physical law for entropy and heat
function of its entropy S, volume V, and mol number N, i.e. U = U (S, V, N), then the temperature is equal to the partial derivative of the internal energy
Second_law_of_thermodynamics
Type of thermodynamic potential
{\displaystyle \left({\frac {\partial {\mathcal {E}}}{\partial T}}\right)_{Q_{\mathrm {ele} },p}=-\left({\frac {\partial S}{\partial Q_{\mathrm {ele} }}}\right)_{T
Gibbs_free_energy
Thermodynamic potential
{-{\frac {\partial }{\partial \beta }}e^{-\beta E_{r}}}{Z}}={\frac {-{\frac {\partial }{\partial \beta }}\sum _{r}e^{-\beta E_{r}}}{Z}}=-{\frac {\partial \log
Helmholtz_free_energy
Diagram showing the relationship between pressure and volume in a system
[citation needed] Note that in some cases specific volume will be plotted on the x-axis instead of volume, in which case the area under the curve represents
Pressure–volume_diagram
Imaginary volume through which a substance's flow is modeled and analyzed
dp={\frac {\partial p}{\partial t}}dt+{\frac {\partial p}{\partial x}}dx+{\frac {\partial p}{\partial y}}dy+{\frac {\partial p}{\partial z}}dz} (the total
Control_volume
Initial step in the phase transition or molecular self-assembly of a substance
before a new phase or self-organised structure appears. For example, if a volume of water is cooled (at atmospheric pressure) significantly below 0 °C, it
Nucleation
Thermodynamic process
relation: p V n = C {\displaystyle pV^{n}=C} where p is the pressure, V is volume, n is the polytropic index, and C is a constant. The polytropic process
Polytropic_process
Idealized thermodynamic cycle
in the same ratio as QH/TH. When a Carnot cycle is plotted on a pressure–volume diagram (Figure 1), the isothermal stages follow the isotherm lines for
Carnot_cycle
Thermodynamic process that is reversible and adiabatic
{\displaystyle C_{p}} = molar specific heat at constant pressure, C v {\displaystyle C_{v}} = molar specific heat at constant volume. Gas laws Adiabatic process
Isentropic_process
Model that is used to predict the performance of steam turbine systems
equations[1] is derived from the energy and mass balance for a control volume. Q ˙ in m ˙ = h 3 − h 2 , {\displaystyle {\frac {{\dot {Q}}_{\text{in}}}{\dot
Rankine_cycle
Assembly of heat engines that work in tandem from the same source of heat
electrical load, because duct burners can have very good efficiency with partial loads. It can enable higher steam production to compensate for the failure
Combined-cycle_power_plant
Property of a thermodynamic system
, N ⇒ ⋯ ⇒ d S = d Q T {\displaystyle T:={\left({\frac {\partial U}{\partial S}}\right)}_{V,N}\ \Rightarrow \ \cdots \ \Rightarrow \ \mathrm {d}
Entropy
Absorption refrigerator invented in 1930
Pressure / Volume Chemical potential / Particle number Vapor quality Reduced properties Material properties Property databases Specific heat capacity
Einstein_refrigerator
Thermodynamic phase transition energy
used the term in the context of calorimetry where a heat transfer caused a volume change in a body while its temperature was constant. In contrast to latent
Latent_heat
Correction factor which describes the deviation of a real gas from ideal gas behavior
reduced specific volume must be found. Unlike the reduced pressure and temperature, the reduced specific volume is not found by using the critical volume. The
Compressibility_factor
{\displaystyle \pi _{T}} . It is defined as a partial derivative of internal energy with respect to volume at constant temperature: π T = ( ∂ U ∂ V ) T
Internal_pressure
Thermodynamic cycle
Pressure / Volume Chemical potential / Particle number Vapor quality Reduced properties Material properties Property databases Specific heat capacity
Miller_cycle
State of thermodynamic systems where no net flow of matter or energy occurs
states that gases dissolve in direct proportion to their partial pressures. By influencing the partial pressure on the top of a closed system, this would help
Thermodynamic_equilibrium
Physical law for definition of temperature
P1V1/N1 = P2V2/N2 where Pi is the pressure in the ith system, Vi is the volume, and Ni is the amount (in moles, or simply the number of atoms) of gas.
Zeroth_law_of_thermodynamics
Thermodynamic process in which temperature remains constant
gas volume. For an isothermal (constant temperature T), reversible process, this integral equals the area under the relevant PV (pressure-volume) isotherm
Isothermal_process
Equations on thermodynamic quantities
the volume of the system constant, the change of entropy satisfies d S = ( ∂ S ∂ T ) V d T {\displaystyle dS=\left({\frac {\partial S}{\partial T}}\right)_{V}dT}
Fundamental thermodynamic relation
Fundamental_thermodynamic_relation
Function describing equilibrium states of a system
Entropy (S) Pressure (P) Temperature (T) Volume (V) Chemical composition Pressure altitude Specific volume (v) or its reciprocal density (ρ) Particle
State_function
Law of thermodynamics establishing the conservation of energy
variables S, entropy, and V, volume: U = U (S, V). In these terms, T, the system's temperature, and P, its pressure, are partial derivatives of U with respect
First_law_of_thermodynamics
T}}\right)_{P}\quad =-{\frac {T}{N}}\,{\frac {\partial ^{2}G}{\partial T^{2}}}} Specific heat at constant volume c V = T N ( ∂ S ∂ T ) V = − T N ∂ 2 A ∂ T
Material properties (thermodynamics)
Material_properties_(thermodynamics)
Type of energy transfer
system, which always occur in conjugate pairs, for example pressure and volume or magnetic flux density and magnetization. In the International System
Work_(thermodynamics)
Refrigerator that uses a heat source
a low partial pressure environment, thus extracting heat from its surroundings (e.g. the refrigerator's compartment). Because of the low partial pressure
Absorption_refrigerator
Equation describing a state of matter under a given set of conditions
between volume and temperature: V 1 T 1 = V 2 T 2 . {\displaystyle {\frac {V_{1}}{T_{1}}}={\frac {V_{2}}{T_{2}}}.} Dalton's law (1801) of partial pressure
Equation_of_state
Engine combustion process
{\displaystyle p} is pressure and V the volume or v {\displaystyle v} the specific volume if the process is placed on a unit mass basis. The idealized Diesel
Diesel_cycle
Measure of how much alcohol is in a liquid
causes a decrease in volume. The phenomenon of volume changes due to mixing dissimilar solutions is called "partial molar volume". Water and ethanol are
Alcohol_by_volume
Solvent property in polymer science
osmotic pressure ( Π {\displaystyle \Pi } ) and the solvent's partial specific volume ( v s {\displaystyle v_{s}} ): Δ μ 1 = − v s Π {\displaystyle \Delta
Theta_solvent
isentrope drawn on the specific volume versus pressure plane. Specifically, the Landau derivative is a second derivative of specific volume with respect to pressure
Landau_derivative
German physicist and physiologist (1821–1894)
seem linear, a fact that is used in current electronic devices to control volume. Helmholtz paved the way in experimental studies on the relationship between
Hermann_von_Helmholtz
Body of matter in a state of internal equilibrium
the initial value ξ i 0 {\displaystyle \xi _{i}^{0}} equal to zero. The specific contribution to the thermodynamics of open non-equilibrium systems was
Thermodynamic_system
Graph relating temperature and entropy during a thermodynamic process or cycle
thermodynamic diagram used to visualize changes to temperature (T ) and specific entropy (s) during a thermodynamic process or cycle as the graph of a curve
Temperature–entropy_diagram
Law of physics
assumption.[citation needed] On the other hand, the molar specific heat at constant volume of a monatomic classical ideal gas, such as helium at room
Third_law_of_thermodynamics
System that converts heat or thermal energy to mechanical work
sink) isobaric (at constant pressure) isometric/isochoric (at constant volume), also referred to as iso-volumetric adiabatic (no heat is added or removed
Heat_engine
Scalar physical quantities representing system states
temperature and convex function of volume. ( ∂ 2 H ∂ P 2 ) S , N ≤ 0 {\displaystyle {\biggl (}{\frac {\partial ^{2}H}{\partial P^{2}}}{\biggr )}_{S,N}\leq 0}
Thermodynamic_potential
Type of energy transfer
_{S_{1}}^{S_{2}}\left({\frac {\partial H}{\partial S}}\right)_{P}\mathrm {d} S+\int _{P_{1}}^{P_{2}}\left({\frac {\partial H}{\partial P}}\right)_{S}\mathrm {d}
Heat
Passage of a system from an initial to a final state of thermodynamic equilibrium
shown. Each process has a well-defined start and end point in the pressure-volume state space. In this particular example, processes 1 and 3 are isothermal
Thermodynamic_process
English physical chemist
Davies, David Gwynne; Bury, Charles R. (1930). "CCLXXXIX.—The partial specific volume of potassium n-octoate in aqueous solution". J. Chem. Soc.: 2263–2267
Charles_Rugeley_Bury
Set of quasilinear hyperbolic equations governing adiabatic and inviscid flow
thermodynamics is the opposite of the partial derivative of the specific internal energy with respect to the specific volume: p ( v , s ) = − ∂ e ( v , s ) ∂
Euler equations (fluid dynamics)
Euler_equations_(fluid_dynamics)
Volume of fluid which passes per unit time
dynamics, the volumetric flow rate (also known as volume flow rate, or volume velocity) is the volume of fluid which passes per unit time; usually it is
Volumetric_flow_rate
Theorem in calculus
represents a volume in three-dimensional space) which is compact and has a piecewise smooth boundary S (also indicated with ∂ V = S {\displaystyle \partial V=S}
Divergence_theorem
Thermodynamic cycle that includes the basic Stirling engine
isentropic processes featured in the Carnot cycle are replaced by two constant-volume regeneration processes. The cycle is reversible, meaning that if supplied
Stirling_cycle
State function whose change relates to the system's maximal work output
U + pV, where U is the internal energy, p is the pressure, and V is the volume. G is the most useful for processes involving a system at constant pressure
Thermodynamic_free_energy
Concentration of water vapour in the air
widely employed: absolute, relative, and specific. Absolute humidity is the mass of water vapor per volume of air (in grams per cubic meter). Relative
Humidity
Branch of thermodynamics
{\displaystyle \sigma =\sum _{i,j}L_{ij}{\frac {\partial F_{i}}{\partial x_{i}}}{\frac {\partial F_{j}}{\partial x_{j}}}} The second law of thermodynamics requires
Non-equilibrium thermodynamics
Non-equilibrium_thermodynamics
Process whose direction can be reversed
reversibility, since expansion work, which can be visualized on a pressure–volume diagram as the area beneath the equilibrium curve, is different for different
Reversible process (thermodynamics)
Reversible_process_(thermodynamics)
Quantifiable conditions of a thermodynamic system at a specific time
thermodynamics, a thermodynamic state of a system is its condition at a specific time; that is, fully identified by values of a suitable set of parameters
Thermodynamic_state
Diagram showing the thermodynamic states of a material
from the physical P–alpha diagram which combines pressure (P) and specific volume (alpha) as its basic coordinates. The P–alpha diagram shows a strong
Thermodynamic_diagrams
Z ∂ T ) V {\displaystyle U=Nk_{\text{B}}T^{2}\left({\frac {\partial \ln Z}{\partial T}}\right)_{V}} S = U T + N k B ln Z − N k ln N + N k {\displaystyle
Table of thermodynamic equations
Table_of_thermodynamic_equations
Linked cyclic series of thermodynamic processes
Decrease in pressure (P), Increase in volume (v), Decrease in temperature (T) 2→3: Isochoric cooling: Constant volume(v), Decrease in pressure (P), Decrease
Thermodynamic_cycle
Process that cannot be undone or reversed
behaviour of large numbers of entities, whose exact behavior is given by more specific laws. While the fundamental theoretical laws of physics are all time-reversible
Irreversible_process
Integral of drug concentration in blood plasma over time
elimination. The amount eliminated by the body (mass) = clearance (volume/time) * AUC (mass*time/volume).[citation needed] In pharmacokinetics, bioavailability generally
Area under the curve (pharmacokinetics)
Area_under_the_curve_(pharmacokinetics)
Concept in general relativity and quantum field theory
surrounding any volume in spacetime limits the information content of the volume. Thus the number of degrees of freedom in any volume is bounded and not
Black_hole_thermodynamics
Dutch physicist (1837–1923)
critical volume, and critical temperature. This general form is applicable to all substances (see Van der Waals equation.) The compound-specific constants
Johannes Diderik van der Waals
Johannes_Diderik_van_der_Waals
Theoretical drug measure in pharmacology
volume of distribution ( V D {\displaystyle V_{D}} , also known as apparent volume of distribution or volume of dilution) is the theoretical volume that
Volume_of_distribution
Equations definiting head capacities in thermodynamics
_{S}=-{\frac {1}{V}}\left({\frac {\partial V}{\partial P}}\right)_{S}\,} A corresponding expression for the difference in specific heat capacities (intensive
Relations between heat capacities
Relations_between_heat_capacities
Idealized thermodynamic cycle used in engines
cycle and Diesel cycle. In the cycle, an ideal gas undergoes 1–2: Constant volume (isochoric) heat addition; 2–3: Isentropic expansion; 3–1: Constant pressure
Lenoir_cycle
Pair of values which express a thermodynamic system's internal energy
pairs of conjugate variables such as temperature and entropy, pressure and volume, or chemical potential and particle number. In fact, all thermodynamic potentials
Conjugate variables (thermodynamics)
Conjugate_variables_(thermodynamics)
Physical quantity of hot and cold
function of the volume and entropy of a homogeneous system in thermodynamic equilibrium, thermodynamic absolute temperature appears as the partial derivative
Temperature
PARTIAL SPECIFIC-VOLUME
PARTIAL SPECIFIC-VOLUME
Girl/Female
Latin American Shakespearean
An offering. Portia was a heroine in Shakespeare's 'The Merchant of Venice'.
Male
English
English form of Roman Latin Martialis, MARTIAL means "of/like Mars."
Male
German
German form of French Percevel, PARZIFAL means "pierced valley."
Male
German
German form of French Percevel, PARZIVAL means "pierced valley."
Boy/Male
Australian, Christian, French, Latin, Swiss
Warring; Like Mars; Roman God Mars
Boy/Male
Hindu, Indian
Lord of Parti; One of the Name of Shri Satya Saibaba
Female
English
English Shakespeare character name derived from Roman Latin Porcius, PORTIA means "pig." A moon of Uranus was given this name.
Boy/Male
Sikh
One on whom there is gods grace, Gods mercy
Boy/Male
Latin
Warring.
Girl/Female
Hindu, Indian
Queen
Girl/Female
Arabic
Precious; Lord of Specific Wood
Male
Hungarian
Hungarian form of Greek Bartholomaios, BARTAL means "son of Talmai."
Surname or Lastname
English
English : variant of Hartell.
Boy/Male
Teutonic
Martial ruler.
Male
Irish
Irish Gaelic legend name, thought by some to have been derived from Latin Bartholomaeus, PARTHALÃN means "son of Talmai." As the legend goes, this name belonged to an early invader of Ireland who was the first to arrive on those shores after the biblical flood.
Boy/Male
Muslim
Canvas
Male
German
Variant spelling of German Parzifal, PARSIFAL means "pierced valley."
Male
Spanish
Spanish form of Roman Latin Martialis, MARCIAL means "of/like Mars."
Girl/Female
Hindu
Wisdom
Boy/Male
Hindu
Lord of parti one of the name of Shri Satya Sai baba
PARTIAL SPECIFIC-VOLUME
PARTIAL SPECIFIC-VOLUME
Girl/Female
American, Australian, Christian, French, German, Hebrew
Little and Womanly; Free Man; A Man; Place Name; A Plain; Diminutive Form of Charlotte; Feminine Diminutive Form of Charles or Carl
Boy/Male
Arabic, Lebanese, Muslim
Comforter; Consoler
Girl/Female
Indian
Fearless
Boy/Male
Muslim/Islamic
Garden devotion
Girl/Female
Indian, Punjabi, Sikh
A Brave Godly Person
Girl/Female
Gujarati, Hindu, Indian, Kannada
Darkness
Girl/Female
American, Australian, British, Christian, English, Latin
Virginal; Unblemished; Young Girls who Assisted at Pagan Religious Ceremonies; Attendant for a Temple
Girl/Female
Muslim/Islamic
Pure
Boy/Male
Spanish
Manly; brave.Andrew.
Female
Italian
Feminine form of Italian Andrea, ANDREINA means "man; warrior."
PARTIAL SPECIFIC-VOLUME
PARTIAL SPECIFIC-VOLUME
PARTIAL SPECIFIC-VOLUME
PARTIAL SPECIFIC-VOLUME
PARTIAL SPECIFIC-VOLUME
a.
Belonging to war, or to an army and navy; -- opposed to civil; as, martial law; a court-martial.
n.
Of, pertaining to, or affecting, a part only; not general or universal; not total or entire; as, a partial eclipse of the moon.
a.
Pertaining to, or containing, iron; chalybeate; as, martial preparations.
adv.
In part; not totally; as, partially true; the sun partially eclipsed.
a.
Specific.
v.
Admitting of being parted; partible.
a.
Specifying; definite, or making definite; limited; precise; discriminating; as, a specific statement.
a.
Of or pertaining to a species; characterizing or constituting a species; possessing the peculiar property or properties of a thing which constitute its species, and distinguish it from other things; as, the specific form of an animal or a plant; the specific qualities of a drug; the specific distinction between virtue and vice.
imp. & p. p.
of Specify
n.
A native Parthia.
a.
Exerting a peculiar influence over any part of the body; preventing or curing disease by a peculiar adaption, and not on general principles; as, quinine is a specific medicine in cases of malaria.
n.
A patrial noun. Thus Romanus, a Roman, and Troas, a woman of Troy, are patrial nouns, or patrials.
n.
Pertaining to a subordinate portion; as, a compound umbel is made up of a several partial umbels; a leaflet is often supported by a partial petiole.
a.
Impartial.
adv.
In a partial manner; with undue bias of mind; with unjust favor or dislike; as, to judge partially.
a.
Of, pertaining to, or suited for, war; military; as, martial music; a martial appearance.
n.
A specific remedy. See Specific, a., 3.
pl.
of Court-martial
v.
Given when departing; as, a parting shot; a parting salute.
n.
Inclined to favor one party in a cause, or one side of a question, more then the other; baised; not indifferent; as, a judge should not be partial.