Propagation constant
propagation constant, propagation constant of a transmission lineThe propagation constant of a sinusoidal electromagnetic wave is a measure of the change undergone by the amplitude and phase of the wave as it propagates in a given direction The quantity being measured can be the voltage, the current in a circuit, or a field vector such as electric field strength or flux density The propagation constant itself measures the change per unit length, but it is otherwise dimensionless In the context of twoport networks and their cascades, propagation constant measures the change undergone by the source quantity as it propagates from one port to the next
The propagation constant's value is expressed logarithmically, almost universally to the base e, rather than the more usual base 10 that is used in telecommunications in other situations The quantity measured, such as voltage, is expressed as a sinusoidal phasor The phase of the sinusoid varies with distance which results in the propagation constant being a complex number, the imaginary part being caused by the phase change
Contents
 1 Alternative names
 2 Definition
 3 Attenuation constant
 31 Copper lines
 32 Optical fibre
 4 Phase constant
 5 Filters and twoport networks
 51 Cascaded networks
 6 See also
 7 Notes
 8 References
 9 External links
Alternative names
The term "propagation constant" is somewhat of a misnomer as it usually varies strongly with ω It is probably the most widely used term but there are a large variety of alternative names used by various authors for this quantity These include transmission parameter, transmission function, propagation parameter, propagation coefficient and transmission constant If the plural is used, it suggests that α and β are being referenced separately but collectively as in transmission parameters, propagation parameters, etc In transmission line theory, α and β are counted among the "secondary coefficients", the term secondary being used to contrast to the primary line coefficients The primary coefficients are the physical properties of the line, namely R,C,L and G, from which the secondary coefficients may be derived using the telegrapher's equation Note that in the field of transmission lines, the term transmission coefficient has a different meaning despite the similarity of name: it is the companion of the reflection coefficient
Definition
The propagation constant, symbol γ } , for a given system is defined by the ratio of the complex amplitude at the source of the wave to the complex amplitude at some distance x, such that,
A 0 A x = e γ x }}}=e^}Since the propagation constant is a complex quantity we can write:
γ = α + i βwhere
 α, the real part, is called the attenuation constant
 β, the imaginary part, is called the phase constant
That β does indeed represent phase can be seen from Euler's formula:
e i θ = cos θ + i sin θ =\cos +i\sin \,\!}which is a sinusoid which varies in phase as θ varies but does not vary in amplitude because
 e i θ  = cos 2 θ + sin 2 θ = 1 \right=+\sin ^}}=1}The reason for the use of base e is also now made clear The imaginary phase constant, iβ, can be added directly to the attenuation constant, α, to form a single complex number that can be handled in one mathematical operation provided they are to the same base Angles measured in radians require base e, so the attenuation is likewise in base e
The propagation constant for copper or any other conductor lines can be calculated from the primary line coefficients by means of the relationship
γ = Z Y }}where
Z = R + i ω L , the series impedance of the line per unit length and, Y = G + i ω C , the shunt admittance of the line per unit lengthAttenuation constant
In telecommunications, the term attenuation constant, also called attenuation parameter or attenuation coefficient, is the attenuation of an electromagnetic wave propagating through a medium per unit distance from the source It is the real part of the propagation constant and is measured in nepers per metre A neper is approximately 87 dB Attenuation constant can be defined by the amplitude ratio
 A 0 A x  = e α x }}}\right=e^}The propagation constant per unit length is defined as the natural logarithmic of ratio of the sending end current or voltage to the receiving end current or voltage
Copper lines
The attenuation constant for copper lines or ones made of any other conductor can be calculated from the primary line coefficients as shown above For a line meeting the distortionless condition, with a conductance G in the insulator, the attenuation constant is given by
α = R G }\,\!}however, a real line is unlikely to meet this condition without the addition of loading coils and, furthermore, there are some frequency dependent effects operating on the primary "constants" which cause a frequency dependence of the loss There are two main components to these losses, the metal loss and the dielectric loss
The loss of most transmission lines are dominated by the metal loss, which causes a frequency dependency due to finite conductivity of metals, and the skin effect inside a conductor The skin effect causes R along the conductor to be approximately dependent on frequency according to
R ∝ ω }}Losses in the dielectric depend on the loss tangent tan δ of the material divided by the wavelength of the signal Thus they are directly proportional to the frequency
α d = π ε r λ tan δ =}} \over }}Optical fibre
The attenuation constant for a particular propagation mode in an optical fiber is the real part of the axial propagation constant
Phase constant
In electromagnetic theory, the phase constant, also called phase change constant, parameter or coefficient is the imaginary component of the propagation constant for a plane wave It represents the change in phase per unit length along the path travelled by the wave at any instant and is equal to real part of the angular wavenumber of the wave It is represented by the symbol β and is measured in units of radians per unit length
From the definition of angular wavenumber for TEM waves:
k = 2 π λ = β }=\beta }For a transmission line, the Heaviside condition of the telegrapher's equation tells us that the wavenumber must be proportional to frequency for the transmission of the wave to be undistorted in the time domain This includes, but is not limited to, the ideal case of a lossless line The reason for this condition can be seen by considering that a useful signal is composed of many different wavelengths in the frequency domain For there to be no distortion of the waveform, all these waves must travel at the same velocity so that they arrive at the far end of the line at the same time as a group Since wave phase velocity is given by
v p = λ T = f ν ~ = ω β =}=}}=}}it is proved that β is required to be proportional to ω In terms of primary coefficients of the line, this yields from the telegrapher's equation for a distortionless line the condition
β = ω L C }}However, practical lines can only be expected to approximately meet this condition over a limited frequency band
In particular, the phase constant β is not always equivalent to the wavenumber k Generally speaking, the following relation
β = kis tenable to the TEM wave transverse electromagnetic wave which travels in free space or TEMdevices such as the coaxial cable and two parallel wires transmission lines Nevertheless, it is invalid to the TE wave transverse electric wave and TM wave transverse magnetic wave For example, in a hollow waveguide where the TEM wave cannot exist but TE and TM waves can propagate,
k = ω c }} β = k 1 − ω c 2 ω 2 ^}}}}}}Here ω c } is the cutoff frequencyIn a rectangular waveguide, the cutoff frequency is
ω c = c n π a 2 + m π b 2 , =c}\right^+\left}\right^}},}where the integers n , m ≥ 0 are the mode numbers, and a and b the lengths of the sides of the rectangle For TE modes, n , m ≥ 0 but n = m = 0 is not allowed, while for TM modes n , m ≥ 1 The phase velocity equals
v p = ω β = c 1 − ω c 2 ω 2 > c =}= }^}}}}}}>c}The phase constant is also an important concept in quantum mechanics because the momentum p of a quantum is directly proportional to it, ie
p = ℏ βwhere ħ is called the reduced Planck constant pronounced "hbar" It is equal to the Planck constant divided by 2π
Filters and twoport networks
The term propagation constant or propagation function is applied to filters and other twoport networks used for signal processing In these cases, however, the attenuation and phase coefficients are expressed in terms of nepers and radians per network section rather than per unit length Some authors make a distinction between per unit length measures for which "constant" is used and per section measures for which "function" is used
The propagation constant is a useful concept in filter design which invariably uses a cascaded section topology In a cascaded topology, the propagation constant, attenuation constant and phase constant of individual sections may be simply added to find the total propagation constant etc
Cascaded networks
Three networks with arbitrary propagation constants and impedances connected in cascade The Zi terms represent image impedance and it is assumed that connections are between matching image impedancesThe ratio of output to input voltage for each network is given by
V 1 V 2 = Z I 1 Z I 2 e γ 1 }}}=}}}}e^}} V 2 V 3 = Z I 2 Z I 3 e γ 2 }}}=}}}}e^}} V 3 V 4 = Z I 3 Z I 4 e γ 3 }}}=}}}}e^}}The terms Z I n Z I m }}}}} are impedance scaling terms and their use is explained in the image impedance article
The overall voltage ratio is given by
V 1 V 4 = V 1 V 2 ⋅ V 2 V 3 ⋅ V 3 V 4 = Z I 1 Z I 4 e γ 1 + γ 2 + γ 3 }}}=}}}\cdot }}}\cdot }}}=}}}}e^+\gamma _+\gamma _}}Thus for n cascaded sections all having matching impedances facing each other, the overall propagation constant is given by
γ t o t a l = γ 1 + γ 2 + γ 3 + ⋯ + γ n }=\gamma _+\gamma _+\gamma _+\cdots +\gamma _}See also
The concept of penetration depth is one of many ways to describe the absorption of electromagnetic waves For the others, and their interrelationships, see the article: Mathematical descriptions of opacity
Notes
 ^ Pozar, David 2012 Microwave Engineering 4th ed John Wiley &Sons pp 62–164 ISBN 9780470631553
 ^ Wang,ZY 2016 "Generalized momentum equation of quantum mechanics" Optical and Quantum Electronics 48 2: 1–9 doi:101007/s1108201502618
 ^ Tremblay,R, Doyon,N, BeaudoinBertrand,J "TETM Electromagnetic modes and states in quantum physics" arXiv:161101472 Bibcode:2016arXiv161101472T CS1 maint: Multiple names: authors list link
 ^ Matthaei et al, p49
 ^ Matthaei et al pp5152
 ^ Matthaei et al pp3738
References
 This article incorporates public domain material from the General Services Administration document "Federal Standard 1037C"
 Matthaei, Young, Jones Microwave Filters, ImpedanceMatching Networks, and Coupling Structures McGrawHill 1964
External links
 "Propagation constant" Online Microwave Encyclopedia 2011 Retrieved February 2, 2011
 Paschotta, Dr Rüdiger 2011 "Propagation Constant" Online Encyclopedia of Laser Physics and Technology Retrieved February 2011 Check date values in: accessdate= help
 Janezic, Michael D; Jeffrey A Jargon February 1999 "Complex Permittivity determination from Propagation Constant measurements" PDF Microwave and Guided Wave Letters, IEEE 9: 76–78 doi:101109/75755052 Retrieved February 2011 Check date values in: accessdate= help Free PDF download is available There is an updated version dated August 6, 2002
propagation constant, propagation constant attenuation, propagation constant beta, propagation constant calculation, propagation constant formula, propagation constant gamma, propagation constant in lossy medium, propagation constant k, propagation constant of a transmission line, propagation constant units
Propagation constant Information about

Propagation constant beatiful post thanks!
29.10.2014
Propagation constant
Propagation constant
Propagation constant viewing the topic.
There are excerpts from wikipedia on this article and video
Random Posts
Body politic
The body politic is a metaphor that regards a nation as a corporate entity,2 likened to a human body...Kakamega
Kakamega is a town in western Kenya lying about 30 km north of the Equator It is the headquarte...Academic year
An academic year is a period of time which schools, colleges and universities use to measure a quant...Lucrezia Borgia
Lucrezia Borgia Italian pronunciation: luˈkrɛttsja ˈbɔrdʒa; Valencian: Lucrècia Borja luˈkrɛsia...Search Engine
Our site has a system which serves search engine function.
You can search all data in our system with above button which written "What did you look for? "
Welcome to our simple, stylish and fast search engine system.
We have prepared this method why you can reach most accurate and most up to date knowladge.
The search engine that developed for you transmits you to the latest and exact information with its basic and quick system.
You can find nearly everything data which found from internet with this system.
Random Posts
IP address blocking
IP address blocking prevents connection between a server or website and certain IP addresses or rang...Gisele Bündchen
Gisele Caroline Bündchen1 Portuguese pronunciation: ʒiˈzɛli kaɾoˈlini ˈbĩtʃẽj, German pronuncia...Sheldon, West Midlands
Sheldon is an area of east Birmingham, England Historically part of Warwickshire, it is close to the...Beverly, Chicago
Beverly is one of the 77 community areas of Chicago, Illinois It is located on the South Side on the...© Copyright © 2014. Search Engine