1. The document describes Love's equivalence principle for modeling aperture antennas, where an imaginary surface enclosing sources is selected and equivalent electric and magnetic current densities are formed over this surface.
2. It provides steps for using this principle to solve aperture problems, including forming equivalent current densities over the surface and solving for radiated fields using auxiliary potential functions.
3. Equations are presented for calculating far-field radiation patterns from equivalent current densities using spherical harmonic functions.
Optical fiber communication Part 2 Sources and DetectorsMadhumita Tamhane
For optical fiber communication, major light sources are hetero-junction-structured semiconductor laser diode and light emitting diodes. Heterojunction consists of two adjoining semiconductor materials with different bandgap energies. They have adequate power for wide range of applications. Detectors used are PiN diode and Avalanche Photodiode. Being very small in size and feeding to small core optical fiber, it is very important to study emission characteristics of sources and their coupling to fiber. As it can operate for low power over a long distance, received power is very small, hence study of noise characteristics of detectors is very essential...
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Intuitive explanation of maxwell electromagnetic equationsAbdiasis Jama
user friendly explanation of maxwell equations
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1 ECE 6340 Fall 2013 Homework 8 Assignment.docxjoyjonna282
1
ECE 6340
Fall 2013
Homework 8
Assignment: Please do Probs. 1-9 and 13 from the set below.
1) In dynamics, we have the equation
E j Aω= − −∇Φ .
(a) Show that in statics, the scalar potential function Φ can be interpreted as a voltage
function. That is, show that in statics
( ) ( )
B
AB
A
V E dr A B≡ ⋅ = Φ −Φ∫ .
(b) Next, explain why this equation is not true (in general) in dynamics.
(c) Explain why the voltage drop (defined as the line integral of the electric field, as
defined above) depends on the path from A to B in dynamics, using Faraday’s law.
(d) Does the right-hand side of the above equation (the difference in the potential
function) depend on the path, in dynamics?
Hint: Note that, according to calculus, for any function ψ we have
dr dx dy dz d
x y z
ψ ψ ψ
ψ ψ
∂ ∂ ∂
∇ ⋅ = + + =
∂ ∂ ∂
.
2) Starting with Maxwell’s equations, show that the electric field radiated by an impressed
current density source J i in an infinite homogeneous region satisfies the equation
( )2 2 iE k E E j Jωµ∇ + = ∇ ∇⋅ + .
Then use Ampere’s law (or, if you prefer, the continuity equation and the electric Gauss
law) to show that this equation may be written as
( )2 2 1 i iE k E J j J
j
ωµ
σ ωε
∇ + = − ∇ ∇⋅ +
+
.
2
Note that the total current density is the sum of the impressed current density and the
conduction current density, the latter obeying Ohm’s law (J c = σE).
Explain why this equation for the electric field would be harder to solve than the equation
that was derived in class for the magnetic vector potential.
3) Show that magnetic field radiated by an impressed current density source satisfies the
equation
2 2 iH k H J∇ + = −∇× .
Explain why this equation for the magnetic field would be harder to solve than the
equation that was derived in class for the magnetic vector potential.
4) Show that in a homogenous region of space the scalar electric potential satisfies the
equation
2 2
i
v
c
k
ρ
ε
∇ Φ + Φ = − ,
where ivρ is the impressed (source) charge density, which is the charge density that goes
along with the impressed current density, being related by
i ivJ jωρ∇⋅ = −
Hint: Start with E j Aω= − −∇Φ and take the divergence of both sides. Also, take the
divergence of both sides of Ampere’s law and use the continuity equation for the
impressed current (given above) to show that
1 ii v
c c
E J
j
ρ
ωε ε
∇⋅ = − ∇⋅ = .
Note: It is also true from the electric Gauss law that
vE
ρ
ε
∇⋅ = ,
but we prefer to have only an impressed (source) charge density on the right-hand side of
the equation for the potential Φ. In the time-harmonic steady state, assuming a
homogeneous and isotropic region, it follows that ρv = ρvi. That is, there is no charge
3
density arising from the conduction current. (If there were no impressed current sources,
the total charge density would therefore be ze ...
Optimization of Surface Impedance for Reducing Surface Waves between AntennasIJMER
International Journal of Modern Engineering Research (IJMER) is Peer reviewed, online Journal. It serves as an international archival forum of scholarly research related to engineering and science education.
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Method of Moment analysis of a printed Archimedian Spiral antenna Piyush Kashyap
A single arm Archimedean spiral printed on a grounded dielectric substrate is analyzed using the method of moments. Piecewise sinusoidal subdomain basis and test functions are used over curved segments that exactly follow the spiral curvature. Results for the input impedance obtained using the curved segmentation approach on MATLAB are compared with those obtained after simulating the model on FEKO. A comparison with published results shows that the curved segment model requires fewer segments and is therefore significantly more computationally efficient than the linear segmentation model.
Numerical Simulations on Flux Tube Tectonic Model for Solar Coronal HeatingRSIS International
The sun is a G-type main sequence star. Corona is an
aura of Plasma that Surrounds the Sun and other Stars. The
heating of solar Corona is one of most important problem in
Astrophysics. There are several mechanism of Coronal heating.
In this paper we discuss Numerical Simulation on Flux tube
Tectonic Model For Solar Coronal Heating .
The metal-insulator-semiconductor (MIS) capacitor is the most useful device in the study of semiconductor surfaces. Since most practical problems in the reliability and stability of all semiconductor devices are intimately related to their surface conditions, an understanding of the surface physics with the help of MIS capacitors is of great importance to device operations.
Determination of Surface Currents on Circular Microstrip AntennaswailGodaymi1
This work aims to present a theoretical analysis of the electric and magnetic surface current densities of a circular
microstrip antenna (CMSA) as a body of revolution.
The rigorous analysis of these problems begins with the application of the equivalence principle, which introduces
an unknown electric current density on the conducting surface and both unknown equivalent electric and magnetic
surface current densities on the dielectric surface. These current densities satisfy the integral equations (IEs) obtained
by canceling the tangential components of the electric field on the conducting surface and enforcing the continuity
of the tangential components of the fields across the dielectric surface. The formulation of the radiation problems is
based on the combined field integral equation. This formulation is coupled with the method of moments (MoMs) as
a numerical solution for this equation.
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CFD Simulation of By-pass Flow in a HRSG module by R&R Consult.pptxR&R Consult
CFD analysis is incredibly effective at solving mysteries and improving the performance of complex systems!
Here's a great example: At a large natural gas-fired power plant, where they use waste heat to generate steam and energy, they were puzzled that their boiler wasn't producing as much steam as expected.
R&R and Tetra Engineering Group Inc. were asked to solve the issue with reduced steam production.
An inspection had shown that a significant amount of hot flue gas was bypassing the boiler tubes, where the heat was supposed to be transferred.
R&R Consult conducted a CFD analysis, which revealed that 6.3% of the flue gas was bypassing the boiler tubes without transferring heat. The analysis also showed that the flue gas was instead being directed along the sides of the boiler and between the modules that were supposed to capture the heat. This was the cause of the reduced performance.
Based on our results, Tetra Engineering installed covering plates to reduce the bypass flow. This improved the boiler's performance and increased electricity production.
It is always satisfying when we can help solve complex challenges like this. Do your systems also need a check-up or optimization? Give us a call!
Work done in cooperation with James Malloy and David Moelling from Tetra Engineering.
More examples of our work https://www.r-r-consult.dk/en/cases-en/
Overview of the fundamental roles in Hydropower generation and the components involved in wider Electrical Engineering.
This paper presents the design and construction of hydroelectric dams from the hydrologist’s survey of the valley before construction, all aspects and involved disciplines, fluid dynamics, structural engineering, generation and mains frequency regulation to the very transmission of power through the network in the United Kingdom.
Author: Robbie Edward Sayers
Collaborators and co editors: Charlie Sims and Connor Healey.
(C) 2024 Robbie E. Sayers
Explore the innovative world of trenchless pipe repair with our comprehensive guide, "The Benefits and Techniques of Trenchless Pipe Repair." This document delves into the modern methods of repairing underground pipes without the need for extensive excavation, highlighting the numerous advantages and the latest techniques used in the industry.
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Cosmetic shop management system project report.pdfKamal Acharya
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Data file handling has been effectively used in the program.
The automated cosmetic shop management system should deal with the automation of general workflow and administration process of the shop. The main processes of the system focus on customer's request where the system is able to search the most appropriate products and deliver it to the customers. It should help the employees to quickly identify the list of cosmetic product that have reached the minimum quantity and also keep a track of expired date for each cosmetic product. It should help the employees to find the rack number in which the product is placed.It is also Faster and more efficient way.
2. Love’s Equivalence Principle of Figure 3(a) produces a null
field within the imaginary surface S.
Since the value of the E = H = 0 within S cannot be disturbed if
the properties of the medium with in it are changed, let us assume
that it is replaced by a perfect electric conductor (σ =∞).
As the electric conductor takes its place, as shown in Fig 3(b),
the electric current density Js , which is tangent to the surface S, is
short-circuited by the electric conductor.
Thus the equivalent problem of Fig3(a) reduces to that of Figure
3(b).
There exists only a magnetic current density Ms over S, and it
radiates in the presence of the electric conductor producing
outside S the original fields E1, H1.
4. The steps that must be used to form an equivalent and solve an
aperture problem are as follows:
1. Select an imaginary surface that encloses the actual sources
(the aperture). The surface must be judiciously chosen so that
the tangential components of the electric and/or the magnetic
field are known, exactly or approximately, over its entire span. In
many cases this surface is a flat plane extending to infinity.
2. Over the imaginary surface form equivalent current densities
Js ,Ms which take one of the following forms:
a. Js and Ms over S assuming that the E- and H-fields within S are
not zero.
b. or Js and Ms over S assuming that the E- and H-fields within S
are zero (Love’s theorem)
c. or Ms over S (Js = 0) assuming that within S the medium is a
perfect electric conductor
6. EA can be
found using
Maxwell’s
equation of
with J = 0.
HF can be
found using
Maxwell’s
equation with
M = 0.
a3
a4
a5
a6
7. d. or Js over S (Ms = 0) assuming that within S the medium is
a perfect magnetic
conductor.
3. Solve the equivalent problem. For forms (a) and (b), above
equations can be used. For form (c), the problem of a
magnetic current source next to a perfect electric conductor
must be solved above equations cannot be used directly,
because the current density does not radiate into an unbounded
medium]. If the electric conductor is an infinite flat plane the
problem can be solved exactly by image theory.
For form (d), the problem of an electric current source next to
a perfect magnetic conductor must be solved.
8. RADIATION EQUATIONS
it was stated that the fields radiated by sources
Js and Ms in an unbounded medium can be computed by
using (a1)–(a6) where the integration must be performed
over the entire surface occupied by Js and Ms.
for far-field observations R can most commonly be
approximated by
5a
5b
14. The Nθ, Nφ, Lθ, and Lφ can be obtained from (6a)
and (7a).
11a
11b
Using the rectangular-to-spherical component
transformation (11a) and (11b) reduce for the
16. Figures 2(a) and 2(b) are used to indicate the geometry.
1.Select a closed surface over which the total electric and
magnetic fields Ea and Ha are known.
2. Form the equivalent current densities Js and Ms over S
using (3) and (4) with H1 = Ha and E1 = Ea.
3. Determine the A and F potentials using (6)–(7a) where
the integration is over the closed surface S.
4. Determine the radiated E- and H-fields using
17. 3’. Determine Nθ, Nφ, Lθ and Lφ using (12a)–(12d).
4’. Determine the radiated E- and H-fields using
(10a)–(10f).