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I am an experimental particle physicist, traveler, teacher, researcher, scientist and communicator of ideas.
I am a quarkist and a bit quirky ! Hypothesis non fingo, eppur si muove, dubito cogito ergo sum are things that turn me on !
Researcher in experimental high energy physics (aka elementary particle physics; like “quarks, leptons & mesons and baryons”) … Teacher of Physics (and occasionally chemistry and maths) Blogger (check my website; mdashf.org) !
Love to read read and read but only stuff that interest me. Love to puff away my time in frivolities, just dreaming and may be thinking.
Right now desperately trying to streamline myself.

Fundamental types of crystal lattices and their symmetry operations
Fundamental types of crystal lattices and their symmetry operations.
Topics covered
a. Types and classes of crystals,b. Symmetry operations in crystals
In this lecture we will follow through our basic knowledge gained in the last lecture. — lecture — I, II, and shed light on the most interesting properties of crystal lattices, viz. their symmetry properties. Based on their properties we will classify them into various types and classes.
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ii. Lattices satisfy additional symmetry operations. But due to the constraint of translational symmetry the total number of symmetry operations that the lattices can satisfy is reduced to a minimum.
iii. This means in 2dimensional lattice constructs we have only 5 types of lattices which satisfy additional symmetry operations. In 3dimensional geometry there are a total of 14 classes of lattices.
iv. Thus in 3dimensional lattices the 14 classes of Bravais lattices are categorized into 7 types or systems of fundamental lattices.
v. The extra symmetry operations are
various rotations,
inversion about a space point and
reflection about a plane passing through a lattice point or
their possible combinations. 
Helmholtz theorem in electrodynamics, Gauge transformation.
Electromagnetic theory, lecture — IV
Topics covered in this lecture
a. Helmholtz theorem — in electrodynamics
b. Gauge transformation — of scalar and vector potential in electrodynamics
c. Coulomb and Lorentz gauge
All electromagnetic theory lectures of this series, will be found here (https://mdashf.org/category/electromagnetictheory/)
In our previous lecture — lecture — III, we discussed in quite detail, the problem of electrostatics and magnetostatics.
We understood how deeply the Helmholtz theorems formulate the entire question of these two branches of electromagnetic phenomena.
But static problems are not sufficient for any rigorous treatment of the electromagnetic theory.
We promised in that lecture to study how Helmholtz theorems lend their magical power to understand the most general nature of electromagnetic phenomena.
In this lecture we will study precisely the applicability of Helmholtz theorems to the problem of electrodynamics and we will see how it leads to a great deal of success in advancing the ability to solve electromagnetic problems of a great variety.

Helmholtz theorem. Scalar and vector potentials

Boundary conditions on electric and magnetic fields.
Electromagnetic theory, Lecture — II.
Boundary conditions on Electric and magnetic fields in Maxwell’s equations
Topics covered
A. Summary of Maxwell’s equations — in free space and in material media
B. Integral forms of Maxwell’s equations — by application of vector calculus
C. Derivation of boundary conditions — on electric and magnetic fields
In the last lecture we formulated the Maxwell’s equations, for free space as well as any material medium in their differential form.
Remember that we say free space to mean that the sources of charge densities and sources of current densities that experience our field vectors, viz. $latex vec{E}$ and $latex vec{B}$ — which are produced by other source densities of charges and currents, are nonexistent.
That is there is no hindrance or onlookers our $latex vec{E}$ and $latex vec{B}$ fields meet on their way when they go on a sojourn, in that space. I also hear they call it by the name vacuum. As far as I know I testify, there is no difference between vacuum and free space.
Vacuum simply means for our purpose and many others, there is no glimpse of matter in the space of consideration. It is therefore the simplest of situation to harp on, before we can target our intelligence for achieving more complicated scenario, and yes there certainly are such situations and they take most of our coveted attention in asking us to solve them.
And sooner than later we would be on our toes trying to grasp the burden the more complicated situations would unleash our way. For the time being we focus on free space which means the sources are zero.
Again by sources we mean, not the sources that produce our vector field $latex vec{E}$ and $latex vec{B}$ but the ones that interact with them, in the path of our fields.

Maxwell’s equations
Electromagnetic theory, Lecture — I.
Maxwell’s equations
This lecture, the web version of the first lecture given in the electromagnetic theory paper of the physics honors degree class, was delivered on 21st December 2017. All electromagnetic theory lectures of this series, will be found here.
Also read part2 of the linked lecture. That describes the subject matter of this lecture, in a good deal of depth.
Topics covered
A. Maxwell’s equations — basic form
B. Displacement current — Correction to Ampere’s law
C. Maxwell’s equations — in material media
Maxwell’s equations
Maxwell’s equations the basic forms
The Maxwell’s equations without the corrections to the Ampere’s law can be written as the following;
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Electrostatics is when the electric charge and electric current densities, that produce these field, known therefore also, as the sources of the field, do not explicitly depend on time, that is, are constants. These sources or distributions depict the behavior of the field, and their independence from time means the fields do not vary in time, but vary only under spatial transformation.
Note that we are not talking about sources in the Maxwell’s equations above, but the ones that actually produce the E and B fields of the equations. The sources present in the equations above would alter these static fields though.
Accordingly the Maxwell equations would change their behavior in dynamic — i.e. time varying conditions, than they exhibit in the static conditions.
Equation (ii) has no names, but sometimes given a name, Gauss law — of magnetostatics.
Equation (iii) is known as Faraday’s law — of electromagnetic induction.
Equation (iv) is known as Ampere’s law.
Inconsistency in Maxwell’s equation
The Maxwell’s equations in this form are not the most general form of the eponymous set of equations. Also they are fraught with some degree of inconsistency.Lets gaze deeper.