Home

Archive

English

Persian

contact us

 

 

 

 

Links 

Articles

Cern Experiment and Violatin of Newton's Second Law

 

LEIBNIZ'S MONADS AND JAVADI'S CPH

World Science Database

General Science Journal

Hadronic Journal

National Research Council Canada

 

 

November 2, 2011: CERN Experiment and Violation of Newton’s Second Law Englishview
 

October 13, 2011: CERN Experiment and Violation of the Newton’s Second Law Persianview
 

November 24, 2008: A New Definition of Gravitonview
 

July 10, 2007: Zero Point Energy and the Dirac Equationview
 

July 10, 2007: Zero Point Energy and the Dirac Equationview
 

June 28, 2007: Unification and CPH Theoryview
 

June 14, 2007: Summary of Physics Conceptsview
 

June 14, 2007: Strong Interaction and CPH Theory Rview
 

June 4, 2007: Quantum Electrodynamics and CPH Theoryview
 

November 30, 2006: Vocabulary of CPH Theoryview
 

November 17, 2006: Thermodynamic Laws Entropy and CPH Theoryview
 

November 17, 2006: Time Function and Absolute Black Holeview
 

October 14, 2006: CPH and Timeview
 

October 13, 2006: CPH Theory and Newton's Second Lawview
 

October 13, 2006: Time Function and Work Energy Theoremview
 

October 13, 2006: CPH Theory and Special Relativityview
 

October 13, 2006: Properties of CPHview
 

July 31, 2006: A New Mechanism of Higgs Bosons in Producing Charge Particlesview
 

July 31, 2006: A New Mechanism of Higgs Bosons in Producing Charge Particlesview
 

May 14, 2006: Speed of Light and CPH Theoryview
 

May 14, 2006: Speed of Light and CPH Theoryview
 

April 28, 2006: Color Charges Curve Spaceview
 

April 28, 2006: Color Charges Curve Spaceview
 

April 17, 2006: Effective Nuclear Chargeview
 

April 17, 2006: Effective Nuclear Chargeview
 

April 12, 2006: Maxwell's Equations in a Gravitational Fieldview
 

April 12, 2006: Maxwell's Equations in a Gravitational Fieldview
 

April 11, 2006: Realization Hawking - End of Physics by CPHview
 

April 7, 2006: Questions and Answers on CPH Theoryview
 

April 7, 2006: Opinions on CPH Theoryview
 

April 7, 2006: Opinions on CPH Theoryview
 

April 7, 2006: Questions and Answers on CPH Theoryview
 

March 23, 2006: Analysis of CPH Theoryview
 

March 23, 2006: Analysis of CPH Theoryview
 

March 21, 2006: Logical Foundation of CPH Theoryview
 

March 21, 2006: Definition Principle and Explanation of CPH Theoryview
 

March 21, 2006: Logical Foundation of CPH Theoryview
 

March 21, 2006: Definition Principle and Explanation of CPH Theoryview
 

March 21, 2006: Experimental Foundation of CPH Theoryview
 

March 21, 2006: Experimental Foundation of CPH Theoryview
 

March 19, 2006: Color Charge/Color Magnet and CPHview
 

March 19, 2006: Sub-Quantum Chromodynamicsview
 

 

 

 

 

A Mathematical Mode for Effective Nuclear Charge

 

 

 
 



 


 

Introduction;

 

The effective nuclear charge (Z*) is the "pull" that the specific electron "feels" from the nucleus. Of the first time Slater did give a simple rule for calculate the effective nuclear charge on any electron in any atoms in 1930. Clementi and Raimondi did their work on effective nuclear charges in the early 1960s. The results of Clementis method are difference of Staler's rule. For example Clementi calculated as Sc from a 4s perspective Z*=4.632, but Staler's Z* are equal 3...

Staler's rule and Clementi's method based on experiments. There is no any analytic method for why and how the strongly of nuclear charge does lose? By according CPH theory force and energy are equivalence. Force converts to energy and energy changes to force. I will give a Mathematical Mode for Effective Nuclear Charge by CPH Theory.

 

Mathematical Mode;

By according Theory of CPH, when a force works on an object/particle, when W (work) is positive, force converts to energy and when W<o, energy changes to force.

Suppose an atom with Z proton is at stationary state, its Nuclear Charge Fz and Effective Nuclear Charge on an electron is Fz*. In during Fz reaches to electron, its works on other electrons is W, so Fw converts to energy E=W and electron feels the effective nuclear charge equal Fz* that given by;

 

Fz*=Fz - Fw

 

Group each electron like this:

(1s)(2s,2p)(3s,3p)(3d)(4s,4p)(4d)(4f)(5s,5p)(5d)(5f)...

Electrons to the right of the electron you have chosen do not contribute.

 

Examples;

Suppose two objects A and B absorb each other. By according CPH Theory a force particle leaves A and pulls it toward B, when force particle reaches to B, another leaves B and pulls it toward A and so on. In the following examples please attend that electrons are moving in their orbits, but Fz (nuclear charge) moves faster than electrons.

 

Hydrogen;

Hydrogen atom contains one proton and one electron in 1s, so Fw=o and Fz=Fz*. Because there is no any other electron in hydrogen atom and Fw=0. Clementi supposed Fz*=1

 

Helium;

Helium contains two protons and two electrons in 1s. Fz=2 from two protons moves toward electron1. Electron2 has electric charge and magnetic field. So, Fz acts on electron2. But direction of Fz is toward the electron1. So, electron2 does change direction of Fz. It depends to distance between electrons in this orbit. Suppose this effect is nothing.

But, Fz  works on electron2, energy of electron2 increases and Fz  loses a part of its strong. So, the effective nuclear charge Fz* on electron1 given by;

Fz*=Fz - Fw

Energy of electron2 increases equal E=W. It leaves its orbit. But electric force leaves it toward nuclear and pulls electron2 toward nuclear. Also, electric force of electron1 acts on it. Then electron2 comes back to its orbit and loses energy E, and E converts to electric force equal Fw. Then Fw does add to Fz* that is coming back of electron1 and Fz=Fz*+Fw reaches to nuclear. So, nuclear feels that effective force of electron1 is equal Fz.      

The effective nuclear charge Fz* on electron2 is same as electron1. By according Clementi calculate Fz*=1.688

 

Lithium;

Lithium has 3 protons and 3 electrons, two electrons are in 1s and one electron is in 2s.

 

For 1s;

Fz=3 from 3 protons moves toward electron1 in 1s orbit . This case is same as Helium, but radius of 1s orbits is smaller than in Helium and distance between electrons is less than Heliums orbit. So deviation direction of Fz is less than in Helium. It shows the effect of deviation direction for Fz is less than Helium. By according Clementi's calculate Fz*=2.691. Do compare with Helium that Fz*=1.688. 

 

For 2s;

There is one electron in orbit 2s in Lithium. So, this electron feels Fz* that is coming of over the orbit 1s. Fz=3 leaves nuclear toward it. Fz works on two electrons in orbit 1s.

Fz loses Fw1 for act on electron1, and Fw2 for act on electron2. So, when Fz reaches to orbit 1s, It comes up to F'z=Fz - (Fw1+Fw2).

In during F'z is passing of orbit 1s, it works on the sum of electron1 and electron2. Suppose this work is equal Fw3.

So, Fw=Fw1+Fw2+Fw3 and Fz*=Fz-Fw reaches to electron in orbit 2s. By according Clementi's calculation Fz*=1.279.

When Fz* reaches to electron, then an other electric force particle equal Fz* leaves it toward nuclear. When it reaches to orbit 1s works on it. In during Fz* is passing of orbit 1s, energy E=W converts to force Fw and Fz=Fz*+Fw reaches to nuclear.

 

Summary;

For calculation the effective nuclear charge Fz* on any electron in any atoms, we must calculate Fw. W is the sum of works that Fz acts on electrons and orbits (or sub orbits) before Fz reaches to it.

For example; For Na from a 3s,

Na has 11 protons and 11 electrons, so;

A. 2 electrons in 1s, Fw1

B. an orbit n1, Fw2

C. 6 electrons in 2p, Fw3

D. a sub orbit 2p, Fw4

E. 2 electrons in 2s, Fw5

F. an orbit n2, Fw6

So, Fw=Fw1+Fw2+Fw3+Fw4+Fw5+Fw6,

And Fz*=Fz-Fw

 

Sincerely

Hossein Javadi

 

 

 

 

 

 
 

 
 

 
 


 

 

 

 
1 2 3 4 5 6 7 8 9 10  Newest articles

 


 

Interesting articles

Faster Than Light 

Light that travels… faster than light!

Before the Big Bang

Structure of Charge Particles

Move Structure of Photon

Structure of Charge Particles

Faster Than Light 

Light that travels… faster than light!

Before the Big Bang

Structure of Charge Particles

Move Structure of Photon

Structure of Charge Particles

Zero Point Energy and the Dirac Equation [PDF] Persian Text


 
Unification and CPH Theory [PDF] 


Strong Interaction and CPH Theory [PDF]


Summary of Physics Concepts [PDF]


Quantum Electrodynamics and CPH Theory [PDF] 


Vocabulary of CPH Theory [PDF] 


Thermodynamic Laws, Entropy and CPH Theory [PDF]


Time Function and Absolute Black Hole [PDF] 


CPH and Time [PDF]Persian Text Only


Time Function and Work Energy Theorem [PDF] Persian Text Only 


Properties of CPH [PDF]Persian Text Only 


CPH Theory and Special Relativity [PDF] Persian Text Only


CPH Theory and Newton's Second Law [PDF] Persian Text Only 

 

A New Mechanism of Higgs Bosons in Producing Charge Particles [PDF] Persian Text 


Logical Foundation of CPH Theory [PDF] Persian Text 


Experimental Foundation of CPH Theory [PDF] Persian Text 


Definition, Principle and Explanation of CPH Theory [PDF] Persian Text


 
Analysis of CPH Theory Persian Text


Opinions on CPH Theory [PDF] Persian Text


 
Questions and Answers on CPH Theory [PDF] Persian Text


 
Realization Hawking - End of Physics by CPH [PDF]Persian Text Only


 
Maxwell's Equations in a Gravitational Field [PDF] Persian Text


 
Effective Nuclear Charge [PDF] Persian Text


 
Color Charges Curve Space [PDF] Persian Text 


Sub-Quantum Chromodynamics [PDF]


 
Color Charge/Color Magnet and CPH [PDF]


 
Speed of Light and CPH Theory [PDF] Persian Text

 

 

 
 
 
 

 

 

free hit counters

 


 

@2003-2012 The CPH theory, All right reserved