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Maxwellโ€™s Core Equations
Exact, Universal,
and
Scary
April 11, 2021
1
Robert S. Eisenberg
Bard Endowed Professor and Chair, emeritus
Department of Physiology and Biophysics
Rush University
Adjunct Professor
Department of Applied Mathematics
Illinois Institute of Technology
Chicago IL
USA
Tufts Math Department
April 11, 2021
2
Presented March 29, 2021
April 11, 2021 3
Abstract
When the Maxwell equations are written without a dielectric constant, they are universal and exact, for biological and
technological applications, from inside atoms to between stars. Dielectric and polarization phenomena need then to be
described by stress strain relations for charge, that show how charge redistributes when the electric field is changed,
in each system of interest.
Conservation of total current (including the ethereal displacement current ๐œบ๐ŸŽ ๐๐„ ๐๐’•) is then as exact as the Maxwell
equations themselves and independent of any property of matter. It is a consequence of the Lorentz invariance of the
elementary charge, a property of all locally inertial systems, described by the theory of relativity.
Exact Conservation of Total Current allows a redefinition of Kirchhoffโ€™s current law that is itself exact. In unbranched
systems like circuit components or ion channels, conservation of total current becomes equality. Spatial dependence
of total current disappears in that case. Hopping phenomena disappear. Spatial Brownian motion disappears. The
infinite variation of a Brownian model of thermal noise becomes the zero spatial variation of total current.
Maxwellโ€™s Core Equations become a perfect (spatial) low pass filter.
An Exact and Universal theory of Electrodynamics is a scary challenge to scientists like me,
trained to be skeptical of all sweeping claims to perfection.
4
Mathematics
describes only a tiny part of life,
๏ƒฒ
๏ƒฅ
u
๏‚ถ
๏‚ถ
April 11, 2021
5
But
Mathematics* Creates
our
Standard of Living
Electronics, Electricity, Computers, Mobile Phones, TV, Games
and Fluid Dynamics, Optics, Structural Mechanics, โ€ฆ.
๏ƒฒ
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u
๏‚ถ
๏‚ถ
April 11, 2021
Essence of Electrodynamics
is
Maxwellโ€™s Core Equations
for the
Flows and Forces of Charge and Current
in matter and space
April 11, 2021
6
Nearly Exact and Universal from Stars
to inside atoms
Eisenberg, Oriols, and Ferry (2017) Dynamics of Current, Charge, and Mass.
Molecular Based Mathematical Biology 5:78-115 and arXiv preprint https://arxiv.org/abs/1708.07400.
is electric field, is magnetic field
is the current of all mass, including brief dielectric transients of the and fields
is charge density (of all types, including dielectric charge of the
๏ฒ
E B
J P D
P
๏€จ ๏€ฉ
0
0
0 0
and fields)
is the permittivity of a vacuum
is the permeability of a vacuum
velocity of light (!)
๏ฅ
๏ญ
๏ญ ๏ฅ ๏€ฝ
D
-0.5
Maxwellโ€™s Core Equations
Describe Electricity with errors <10-6
in biological and technological applications
April 11, 2021
7
๐๐ข๐ฏ ๐„ = ๐†
๐œบ๐ŸŽ
๐œ๐ฎ๐ซ๐ฅ ๐„ = โˆ’
๐œ•๐
๐œ•๐‘ก
๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0 ๐‰ + ๐œ€0
๐œ•๐„
๐œ•๐‘ก
๐๐ข๐ฏ ๐ = ๐ŸŽ
8
Advanced Photon Source Argonne National Laboratory
Beam ~๐Ÿ๐ŸŽ๐Ÿ๐ŸŽ
eV
Beam length ๐Ÿ๐ŸŽ๐Ÿ‘
m
Tolerance < ๐Ÿ๐ŸŽโˆ’๐Ÿ•
m
Beam Current ๐Ÿ๐ŸŽ๐ŸŽ mA
Beam Power ๐Ÿ๐ŸŽ๐Ÿ—
๐ฐ๐š๐ญ๐ญ๐ฌ
Error in Theory
< ๐Ÿ๐ŸŽโˆ’๐Ÿ๐ŸŽ
Source Internet
April 11, 2021
9
April 11, 2021
Richard Feynman
โ€œWhenever you see a sweeping statement that a
tremendous amount can come from a very small number of assumptions,
You always find that it is False
There are usually a large number of
Implied Assumptions
that are far from obvious if you think about them sufficiently carefully.โ€
Section 26-1.
The Feynman Lectures on Physics, Mainly Electromagnetism and Matter 1963 also at http://www.feynmanlectures.caltech.edu/II_toc.html
CHALLENGE TO THE AUDIENCE
Find and Discuss the Implied Assumptions in this Talk
Contact me at Bob.Eisenberg@gmail.com
Maxwellโ€™s Core Equations are Universal and Exact
But they are Complicated Differential Equations
need very complicated mathematics to describe universal physics
0
๏ฒ
๏ฅ
๏ƒ‘๏ƒ— ๏€ฝ
E 0
๏ƒ‘๏ƒ— ๏€ฝ
B
t
๏‚ถ
๏ƒ‘๏‚ด ๏€ฝ ๏€ญ
๏‚ถ
B
E 0 0
t
๏ญ ๏ฅ
๏‚ถ
๏ƒฆ ๏ƒถ
๏ƒ‘๏‚ด ๏€ฝ ๏€ซ
๏ƒง ๏ƒท
๏‚ถ
๏ƒจ ๏ƒธ
E
B J
Magneto โ€˜staticsโ€™
Electro โ€˜staticsโ€™
Electrodynamics Magnetodynamics
or
Integrated Circuit Potassium Ion Channel ๐‘ฒ๐•๐Ÿ.๐Ÿ
PDB: 1BL8
10
Integrated Circuit Potassium Ion Channel ๐‘ฒ๐•๐Ÿ.๐Ÿ
PDB: 1BL8
April 11, 2021
Donโ€™t Recognize these Maxwell Equations?
โ€œ โ€ฆ if we exhibit in every case all the charges, whatever their origin, the equations are always correct โ€ฆ
The fundamental equations for E โ€ฆ represent our deepest and most complete understanding of electrostatics.โ€
Section 10-4 Feynman, Leighton, and Sands (1963) The Feynman: Lectures on Physics, Vol. 2 Mainly Electromagnetism and Matter.
http://www.feynmanlectures.caltech.edu/II_toc.html
April 11, 2021
11
๐๐ข๐ฏ ๐„ = ๐†
๐œบ๐ŸŽ
๐œ๐ฎ๐ซ๐ฅ ๐„ = โˆ’
๐œ•๐
๐œ•๐‘ก
๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0 ๐‰ + ๐œ€0
๐œ•๐„
๐œ•๐‘ก
๐๐ข๐ฏ ๐ = ๐ŸŽ
is electric field, is magnetic field
is the current of all mass, including brief dielectric transients of the and fields
is charge density (of all types)
๏ฒ
E B
J P D
Relativistic
Property of
Space
NOT matter
Where is the dielectric constant ๐›†๐ซ? โ€ฆโ€ฆ
more later
April 11, 2021
12
๐๐ข๐ฏ ๐œ๐ฎ๐ซ๐ฅ ๐ = 0 = ๐œ‡0 ๐๐ข๐ฏ ๐‰ ๐‘ฅ, ๐‘ก + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก
๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0 ๐‰ ๐‘ฅ, ๐‘ก + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก
Flux of All Charges
๐๐ข๐ฏ ๐‰ ๐‘ฅ, ๐‘ก = โˆ’ ๐œ€0 ๐๐ข๐ฏ ๐œ•๐„ ๐œ•๐‘ก = โˆ’ ๐œ€0 ๐ ๐๐ข๐ฏ ๐„ ๐๐’•
But ๐๐ข๐ฏ ๐„ = ฯ ฮต0
Corollaries of Maxwellโ€™s Core Equations
Derivation of the Continuity Equation
Linking Flux and Content
๐๐ข๐ฏ ๐‰ = โˆ’ ๐œ•ฯ ๐œ•๐‘ก
Corollaries of Maxwellโ€™s Core Equations
Continuity Equation
Linking Flux and Content
April 11, 2021
13
๐๐ข๐ฏ ๐‰ = โˆ’
๐œ•ฯ
๐œ•๐‘ก
Question for Students
This is not a useful equation on atomic scale
Why?
April 11, 2021
14
Continuity Equation
Linking Flux and Content
Feynmanโ€™s Hidden Implications
Must know all charges ๐† ๐’™, ๐’š, ๐’› ๐’•
๐๐ข๐ฏ ๐‰ = โˆ’
๐œ•ฯ ๐‘ฅ, ๐‘ฆ, ๐‘ง ๐‘ก
๐œ•๐‘ก
Oh Dear!
Often impossible
at all times
April 11, 2021
15
Continuity Equation
Feynmanโ€™s Hidden Implications
Must know all charges and how they move
๐๐ข๐ฏ ๐‰ = โˆ’
๐œ•ฯ ๐‘ฅ, ๐‘ฆ, ๐‘ง ๐‘ก
๐œ•๐‘ก
Source Internet
April 11, 2021
16
Hopeless, if one must
โ€œโ€ฆ exhibit in every case all the charges,
whatever their originโ€
at all times
Section 10-4 of Feynman, Leighton, and Sands (1963) vol. 2 Electromagnetism and Matter
April 11, 2021
17
Without Conservation of Current
Need to Know ALL charges at all times!!
Hopeless in large systems
where all ions interact with each other!
April 11, 2021
18
Fortunately,
it is not hopeless
Stay Tuned
integrated circuit
Source: textbooks and internet
Seems Hopeless
April 11, 2021 19
Kirchhoffโ€™s Current Law
Brings hope
It is NOT necessary in computers to know all the charges!
Kirchhoffโ€™s Current law is (almost) enough
๐๐ข๐ฏ ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐ŸŽ = ๐œ‡0๐๐ข๐ฏ ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก
Total Current = ๐‰๐ญ๐จ๐ญ๐š๐ฅ
๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0(๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก)
April 11, 2021
20
Corollaries of Maxwell Equations
Conservation of Current
Linking Current and Electric Field
๐๐ข๐ฏ ๐‰๐ญ๐จ๐ญ๐š๐ฅ = 0
๐‰ = Flux of All Charges with mass, however small or transient
Corollaries of Maxwell Equations
Conservation of Total Current
๐๐ข๐ฏ ๐‰๐ญ๐จ๐ญ๐š๐ฅ = 0
Notice: there are ZERO adjustable or vaguely defined parameters
๐‰, ๐„, ๐‰๐ญ๐จ๐ญ๐š๐ฅ are routinely measured in laboratories
April 11, 2021
21
April 11, 2021
22
Scientists are Taught to be Skeptical
Particularly of Universal Exact Theories
as they should be!
23
April 11, 2021
Richard Feynman
โ€œWhenever you see a sweeping statement that a tremendous amount can come
from a very small number of assumptions,
You always find that it is False.
There are usually a large number of
Implied Assumptions
that are far from obvious if you think about them sufficiently carefully.โ€
Section 26-1.
The Feynman Lectures on Physics Vol 2 (1963) also at http://www.feynmanlectures.caltech.edu/II_toc.html
April 11, 2021
24
Challenge to Audience
What are implied assumptions?
in Conservation of Total Current and Core Maxwell Equations
Contact Bob.Eisenberg@gmail.com
April 11, 2021
25
Challenge to Audience
What are implied assumptions?
Hint:
Look at usual formulation of Maxwell Equations
Textbook formulation of Maxwell Equations
Depends on Dielectric Properties
Bold red means dangerously oversimplified: ๐ƒ, ๐‰, ๐œบ๐ซ, ๐œŒ๐‘“
๐๐ข๐ฏ ๐ƒ = ๐๐ข๐ฏ ๐œบ๐’“๐œ€0๐„ = ๐œŒ๐‘“
1
๐œ‡0
๐œ๐ฎ๐ซ๐ฅ ๐ = ๐‰ + ๐œบ๐ซ๐œ€0
๐œ•๐„
๐œ•๐‘ก Relativistic Property
of
Space
NOT matter
Mechanical Systems need model
of how force changes mass distribution
Stress Strain Relation is needed in mechanics
Hookeโ€™s law or its time dependent and nonlinear generalizations
Electrical Systems need model of how electrical force changes charge distribution
Polarization is Stress Strain of Charge
Model of dielectric and its time dependent and nonlinear generalizations
April 11, 2021
27
What is a Dielectric?
What is Polarization?
Gravitational Field Distorts Shape of Stars
Double Star VFTS 352
Mechanical Systems need Model
of how Force changes Mass distribution
STRESS STAIN RELATION is needed in models of mechanics
April 11, 2021
28
Source Internet
Electric Force Moves Charge so Electric Force Changes ๐†
April 11, 2021
29
Polarization of Electron Orbitals of Carbon
Source Internet and Textbooks
Polarization is Stress Strain of Charge
Polarization is almost never ideal
It always depends strongly on time
It often depends on the electric field
Source Internet
Polarization
is the Electrical Analog of the STRESS STRAIN relationship of Mechanics
Polarization is the change in Charge Distribution
when Electric Force changes
Polarization depends on time
because charge takes time to move
Polarization cannot be described by a dielectric constant independent of time
April 11, 2021
30
Dielectric Model does not fit data
April 11, 2021
31
Bulk (homogeneous, unstructured) Ionic Solution
Electrical Systems need Models
of how electrical force changes charge distribution
Electrical Systems need
Model of How Electrical Force changes Charge Distribution
Dielectric Model does not fit data from Proteins
Wolf, Gulich, Lunkenheimer & Loidl. 2012.
Biochimica et Biophysica Acta (BBA) โ€“
Proteins and Proteomics 1824:723-730.
April 11, 2021
32
80 -
- 1
as Feynman hints
Move the physics of dielectrics into ๐‰ and ๐† to make
Maxwellโ€™s Core Equations
๐๐ข๐ฏ ๐„ = ๐†
๐œบ๐ŸŽ
๐๐ข๐ฏ ๐ƒ = ๐๐ข๐ฏ ๐œบ๐’“๐œ€0๐„ = ๐œŒ๐‘“
1
๐œ‡0
๐œ๐ฎ๐ซ๐ฅ ๐ = ๐‰ + ๐œ€0
๐œ•๐„
๐œ•๐‘ก
1
๐œ‡0
๐œ๐ฎ๐ซ๐ฅ ๐ = ๐‰ + ๐œบ๐ซ๐œ€0
๐œ•๐„
๐œ•๐‘ก
Polarization is part of ๐‰ and ๐›’
When nothing is known about polarization, it is customary and appropriate to include the
dielectric constant ๐œบ๐’“ as a single real positive constant ๐œบ๐’“โ‰ฅ ๐Ÿ
Maxwellโ€™s Core Equations
Describe Electricity with no errors, <10-6
in any technological situation
April 11, 2021
34
๐๐ข๐ฏ ๐„ = ๐†
๐œบ๐ŸŽ
๐œ๐ฎ๐ซ๐ฅ ๐„ = โˆ’
๐œ•๐
๐œ•๐‘ก
๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0 ๐‰ + ๐œ€0
๐œ•๐„
๐œ•๐‘ก
๐๐ข๐ฏ ๐ = ๐ŸŽ
Implicit Assumptions are ONLY in ๐†
Relativistic
Property of
Space
NOT matter
NO Implicit Assumptions in
Conservation of Total Current
๐๐ข๐ฏ ๐‰๐ญ๐จ๐ญ๐š๐ฅ = 0
๐›’ does not appear
No adjustable parameters
๐‰ and ๐„ and ๐‰๐ญ๐จ๐ญ๐š๐ฅ are routinely measured in laboratories!!!
April 11, 2021
35
๐๐ข๐ฏ ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก = 0
Relativistic
Property of
Space
NOT matter
Flux of all charge
with mass
Conservation of Total Current
๐๐ข๐ฏ ๐‰๐ญ๐จ๐ญ๐š๐ฅ = 0
๐›’ does not appear
No adjustable parameters
๐‰ and ๐„ and ๐‰๐ญ๐จ๐ญ๐š๐ฅ are routinely measured in laboratories!!!
April 11, 2021
36
No implicit parameters or assumptions are visible
Audience:
Can you find any? Contact Bob.Eisenberg@gmail.com
April 11, 2021
37
Scientists are Taught to be Skeptical
Particularly of Universal Exact Theories
as they should be
but
Conservation of Total Current
appears to be
Universal and Exact
Independent of all properties of matter and charge
April 11, 2021 38
Conservation of Total Current is NOT a theory of everything
Conservation only describes
Total Current ๐‰๐’•๐’๐’•๐’‚๐’
When flux ๐‰ of charge is important, conservation of current is
not enough
div ๐‰ + ๐œ€0
๐œ•๐„
๐œ•๐‘ก
๐“๐จ๐ญ๐š๐ฅ ๐‚๐ฎ๐ซ๐ซ๐ž๐ง๐ญ
๐‰๐’•๐’๐’•๐’‚๐’
= 0
โŸน ๐๐ข๐ฏ ๐‰ โ‰  ๐ŸŽ
April 11, 2021 39
Conservation only describes
Total Current ๐‰๐’•๐’๐’•๐’‚๐’
When flux ๐‰ of charge or charge movement is important,
conservation of current is not enough
div ๐‰ + ๐œ€0
๐œ•๐„
๐œ•๐‘ก
= 0 โŸน div ๐‰ โ‰  ๐ŸŽ
div ๐‰ = โˆ’ div ๐œ€0
๐œ•๐„
๐œ•๐‘ก
โ‰  ๐ŸŽ
April 11, 2021 40
Flux ๐‰ of charged matter is NOT NOT NOT conserved
div ๐‰ + ๐œ€0
๐œ•๐„
๐œ•๐‘ก
= 0 โŸน ๐๐ข๐ฏ ๐‰ โ‰  ๐ŸŽ
Maxwell core Equations imply that
Charge and Matter accumulate because ๐œ€0
๐œ•E
๐œ•๐‘ก
โ‰  0
div ๐‰ = โˆ’๐œ€0
๐œ•๐„
๐œ•๐‘ก
โ‰  0
In physical language of electronics,
Some charge accumulates in the โ€˜stray capacitanceโ€™
of space
independent of matter
๐ผin
๐‘‰๐‘œ๐‘ข๐‘ก = ๐ผ๐‘–๐‘› 1 โˆ’ ๐‘’โˆ’๐‘ก ๐‘…๐ถ
Eisenberg, B., N. Gold, Z. Song, and H. Huang. 2018. What Current Flows Through a Resistor? arXiv preprint arXiv:1805.04814.
Eisenberg, R. S. 2019. Kirchhoff's Law can be Exact. arXiv preprint:1905.13574.
Relativistic
Property of
Space
NOT matter
April 11, 2021
41
In language of electronics
Flux of electrons into a Resistor does NOT equal Flux of electrons out of Resistor
Total Current I1 into a Resistor DOES EQUAL the Total Current I2 out of a Resistor
Eisenberg, B., N. Gold, Z. Song, and H. Huang. 2018. What Current Flows Through a Resistor? arXiv preprint arXiv:1805.04814.
Eisenberg, R. S. 2019. Kirchhoff's Law can be Exact. arXiv preprint available at https://arxiv.org/abs/1905.13574.
Includes
Relativistic
Property of
Space
NOT matter
April 11, 2021
42
๐๐ข๐ฏ ๐„ = 0
๐œ๐ฎ๐ซ๐ฅ ๐„ = โˆ’
๐œ•๐
๐œ•๐‘ก
๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0๐œ€0 ๐œ•๐„ ๐œ•๐‘ก
๐ธ๐‘กโ„Ž๐‘’๐‘Ÿ๐‘’๐‘Ž๐‘™ ๐ถ๐‘ข๐‘Ÿ๐‘Ÿ๐‘’๐‘›๐‘ก
= cโˆ’2
๐œ•๐„ ๐œ•๐‘ก
๐๐ข๐ฏ ๐ = ๐ŸŽ
Electromagnetic Field Exists in Vacuum
where ๐† = 0 and ๐‰ = 0 and ๐’„ = velocity of light
because of the relativistic properties space
Ethereal Current = Displacement Current
Derivation of Wave Equation is in every textbook, starting with ๐œ๐ฎ๐ซ๐ฅ ๐œ๐ฎ๐ซ๐ฅ ๐„
Relativistic
Property of
Space
NOT matter
Relativistic
Property of
Space
NOT matter
April 11, 2021 43
Source Internet
Light travels through the
Vacuum of Space
The Sun
with Prominence
Galaxy
April 11, 2021
44
Conservation of Total Current ๐‘ฑ๐’•๐’๐’•๐’‚๐’
is
Universal and Exact
because
It is a Property of Space
๐๐„ ๐๐’• in a perfect vacuum produces ๐ field
Not a property of matter
It arises from the Principle of Relativity
every textbook and
Dunstan, D. (2008) Phil Trans Roy Soc A: 366 1861
Charge does not vary when velocity โ†’ speed of light
Length, time, and (relativistic) Mass, do vary
April 11, 2021
45
Conservation of Total Current ๐‘ฑ๐’•๐’๐’•๐’‚๐’
is a
Property of Space
not matter
That is why it is Universal and Exact
An example of
Feynmanโ€™s
Hidden Factor
April 11, 2021
46
Current
Current
= ๐œบ๐ŸŽ
๐››๐„
๐๐’•
Vacuum Current
Vacuum current = Ethereal current = Displacement Current
All are names for the same thing ๐œบ๐ŸŽ ๐››๐„ ๐๐’•
Well known Example
Taught,
or should be taught,
In First Year of Physics
April 11, 2021
47
Conservation of Current is Exact and Universal
So what?
Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ must always be
described by Continuum Equations
Particle motion ๐‰ itself does NOT define Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ
Contradicts Intuition
Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ โ‰  Flux of charge ๐‰
Flux ๐‰ is defined by only particle motion
Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ is not defined by particle motion alone
April 11, 2021
48
Contradicts Intuition
Small Systems
REQUIRE
Continuum Description
of
Electric Current
Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ does NOT flow by hopping
Current is independent of location in series systems
Particle Motion can be hopping, not current
โ€œHopping Models Ignore Capacitive Currentsโ€
Paraphrase from Landauer (1992)
Conductance from transmission: common sense points.
Physica Scripta 1992 p.110
April 11, 2021
49
Eisenberg, B., N. Gold, Z. Song, and H. Huang. 2018. What Current Flows Through a
Resistor? arXiv preprint arXiv:1805.04814.
Eisenberg, R. S. 2019. Kirchhoff's Law can be Exact. arXiv preprint available at
https://arxiv.org/abs/1905.13574.
April 11, 2021
50
Contradicts Intuition
Small Systems
REQUIRE
Continuum Description
Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ
does NOT flow by hopping
Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ is independent of location in series systems
Particle Motion ๐‰ can be hopping, not total current ๐‰๐ญ๐จ๐ญ๐š๐ฅ
โ€œHopping Models Ignore Capacitive Currentsโ€
Paraphrase from Landauer (1992)
Conductance from transmission: common sense points.
Physica Scripta 1992 p.110
April 11, 2021
51
Conservation of Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ
is
EQUALITY of Total Current in a Channel
or
Series System
Landauer (1992) Physica Scripta T42 p 110.
โ€œIt is, after all, the sum of electron current and displacement current
which has no divergence.
One of those two components can take over from the other.โ€
โ€œElectrodynamic fields are endowed by unique features,
including an exquisite spatial nonlocalityโ€
Slight paraphrase of Lundeberg et al (2017)
Tuning quantum nonlocal effects plasmonics
Science 357:187-191
*
i E t
๏€ฝ ๏‚ถ ๏‚ถ ๏€ฝ ๏‚ถ ๏‚ถ
i D t
D = permittivity ๏‚ด E
Ag AgCl
Ag AgCl
but
Continuity of Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ is Exact
๐‰๐ญ๐จ๐ญ๐š๐ฅ ๐ข๐ง ๐ƒ๐ž๐ฏ๐ข๐œ๐ž ๐Ÿ = ๐‰๐ญ๐จ๐ญ๐š๐ฅ ๐ข๐ง ๐ƒ๐ž๐ฏ๐ข๐œ๐ž ๐Ÿ = ๐‰๐ญ๐จ๐ญ๐š๐ฅ ๐ข๐ง ๐ƒ๐ž๐ฏ๐ข๐œ๐ž ๐Ÿ‘ โ€ฆ
no matter what carries the current ๐‰
at all times and all locations!
Flux and Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ have very
Different Physics
in Different Systems
Eisenberg (2016) Mass Action and Conservation of Current.
Hungarian Journal of Industry and Chemistry Posted on arXiv.org with paper ID arXiv:1502.07251 44:1-28.
Conservation of Total Current ๐‰๐’•๐’๐’•๐’‚๐’ is Exact
even though
Physics of Charge Flow
Varies Profoundly
Electrodynamic Fields ๐„, ๐ take on the
Values that Conserves total Current ๐‰๐’•๐’๐’•๐’‚๐’
This is NOT mysterious
E is the force field that moves atoms
Details and PROOF
including quantum mechanics at
Eisenberg, Oriols, and Ferry. 2017. Dynamics of Current, Charge, and Mass.
Molecular Based Mathematical Biology 5:78-115
and arXiv https://arxiv.org/abs/1708.07400
so total current ๐‰ ๐‘ฅ, ๐‘ก + ฮต0 ๐œ•๐‘ฌ ๐œ•๐‘ก is always conserved
E is a force field that moves atoms
because atoms have charge
so total current ๐‰๐’•๐’๐’•๐’‚๐’ = ๐‰ ๐‘ฅ, ๐‘ก + ฮต0 ๐œ•๐‘ฌ ๐œ•๐‘ก is always conserved
Potassium Ion Channel ๐‘ฒ๐•๐Ÿ.๐Ÿ
PDB: 1BL8
Details and PROOF
including quantum mechanics at
Eisenberg, Oriols, and Ferry. 2017. Dynamics of Current, Charge, and Mass.
Molecular Based Mathematical Biology 5:78-115
and arXiv https://arxiv.org/abs/1708.07400
April 11, 2021
56
EQUALITY of Total Current ๐‰๐’•๐’๐’•๐’‚๐’
is
an Enormous Simplification
Eisenberg, B., N. Gold, Z. Song, and H. Huang. 2018. What Current Flows Through a Resistor?
arXiv preprint https://arxiv.org/abs/1805.04814.
Eisenberg, R. S. 2019. Kirchhoff's Law can be Exact. arXiv preprint available at
https://arxiv.org/abs/1905.13574.
57
What does this mean for theory and simulations?
Opportunity to Simplify Algorithms and Codes
perhaps dramatically
Spatial Dependence is Already Known
Only have to average the time dependence
Ma, Li and Liu (2016). arXiv:1605.04886; Ma, Li and Liu (2016). arXiv:1606.03625.
Differential equation in ๐’™ is not needed for ๐‰๐’•๐’๐’•๐’‚๐’
๐‰๐’•๐’๐’•๐’‚๐’ = ๐‰ + ๐›†๐ŸŽ ๐๐‘ฌ ๐๐’•
April 11, 2021
Current flow is very smooth in spatial coordinate
58
What does this mean for theory and simulations?
Opportunity to Simplify Algorithms and Codes
perhaps dramatically
Spatial Dependence is Already Known
Only have to average the time dependence
Ma, Li and Liu (2016). arXiv:1605.04886; Ma, Li and Liu (2016). arXiv:1606.03625.
Current flow is very smooth in spatial coordinate
Differential equation in ๐’™ is not needed for ๐‰๐’•๐’๐’•๐’‚๐’ = ๐‰ + ๐›†๐ŸŽ ๐๐‘ฌ ๐๐’•
April 11, 2021
๐‘ก = 0
x
t
๐‚๐ฎ๐ซ๐ซ๐ž๐ง๐ญ
Time vs
Space
One Dimensional Systems like Channels or Circuit Components
๐‚๐ฎ๐ซ๐ซ๐ž๐ง๐ญ
๐‘ก = 400
๐‘ก = 800
Current Noise ๐‰๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ is Zero in Space
April 11, 2021
59
Current Noise
๐‰๐’•๐’๐’•๐’‚๐’
is
HUGE in time
60
EQUALITY of Total Current ๐‰๐’•๐’๐’•๐’‚๐’
is
an Enormous Simplification
It can create a
It can
of Brownian Motion
into a
April 11, 2021
61
What does this mean for Mathematical Models?
The image of total current flow ๐‰๐’•๐’๐’•๐’‚๐’ is very
different
VERY SMOOTH in space
Total Current ๐‰๐’•๐’๐’•๐’‚๐’ does not vary in space so
Spatial Derivatives are not needed to
describe total current
But they are needed to describe everything else.
April 11, 2021
April 11, 2021
62
Revolution in Biophysics
Total Current flow ๐‰๐’•๐’๐’•๐’‚๐’ is equal everywhere
in a one dimensional channel
Thermal Motion in Space does not appear in
equations for flow of total current ๐‰๐’•๐’๐’•๐’‚๐’ in a
one dimensional channel
Thermal motion appears ONLY in time
Eisenberg (2020)
Electrodynamics Correlates Knock-on and Knock-off: Current is Spatially Uniform in Ion Channels.
Preprint on arXiv at https://arxiv.org/abs/2002.09012.
April 11, 2021
63
What does this mean for Ion Channels?
Knock On and Knock Off of Ions
is
IRRELEVANT for the Total Current ๐‰๐’•๐’๐’•๐’‚๐’ Through the Channel
Corry (2018) The naked truth about K+ selectivity. Nature Chemistry 10:799-800.
Eisenberg (2020)
Electrodynamics Correlates Knock-on and
Knock-off: Current is Spatially Uniform in
Ion Channels.
Preprint on arXiv at
https://arxiv.org/abs/2002.09012.
April 11, 2021
64
View of Channels has been focused on movements of individual ions
in channels,
But
Total Current ๐‰๐’•๐’๐’•๐’‚๐’ is equal everywhere
in a one dimensional channel
Position does not appear in equations for total
current ๐‰๐’•๐’๐’•๐’‚๐’ in a one dimensional channel
References and Proofs in
Eisenberg (2019) Kirchhoff's Law can be Exact. arXiv: 1905.13574
Eisenberg, Gold, Song, and Huang (2018)
What Current Flows Through a Resistor?
arXiv:1805.04814
April 11, 2021 65
Turn from Biophysics to Electricity and Electronics
And then
Back to Biology
Kirchhoffโ€™s Current Law
Should be for TOTAL CURRENT
References and Proofs in
Eisenberg (2019) Kirchhoff's Law can be Exact. arXiv: 1905.13574
Eisenberg, Gold, Song, and Huang (2018)
What Current Flows Through a Resistor?
arXiv:1805.04814
April 11, 2021
66
It is NOT necessary in our computers
to know all the charges!
Kirchhoffโ€™s law is (almost) enough
Source: textbooks and internet
Source: textbooks and internet
April 11, 2021
67
Integrated Circuits are Designed
with Kirchhoffโ€™s Current Law
and little else!!!
Hard as that is to believe
Source: textbooks and internet
Usual Derivation of Kirchhoffโ€™s law
is on
Long Time Scale โ‰ซ ๐Ÿ๐ŸŽโˆ’๐Ÿ”
sec
NOT AT ALL at ๐Ÿ๐ŸŽโˆ’๐Ÿ๐ŸŽ
sec
Usual Derivation of Kirchhoffโ€™s law is about
fluxes
BUT
FLUXES ARE NOT CONSERVED
according to experiment or Maxwell equations
NOT AT ALL at ๐Ÿ๐ŸŽโˆ’๐Ÿ๐ŸŽ
sec
April 11, 2021
70
Maxwell div ๐‰๐’•๐’๐’•๐’‚๐’ = ๐ŸŽ
and
Kirchhoff div ๐‰ โ‰  ๐ŸŽ
DISAGREE
in usual derivation of Kirchhoff
using flux ๐‰ of charges
๐‘น๐‘ช = charging time = ๐Ÿ๐ŸŽโˆ’๐Ÿ๐Ÿ farads ร— ๐Ÿ๐ŸŽ๐Ÿ‘ ohm = ๐Ÿ๐ŸŽโˆ’๐Ÿ— ๐ฌ๐ž๐œ
FLUXES ๐‰ ARE NOT CONSERVED
I๐ข๐ง
๐‘ฝ๐’๐’–๐’• = ๐‘ฐ๐’Š๐’ ๐Ÿ โˆ’ ๐’†โˆ’๐’• ๐‘น๐‘ช
April 11, 2021
72
Kirchhoffโ€™s Laws Describe TOTAL CURRENT ๐‰๐’•๐’๐’•๐’‚๐’
Not flux ๐‰
Valid whenever branched network is valid
And Maxwellโ€™s Core Equations are Valid
References and Proofs in
Eisenberg (2019) Kirchhoff's Law can be Exact. arXiv: 1905.13574
Eisenberg, Gold, Song, and Huang (2018)
What Current Flows Through a Resistor?
arXiv:1805.04814
April 11, 2021
73
Deriving Kirchhoffโ€™s Laws
from Maxwell Equations
and conservation of current
is
Trivial if you use Total Current ๐‰๐’•๐’๐’•๐’‚๐’
References and Proofs in
Eisenberg (2019) Kirchhoff's Law can be Exact.
arXiv: 1905.13574
Eisenberg, Gold, Song, and Huang (2018)
What Current Flows Through a Resistor?
arXiv:1805.04814
April 11, 2021
74
All is obvious to a fine practicing engineer and old friend
โ€œBob, why do you need all that math?
Everyone knows how to use Kirchhoff.
Everyone knows you have to include the displacement current.
No one would try to keep track of all the chargesโ€
Paraphrase of email exchange, with permission
Alan Finkel
Co-designer* of AxoPatch
Amplifier
Founder Axon Instruments,
Recently
Chief Scientist
Australian Goverment
*with Eisenberg, Levis, and Rae
April 11, 2021
75
Conservation of Total Current
is important in
Biology
April 11, 2021
76
Conservation of Current
is
Practically Important
in
Understanding
Transporters
Oxidative
Phosphorylation
Photosynthesis
main processes in life
Applying Maxwell to Transporters
๐๐ข๐ฏ ๐‰ ๐‘ฅ, ๐‘ก + ๐œ€0
๐œ•๐„ ๐‘ฅ, ๐‘ก
๐œ•๐‘ก
= ๐ŸŽ
Sum of Currents in a Transporter = zero in โ€˜small cellโ€™, mitochondrion, HHK, etc.
so
Currents are Coupled in a Transporter in a โ€˜small cellโ€™
Currents are NOT coupled by Conservation of Current
in standard bilayer setup
Conservation of
Total Current
Source internet Liu, Hsieh, and Eisenberg (2016)
J Phys Chem B 120:2658-2669
Bilayer Setup โ€˜voltage clampโ€™
Inhomogeneous Dirichlet Condition
for Classic Voltage Clamp Hodgkin Huxley 1952
Natural Setup: small cell, etc.
Homogeneous Neumann Boundary Condition for total current
Fig. 10 of Hodgkin Huxley Katz 1952
Na+ Ca++
Na+ Ca++
๐ผ = ๐ผ๐‘๐‘Ž + ๐ผ๐ถ๐‘Ž = ๐ŸŽ
๐ผ๐‘๐‘Ž = โˆ’๐ผ๐ถ๐‘Ž
๐ผ๐‘๐‘Ž ๐ผ๐ถ๐‘Ž
Independent
Currents
79
Biophysical Prediction
Eisenberg (2020)
Electrodynamics Correlates Knock-on and Knock-off: Current is Spatially Uniform in Ion Channels.
Preprint on arXiv at https://arxiv.org/abs/2002.09012.
Applying Maxwell To
Mitochondrion
Depends on
Conservation of Current
Source Internet
April 11, 2021
81
Without Conservation of Current
Need to Know ALL charges at all times!!
Hopeless in large systems
where all ions interact with each other!
NOTE
Chemical Kinetics does not conserve current,
in its usual form
Does Molecular Dynamics conserve current?
April 11, 2021
82
With Conservation of Current
no more difficult than
large circuit problems
April 11, 2021 83
Any Questions?
April 11, 2021 84
Extra Slides
April 11, 2021 85
Polarization of Matter ฮตr โˆ’ 1 ฮต0
๐œบ๐’“ involves all movements of matter that do not translate mass,
roughly speaking
๐œบ๐’“ โˆ’ ๐Ÿ ๐œบ๐ŸŽ
is as complex
as the motion of matter itself.
Seems hopeless to make a general theory
What are the problems with textbook Maxwell Equations?
๐œบ๐’“๐œบ๐ŸŽ is a hybrid
๐๐‘ฌ ๐๐’• creating ๐‘ฉ field in a vacuum
is
Mysterious
Electric & Magnetic Fields takes on the
Value that Conserves Current
Details and PROOF
including quantum mechanics at
https://arxiv.org/abs/1609.09175
Specifically,
๐„ & ๐ moves atoms
Creates the โ€˜etherealโ€™ current ฮต๐ŸŽ ๐๐„ ๐๐’•
So total current ๐‰ + ฮต๐ŸŽ ๐๐„ ๐๐’• is always conserved
April 11, 2021 88
Profound Implications of One Dimensional Systems for atomic
view of ion channels
Spatial Variable does NOT appear
in description of current in a one
dimensional channel
April 11, 2021 89
Spatial Variable does NOT appear
in description of current in a one
dimensional channel
April 11, 2021 90
Hopping Model is
COMPLETELY INAPPROPRIATE
for current that is uniform in ๐’™
April 11, 2021 91
Spatial Variable does appear in
description of ion movement in a
one dimensional channel
April 11, 2021 92
Spatial Variable does NOT appear
in description of current in a one
dimensional channel
April 11, 2021 93
Spatial Variable does NOT appear in description of current in a
one dimensional channel
We need a Molecular Dynamics that
1) conserves current
2) has one dielectric constant
3) extends to biological time scales
April 11, 2021 94
Spatial Variable does NOT appear in description of
current in a one dimensional channel
Quasi-particle for current CONDUCTON
left over is DIFFUSON + POLARON.
๐šบ = PERMION*
*Elber, Chen, Rojewska, and Eisenberg. 1995.
Sodium in gramicidin: An example of a permion.
Biophys. J. 68:906-924.
April 11, 2021 95
With Conservation of Current
mitochondria are no more difficult than
large circuit problems
Applying Maxwell to Mitochondria
Seems Hopeless
Source: textbooks and internet
But Stay Tuned for Future Work
Applying Maxwell To Mitochondrion
Depends on
Conservation of Current
and depends on collaboration of Oscar Juarez, Chun Liu, and Bob Eisenberg
April 11, 2021 98
With Conservation of Current
no more difficult than
large circuit problems
April 11, 2021 99
Spatial Variable does NOT appear in description of
current in a one dimensional channel
Another way is to include equality of current
as a constraint in time averaging schemes
e.g., of Ma and Liu
Ma, Li, and Liu. 2016.. arXiv:1605.04886.
Ma, Li, and Liu. 2016. arXiv:1606.03625.
Derivation of Kirchhoffโ€™s Law is at DC
Derivation of Kirchhoffโ€™s law is about fluxes
How can that work in a computer at ๐Ÿ๐ŸŽโˆ’๐Ÿ๐ŸŽ
sec?
References and Proofs in
Eisenberg (2019) Kirchhoff's Law can be Exact. arXiv: 1905.13574
Eisenberg, Gold, Song, and Huang (2018)
What Current Flows Through a Resistor?
arXiv:1805.04814
April 11, 2021 101
Traditional Form of Maxwell Equations Cannot be Used
Maxwellโ€™s equations do not deal with
Diffusion
Convection
Complex materials
Complicated dielectric properties
Eisenberg, 2019. Dielectric Dilemma. arXxiv: 1901.10805.
April 11, 2021 102
It is necessary to update Maxwellโ€™s Equations
to see how
Kirchhoffโ€™s law & Conservation of Current
apply to
Complex Liquids
and
Complex Biological Systems
Eisenberg, R. S. 2019. Updating Maxwell with Electrons, Charge, and More Realistic
Polarization. arXiv 1904.09695
.
Eisenberg, Oriols, and Ferry. 2017. Dynamics of Current, Charge, and Mass. Molecular Based
Mathematical Biology 5:78-115 and arXiv preprint 1708.07400.
April 11, 2021 103
It is necessary to update Maxwellโ€™s Equations
https://arxiv.org/abs/1904.09695
Not just my opinion
This is the opinion* of Nobel Prize winners in Physics,
Richard Feynman
(quantum electrodynamics)
and
Edward Purcell
(nuclear magnetic resonance)
*p. 10-7 of Feynman, Leighton, and Sands. 1963. Mainly Electromagnetism and Matter
*p. 506 of Purcell and Morin. 2013. Electricity and Magnetism
April 11, 2021 104
Maxwellโ€™s equations do not deal with
Diffusion
Convection
Complex materials
Complicated dielectric properties
Indeed, Maxwellโ€™s original equations do not include ions or electrons or their movement!
Textbook treatments do not deal with other forces like diffusion or convection at all.
What are the PHYSICAL problems
with traditional Maxwell Equations?
Eisenberg, 2019. Dielectric Dilemma. arXxiv: 1901.10805.
105
NOT hopeless,
Maxwell Predicts Important Biophysics
Independent
of details of the Mitochondrion
if a
branched
One-dimensional Formulation
is appropriate
April 11, 2021 106
Inside Channels
PROFOUND SIMIPLIFICATION
If we can figure out how to exploit it
April 11, 2021 107
Profound Implications of One
Dimensional Systems for atomic
view of ion channels
Current is equal everywhere in a channel
At all times and under all conditions
that the Maxwell Equations Apply
April 11, 2021 108
April 11, 2021 109
Polarization of Matter ฮตr โˆ’ 1 ฮต0
๐œบ๐’“ involves all movements of matter that do not translate mass,
roughly speaking
๐œบ๐’“ โˆ’ ๐Ÿ ๐œบ๐ŸŽ
is as complex
as the motion of matter itself.
Seems hopeless to make a general theory
What are the problems with textbook Maxwell Equations?
๐œบ๐’“๐œบ๐ŸŽ is a hybrid
April 11, 2021 110
Continuity of Current is Exact in
Kelvinโ€™s Submarine Telegraph
๐’Š๐๐ž๐ฐ๐Ÿ๐จ๐ฎ๐ง๐๐ฅ๐š๐ง๐ = ๐’Š๐ˆ๐ซ๐ž๐ฅ๐š๐ง๐
How can that possibly be true?
April 11, 2021 111
It is NOT necessary to know the charges
to understand one crucial property of current.
Total Current is conserved
independent of any property of charge or matter
Conservation of Current
๐๐ข๐ฏ ๐‰๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ = 0
Applying Maxwell to Transporters
1) Sum of Currents in a Transporter is zero in โ€˜small cellโ€™, mitochondrion, etc.
2) Currents are Coupled in a Transporter in a natural setting by Maxwell
3) Bilayer set up does NOT require currents to sum to zero.
Bilayer setup sets voltage across transporter, currents are not controlled.
4) So transporter currents are NOT coupled by Conservation of Current
in standard bilayer setup
Natural Setting
Experimental Setting
Polarization of Electron Orbitals
April 11, 2021
113
Source Internet

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Core Maxwell Equations are Scary April 11, 2021

  • 1. Maxwellโ€™s Core Equations Exact, Universal, and Scary April 11, 2021 1 Robert S. Eisenberg Bard Endowed Professor and Chair, emeritus Department of Physiology and Biophysics Rush University Adjunct Professor Department of Applied Mathematics Illinois Institute of Technology Chicago IL USA
  • 2. Tufts Math Department April 11, 2021 2 Presented March 29, 2021
  • 3. April 11, 2021 3 Abstract When the Maxwell equations are written without a dielectric constant, they are universal and exact, for biological and technological applications, from inside atoms to between stars. Dielectric and polarization phenomena need then to be described by stress strain relations for charge, that show how charge redistributes when the electric field is changed, in each system of interest. Conservation of total current (including the ethereal displacement current ๐œบ๐ŸŽ ๐๐„ ๐๐’•) is then as exact as the Maxwell equations themselves and independent of any property of matter. It is a consequence of the Lorentz invariance of the elementary charge, a property of all locally inertial systems, described by the theory of relativity. Exact Conservation of Total Current allows a redefinition of Kirchhoffโ€™s current law that is itself exact. In unbranched systems like circuit components or ion channels, conservation of total current becomes equality. Spatial dependence of total current disappears in that case. Hopping phenomena disappear. Spatial Brownian motion disappears. The infinite variation of a Brownian model of thermal noise becomes the zero spatial variation of total current. Maxwellโ€™s Core Equations become a perfect (spatial) low pass filter. An Exact and Universal theory of Electrodynamics is a scary challenge to scientists like me, trained to be skeptical of all sweeping claims to perfection.
  • 4. 4 Mathematics describes only a tiny part of life, ๏ƒฒ ๏ƒฅ u ๏‚ถ ๏‚ถ April 11, 2021
  • 5. 5 But Mathematics* Creates our Standard of Living Electronics, Electricity, Computers, Mobile Phones, TV, Games and Fluid Dynamics, Optics, Structural Mechanics, โ€ฆ. ๏ƒฒ ๏ƒฅ u ๏‚ถ ๏‚ถ April 11, 2021
  • 6. Essence of Electrodynamics is Maxwellโ€™s Core Equations for the Flows and Forces of Charge and Current in matter and space April 11, 2021 6 Nearly Exact and Universal from Stars to inside atoms Eisenberg, Oriols, and Ferry (2017) Dynamics of Current, Charge, and Mass. Molecular Based Mathematical Biology 5:78-115 and arXiv preprint https://arxiv.org/abs/1708.07400.
  • 7. is electric field, is magnetic field is the current of all mass, including brief dielectric transients of the and fields is charge density (of all types, including dielectric charge of the ๏ฒ E B J P D P ๏€จ ๏€ฉ 0 0 0 0 and fields) is the permittivity of a vacuum is the permeability of a vacuum velocity of light (!) ๏ฅ ๏ญ ๏ญ ๏ฅ ๏€ฝ D -0.5 Maxwellโ€™s Core Equations Describe Electricity with errors <10-6 in biological and technological applications April 11, 2021 7 ๐๐ข๐ฏ ๐„ = ๐† ๐œบ๐ŸŽ ๐œ๐ฎ๐ซ๐ฅ ๐„ = โˆ’ ๐œ•๐ ๐œ•๐‘ก ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0 ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก ๐๐ข๐ฏ ๐ = ๐ŸŽ
  • 8. 8 Advanced Photon Source Argonne National Laboratory Beam ~๐Ÿ๐ŸŽ๐Ÿ๐ŸŽ eV Beam length ๐Ÿ๐ŸŽ๐Ÿ‘ m Tolerance < ๐Ÿ๐ŸŽโˆ’๐Ÿ• m Beam Current ๐Ÿ๐ŸŽ๐ŸŽ mA Beam Power ๐Ÿ๐ŸŽ๐Ÿ— ๐ฐ๐š๐ญ๐ญ๐ฌ Error in Theory < ๐Ÿ๐ŸŽโˆ’๐Ÿ๐ŸŽ Source Internet April 11, 2021
  • 9. 9 April 11, 2021 Richard Feynman โ€œWhenever you see a sweeping statement that a tremendous amount can come from a very small number of assumptions, You always find that it is False There are usually a large number of Implied Assumptions that are far from obvious if you think about them sufficiently carefully.โ€ Section 26-1. The Feynman Lectures on Physics, Mainly Electromagnetism and Matter 1963 also at http://www.feynmanlectures.caltech.edu/II_toc.html CHALLENGE TO THE AUDIENCE Find and Discuss the Implied Assumptions in this Talk Contact me at Bob.Eisenberg@gmail.com
  • 10. Maxwellโ€™s Core Equations are Universal and Exact But they are Complicated Differential Equations need very complicated mathematics to describe universal physics 0 ๏ฒ ๏ฅ ๏ƒ‘๏ƒ— ๏€ฝ E 0 ๏ƒ‘๏ƒ— ๏€ฝ B t ๏‚ถ ๏ƒ‘๏‚ด ๏€ฝ ๏€ญ ๏‚ถ B E 0 0 t ๏ญ ๏ฅ ๏‚ถ ๏ƒฆ ๏ƒถ ๏ƒ‘๏‚ด ๏€ฝ ๏€ซ ๏ƒง ๏ƒท ๏‚ถ ๏ƒจ ๏ƒธ E B J Magneto โ€˜staticsโ€™ Electro โ€˜staticsโ€™ Electrodynamics Magnetodynamics or Integrated Circuit Potassium Ion Channel ๐‘ฒ๐•๐Ÿ.๐Ÿ PDB: 1BL8 10 Integrated Circuit Potassium Ion Channel ๐‘ฒ๐•๐Ÿ.๐Ÿ PDB: 1BL8 April 11, 2021
  • 11. Donโ€™t Recognize these Maxwell Equations? โ€œ โ€ฆ if we exhibit in every case all the charges, whatever their origin, the equations are always correct โ€ฆ The fundamental equations for E โ€ฆ represent our deepest and most complete understanding of electrostatics.โ€ Section 10-4 Feynman, Leighton, and Sands (1963) The Feynman: Lectures on Physics, Vol. 2 Mainly Electromagnetism and Matter. http://www.feynmanlectures.caltech.edu/II_toc.html April 11, 2021 11 ๐๐ข๐ฏ ๐„ = ๐† ๐œบ๐ŸŽ ๐œ๐ฎ๐ซ๐ฅ ๐„ = โˆ’ ๐œ•๐ ๐œ•๐‘ก ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0 ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก ๐๐ข๐ฏ ๐ = ๐ŸŽ is electric field, is magnetic field is the current of all mass, including brief dielectric transients of the and fields is charge density (of all types) ๏ฒ E B J P D Relativistic Property of Space NOT matter Where is the dielectric constant ๐›†๐ซ? โ€ฆโ€ฆ more later
  • 12. April 11, 2021 12 ๐๐ข๐ฏ ๐œ๐ฎ๐ซ๐ฅ ๐ = 0 = ๐œ‡0 ๐๐ข๐ฏ ๐‰ ๐‘ฅ, ๐‘ก + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0 ๐‰ ๐‘ฅ, ๐‘ก + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก Flux of All Charges ๐๐ข๐ฏ ๐‰ ๐‘ฅ, ๐‘ก = โˆ’ ๐œ€0 ๐๐ข๐ฏ ๐œ•๐„ ๐œ•๐‘ก = โˆ’ ๐œ€0 ๐ ๐๐ข๐ฏ ๐„ ๐๐’• But ๐๐ข๐ฏ ๐„ = ฯ ฮต0 Corollaries of Maxwellโ€™s Core Equations Derivation of the Continuity Equation Linking Flux and Content ๐๐ข๐ฏ ๐‰ = โˆ’ ๐œ•ฯ ๐œ•๐‘ก
  • 13. Corollaries of Maxwellโ€™s Core Equations Continuity Equation Linking Flux and Content April 11, 2021 13 ๐๐ข๐ฏ ๐‰ = โˆ’ ๐œ•ฯ ๐œ•๐‘ก Question for Students This is not a useful equation on atomic scale Why?
  • 14. April 11, 2021 14 Continuity Equation Linking Flux and Content Feynmanโ€™s Hidden Implications Must know all charges ๐† ๐’™, ๐’š, ๐’› ๐’• ๐๐ข๐ฏ ๐‰ = โˆ’ ๐œ•ฯ ๐‘ฅ, ๐‘ฆ, ๐‘ง ๐‘ก ๐œ•๐‘ก Oh Dear! Often impossible at all times
  • 15. April 11, 2021 15 Continuity Equation Feynmanโ€™s Hidden Implications Must know all charges and how they move ๐๐ข๐ฏ ๐‰ = โˆ’ ๐œ•ฯ ๐‘ฅ, ๐‘ฆ, ๐‘ง ๐‘ก ๐œ•๐‘ก Source Internet
  • 16. April 11, 2021 16 Hopeless, if one must โ€œโ€ฆ exhibit in every case all the charges, whatever their originโ€ at all times Section 10-4 of Feynman, Leighton, and Sands (1963) vol. 2 Electromagnetism and Matter
  • 17. April 11, 2021 17 Without Conservation of Current Need to Know ALL charges at all times!! Hopeless in large systems where all ions interact with each other!
  • 18. April 11, 2021 18 Fortunately, it is not hopeless Stay Tuned integrated circuit Source: textbooks and internet Seems Hopeless
  • 19. April 11, 2021 19 Kirchhoffโ€™s Current Law Brings hope It is NOT necessary in computers to know all the charges! Kirchhoffโ€™s Current law is (almost) enough
  • 20. ๐๐ข๐ฏ ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐ŸŽ = ๐œ‡0๐๐ข๐ฏ ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก Total Current = ๐‰๐ญ๐จ๐ญ๐š๐ฅ ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0(๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก) April 11, 2021 20 Corollaries of Maxwell Equations Conservation of Current Linking Current and Electric Field ๐๐ข๐ฏ ๐‰๐ญ๐จ๐ญ๐š๐ฅ = 0 ๐‰ = Flux of All Charges with mass, however small or transient
  • 21. Corollaries of Maxwell Equations Conservation of Total Current ๐๐ข๐ฏ ๐‰๐ญ๐จ๐ญ๐š๐ฅ = 0 Notice: there are ZERO adjustable or vaguely defined parameters ๐‰, ๐„, ๐‰๐ญ๐จ๐ญ๐š๐ฅ are routinely measured in laboratories April 11, 2021 21
  • 22. April 11, 2021 22 Scientists are Taught to be Skeptical Particularly of Universal Exact Theories as they should be!
  • 23. 23 April 11, 2021 Richard Feynman โ€œWhenever you see a sweeping statement that a tremendous amount can come from a very small number of assumptions, You always find that it is False. There are usually a large number of Implied Assumptions that are far from obvious if you think about them sufficiently carefully.โ€ Section 26-1. The Feynman Lectures on Physics Vol 2 (1963) also at http://www.feynmanlectures.caltech.edu/II_toc.html
  • 24. April 11, 2021 24 Challenge to Audience What are implied assumptions? in Conservation of Total Current and Core Maxwell Equations Contact Bob.Eisenberg@gmail.com
  • 25. April 11, 2021 25 Challenge to Audience What are implied assumptions? Hint: Look at usual formulation of Maxwell Equations
  • 26. Textbook formulation of Maxwell Equations Depends on Dielectric Properties Bold red means dangerously oversimplified: ๐ƒ, ๐‰, ๐œบ๐ซ, ๐œŒ๐‘“ ๐๐ข๐ฏ ๐ƒ = ๐๐ข๐ฏ ๐œบ๐’“๐œ€0๐„ = ๐œŒ๐‘“ 1 ๐œ‡0 ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐‰ + ๐œบ๐ซ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก Relativistic Property of Space NOT matter
  • 27. Mechanical Systems need model of how force changes mass distribution Stress Strain Relation is needed in mechanics Hookeโ€™s law or its time dependent and nonlinear generalizations Electrical Systems need model of how electrical force changes charge distribution Polarization is Stress Strain of Charge Model of dielectric and its time dependent and nonlinear generalizations April 11, 2021 27 What is a Dielectric? What is Polarization?
  • 28. Gravitational Field Distorts Shape of Stars Double Star VFTS 352 Mechanical Systems need Model of how Force changes Mass distribution STRESS STAIN RELATION is needed in models of mechanics April 11, 2021 28 Source Internet
  • 29. Electric Force Moves Charge so Electric Force Changes ๐† April 11, 2021 29 Polarization of Electron Orbitals of Carbon Source Internet and Textbooks Polarization is Stress Strain of Charge Polarization is almost never ideal It always depends strongly on time It often depends on the electric field Source Internet
  • 30. Polarization is the Electrical Analog of the STRESS STRAIN relationship of Mechanics Polarization is the change in Charge Distribution when Electric Force changes Polarization depends on time because charge takes time to move Polarization cannot be described by a dielectric constant independent of time April 11, 2021 30
  • 31. Dielectric Model does not fit data April 11, 2021 31 Bulk (homogeneous, unstructured) Ionic Solution Electrical Systems need Models of how electrical force changes charge distribution
  • 32. Electrical Systems need Model of How Electrical Force changes Charge Distribution Dielectric Model does not fit data from Proteins Wolf, Gulich, Lunkenheimer & Loidl. 2012. Biochimica et Biophysica Acta (BBA) โ€“ Proteins and Proteomics 1824:723-730. April 11, 2021 32 80 - - 1
  • 33. as Feynman hints Move the physics of dielectrics into ๐‰ and ๐† to make Maxwellโ€™s Core Equations ๐๐ข๐ฏ ๐„ = ๐† ๐œบ๐ŸŽ ๐๐ข๐ฏ ๐ƒ = ๐๐ข๐ฏ ๐œบ๐’“๐œ€0๐„ = ๐œŒ๐‘“ 1 ๐œ‡0 ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก 1 ๐œ‡0 ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐‰ + ๐œบ๐ซ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก Polarization is part of ๐‰ and ๐›’ When nothing is known about polarization, it is customary and appropriate to include the dielectric constant ๐œบ๐’“ as a single real positive constant ๐œบ๐’“โ‰ฅ ๐Ÿ
  • 34. Maxwellโ€™s Core Equations Describe Electricity with no errors, <10-6 in any technological situation April 11, 2021 34 ๐๐ข๐ฏ ๐„ = ๐† ๐œบ๐ŸŽ ๐œ๐ฎ๐ซ๐ฅ ๐„ = โˆ’ ๐œ•๐ ๐œ•๐‘ก ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0 ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก ๐๐ข๐ฏ ๐ = ๐ŸŽ Implicit Assumptions are ONLY in ๐† Relativistic Property of Space NOT matter
  • 35. NO Implicit Assumptions in Conservation of Total Current ๐๐ข๐ฏ ๐‰๐ญ๐จ๐ญ๐š๐ฅ = 0 ๐›’ does not appear No adjustable parameters ๐‰ and ๐„ and ๐‰๐ญ๐จ๐ญ๐š๐ฅ are routinely measured in laboratories!!! April 11, 2021 35 ๐๐ข๐ฏ ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก = 0 Relativistic Property of Space NOT matter Flux of all charge with mass
  • 36. Conservation of Total Current ๐๐ข๐ฏ ๐‰๐ญ๐จ๐ญ๐š๐ฅ = 0 ๐›’ does not appear No adjustable parameters ๐‰ and ๐„ and ๐‰๐ญ๐จ๐ญ๐š๐ฅ are routinely measured in laboratories!!! April 11, 2021 36 No implicit parameters or assumptions are visible Audience: Can you find any? Contact Bob.Eisenberg@gmail.com
  • 37. April 11, 2021 37 Scientists are Taught to be Skeptical Particularly of Universal Exact Theories as they should be but Conservation of Total Current appears to be Universal and Exact Independent of all properties of matter and charge
  • 38. April 11, 2021 38 Conservation of Total Current is NOT a theory of everything Conservation only describes Total Current ๐‰๐’•๐’๐’•๐’‚๐’ When flux ๐‰ of charge is important, conservation of current is not enough div ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก ๐“๐จ๐ญ๐š๐ฅ ๐‚๐ฎ๐ซ๐ซ๐ž๐ง๐ญ ๐‰๐’•๐’๐’•๐’‚๐’ = 0 โŸน ๐๐ข๐ฏ ๐‰ โ‰  ๐ŸŽ
  • 39. April 11, 2021 39 Conservation only describes Total Current ๐‰๐’•๐’๐’•๐’‚๐’ When flux ๐‰ of charge or charge movement is important, conservation of current is not enough div ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก = 0 โŸน div ๐‰ โ‰  ๐ŸŽ div ๐‰ = โˆ’ div ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก โ‰  ๐ŸŽ
  • 40. April 11, 2021 40 Flux ๐‰ of charged matter is NOT NOT NOT conserved div ๐‰ + ๐œ€0 ๐œ•๐„ ๐œ•๐‘ก = 0 โŸน ๐๐ข๐ฏ ๐‰ โ‰  ๐ŸŽ Maxwell core Equations imply that Charge and Matter accumulate because ๐œ€0 ๐œ•E ๐œ•๐‘ก โ‰  0 div ๐‰ = โˆ’๐œ€0 ๐œ•๐„ ๐œ•๐‘ก โ‰  0 In physical language of electronics, Some charge accumulates in the โ€˜stray capacitanceโ€™ of space independent of matter ๐ผin ๐‘‰๐‘œ๐‘ข๐‘ก = ๐ผ๐‘–๐‘› 1 โˆ’ ๐‘’โˆ’๐‘ก ๐‘…๐ถ Eisenberg, B., N. Gold, Z. Song, and H. Huang. 2018. What Current Flows Through a Resistor? arXiv preprint arXiv:1805.04814. Eisenberg, R. S. 2019. Kirchhoff's Law can be Exact. arXiv preprint:1905.13574. Relativistic Property of Space NOT matter
  • 41. April 11, 2021 41 In language of electronics Flux of electrons into a Resistor does NOT equal Flux of electrons out of Resistor Total Current I1 into a Resistor DOES EQUAL the Total Current I2 out of a Resistor Eisenberg, B., N. Gold, Z. Song, and H. Huang. 2018. What Current Flows Through a Resistor? arXiv preprint arXiv:1805.04814. Eisenberg, R. S. 2019. Kirchhoff's Law can be Exact. arXiv preprint available at https://arxiv.org/abs/1905.13574. Includes Relativistic Property of Space NOT matter
  • 42. April 11, 2021 42 ๐๐ข๐ฏ ๐„ = 0 ๐œ๐ฎ๐ซ๐ฅ ๐„ = โˆ’ ๐œ•๐ ๐œ•๐‘ก ๐œ๐ฎ๐ซ๐ฅ ๐ = ๐œ‡0๐œ€0 ๐œ•๐„ ๐œ•๐‘ก ๐ธ๐‘กโ„Ž๐‘’๐‘Ÿ๐‘’๐‘Ž๐‘™ ๐ถ๐‘ข๐‘Ÿ๐‘Ÿ๐‘’๐‘›๐‘ก = cโˆ’2 ๐œ•๐„ ๐œ•๐‘ก ๐๐ข๐ฏ ๐ = ๐ŸŽ Electromagnetic Field Exists in Vacuum where ๐† = 0 and ๐‰ = 0 and ๐’„ = velocity of light because of the relativistic properties space Ethereal Current = Displacement Current Derivation of Wave Equation is in every textbook, starting with ๐œ๐ฎ๐ซ๐ฅ ๐œ๐ฎ๐ซ๐ฅ ๐„ Relativistic Property of Space NOT matter Relativistic Property of Space NOT matter
  • 43. April 11, 2021 43 Source Internet Light travels through the Vacuum of Space The Sun with Prominence Galaxy
  • 44. April 11, 2021 44 Conservation of Total Current ๐‘ฑ๐’•๐’๐’•๐’‚๐’ is Universal and Exact because It is a Property of Space ๐๐„ ๐๐’• in a perfect vacuum produces ๐ field Not a property of matter It arises from the Principle of Relativity every textbook and Dunstan, D. (2008) Phil Trans Roy Soc A: 366 1861 Charge does not vary when velocity โ†’ speed of light Length, time, and (relativistic) Mass, do vary
  • 45. April 11, 2021 45 Conservation of Total Current ๐‘ฑ๐’•๐’๐’•๐’‚๐’ is a Property of Space not matter That is why it is Universal and Exact An example of Feynmanโ€™s Hidden Factor
  • 46. April 11, 2021 46 Current Current = ๐œบ๐ŸŽ ๐››๐„ ๐๐’• Vacuum Current Vacuum current = Ethereal current = Displacement Current All are names for the same thing ๐œบ๐ŸŽ ๐››๐„ ๐๐’• Well known Example Taught, or should be taught, In First Year of Physics
  • 47. April 11, 2021 47 Conservation of Current is Exact and Universal So what? Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ must always be described by Continuum Equations Particle motion ๐‰ itself does NOT define Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ Contradicts Intuition Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ โ‰  Flux of charge ๐‰ Flux ๐‰ is defined by only particle motion Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ is not defined by particle motion alone
  • 48. April 11, 2021 48 Contradicts Intuition Small Systems REQUIRE Continuum Description of Electric Current Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ does NOT flow by hopping Current is independent of location in series systems Particle Motion can be hopping, not current โ€œHopping Models Ignore Capacitive Currentsโ€ Paraphrase from Landauer (1992) Conductance from transmission: common sense points. Physica Scripta 1992 p.110
  • 49. April 11, 2021 49 Eisenberg, B., N. Gold, Z. Song, and H. Huang. 2018. What Current Flows Through a Resistor? arXiv preprint arXiv:1805.04814. Eisenberg, R. S. 2019. Kirchhoff's Law can be Exact. arXiv preprint available at https://arxiv.org/abs/1905.13574.
  • 50. April 11, 2021 50 Contradicts Intuition Small Systems REQUIRE Continuum Description Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ does NOT flow by hopping Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ is independent of location in series systems Particle Motion ๐‰ can be hopping, not total current ๐‰๐ญ๐จ๐ญ๐š๐ฅ โ€œHopping Models Ignore Capacitive Currentsโ€ Paraphrase from Landauer (1992) Conductance from transmission: common sense points. Physica Scripta 1992 p.110
  • 51. April 11, 2021 51 Conservation of Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ is EQUALITY of Total Current in a Channel or Series System Landauer (1992) Physica Scripta T42 p 110. โ€œIt is, after all, the sum of electron current and displacement current which has no divergence. One of those two components can take over from the other.โ€ โ€œElectrodynamic fields are endowed by unique features, including an exquisite spatial nonlocalityโ€ Slight paraphrase of Lundeberg et al (2017) Tuning quantum nonlocal effects plasmonics Science 357:187-191
  • 52. * i E t ๏€ฝ ๏‚ถ ๏‚ถ ๏€ฝ ๏‚ถ ๏‚ถ i D t D = permittivity ๏‚ด E Ag AgCl Ag AgCl but Continuity of Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ is Exact ๐‰๐ญ๐จ๐ญ๐š๐ฅ ๐ข๐ง ๐ƒ๐ž๐ฏ๐ข๐œ๐ž ๐Ÿ = ๐‰๐ญ๐จ๐ญ๐š๐ฅ ๐ข๐ง ๐ƒ๐ž๐ฏ๐ข๐œ๐ž ๐Ÿ = ๐‰๐ญ๐จ๐ญ๐š๐ฅ ๐ข๐ง ๐ƒ๐ž๐ฏ๐ข๐œ๐ž ๐Ÿ‘ โ€ฆ no matter what carries the current ๐‰ at all times and all locations! Flux and Total Current ๐‰๐ญ๐จ๐ญ๐š๐ฅ have very Different Physics in Different Systems Eisenberg (2016) Mass Action and Conservation of Current. Hungarian Journal of Industry and Chemistry Posted on arXiv.org with paper ID arXiv:1502.07251 44:1-28.
  • 53. Conservation of Total Current ๐‰๐’•๐’๐’•๐’‚๐’ is Exact even though Physics of Charge Flow Varies Profoundly
  • 54. Electrodynamic Fields ๐„, ๐ take on the Values that Conserves total Current ๐‰๐’•๐’๐’•๐’‚๐’ This is NOT mysterious E is the force field that moves atoms Details and PROOF including quantum mechanics at Eisenberg, Oriols, and Ferry. 2017. Dynamics of Current, Charge, and Mass. Molecular Based Mathematical Biology 5:78-115 and arXiv https://arxiv.org/abs/1708.07400 so total current ๐‰ ๐‘ฅ, ๐‘ก + ฮต0 ๐œ•๐‘ฌ ๐œ•๐‘ก is always conserved
  • 55. E is a force field that moves atoms because atoms have charge so total current ๐‰๐’•๐’๐’•๐’‚๐’ = ๐‰ ๐‘ฅ, ๐‘ก + ฮต0 ๐œ•๐‘ฌ ๐œ•๐‘ก is always conserved Potassium Ion Channel ๐‘ฒ๐•๐Ÿ.๐Ÿ PDB: 1BL8 Details and PROOF including quantum mechanics at Eisenberg, Oriols, and Ferry. 2017. Dynamics of Current, Charge, and Mass. Molecular Based Mathematical Biology 5:78-115 and arXiv https://arxiv.org/abs/1708.07400
  • 56. April 11, 2021 56 EQUALITY of Total Current ๐‰๐’•๐’๐’•๐’‚๐’ is an Enormous Simplification Eisenberg, B., N. Gold, Z. Song, and H. Huang. 2018. What Current Flows Through a Resistor? arXiv preprint https://arxiv.org/abs/1805.04814. Eisenberg, R. S. 2019. Kirchhoff's Law can be Exact. arXiv preprint available at https://arxiv.org/abs/1905.13574.
  • 57. 57 What does this mean for theory and simulations? Opportunity to Simplify Algorithms and Codes perhaps dramatically Spatial Dependence is Already Known Only have to average the time dependence Ma, Li and Liu (2016). arXiv:1605.04886; Ma, Li and Liu (2016). arXiv:1606.03625. Differential equation in ๐’™ is not needed for ๐‰๐’•๐’๐’•๐’‚๐’ ๐‰๐’•๐’๐’•๐’‚๐’ = ๐‰ + ๐›†๐ŸŽ ๐๐‘ฌ ๐๐’• April 11, 2021 Current flow is very smooth in spatial coordinate
  • 58. 58 What does this mean for theory and simulations? Opportunity to Simplify Algorithms and Codes perhaps dramatically Spatial Dependence is Already Known Only have to average the time dependence Ma, Li and Liu (2016). arXiv:1605.04886; Ma, Li and Liu (2016). arXiv:1606.03625. Current flow is very smooth in spatial coordinate Differential equation in ๐’™ is not needed for ๐‰๐’•๐’๐’•๐’‚๐’ = ๐‰ + ๐›†๐ŸŽ ๐๐‘ฌ ๐๐’• April 11, 2021
  • 59. ๐‘ก = 0 x t ๐‚๐ฎ๐ซ๐ซ๐ž๐ง๐ญ Time vs Space One Dimensional Systems like Channels or Circuit Components ๐‚๐ฎ๐ซ๐ซ๐ž๐ง๐ญ ๐‘ก = 400 ๐‘ก = 800 Current Noise ๐‰๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ is Zero in Space April 11, 2021 59 Current Noise ๐‰๐’•๐’๐’•๐’‚๐’ is HUGE in time
  • 60. 60 EQUALITY of Total Current ๐‰๐’•๐’๐’•๐’‚๐’ is an Enormous Simplification It can create a It can of Brownian Motion into a April 11, 2021
  • 61. 61 What does this mean for Mathematical Models? The image of total current flow ๐‰๐’•๐’๐’•๐’‚๐’ is very different VERY SMOOTH in space Total Current ๐‰๐’•๐’๐’•๐’‚๐’ does not vary in space so Spatial Derivatives are not needed to describe total current But they are needed to describe everything else. April 11, 2021
  • 62. April 11, 2021 62 Revolution in Biophysics Total Current flow ๐‰๐’•๐’๐’•๐’‚๐’ is equal everywhere in a one dimensional channel Thermal Motion in Space does not appear in equations for flow of total current ๐‰๐’•๐’๐’•๐’‚๐’ in a one dimensional channel Thermal motion appears ONLY in time Eisenberg (2020) Electrodynamics Correlates Knock-on and Knock-off: Current is Spatially Uniform in Ion Channels. Preprint on arXiv at https://arxiv.org/abs/2002.09012.
  • 63. April 11, 2021 63 What does this mean for Ion Channels? Knock On and Knock Off of Ions is IRRELEVANT for the Total Current ๐‰๐’•๐’๐’•๐’‚๐’ Through the Channel Corry (2018) The naked truth about K+ selectivity. Nature Chemistry 10:799-800. Eisenberg (2020) Electrodynamics Correlates Knock-on and Knock-off: Current is Spatially Uniform in Ion Channels. Preprint on arXiv at https://arxiv.org/abs/2002.09012.
  • 64. April 11, 2021 64 View of Channels has been focused on movements of individual ions in channels, But Total Current ๐‰๐’•๐’๐’•๐’‚๐’ is equal everywhere in a one dimensional channel Position does not appear in equations for total current ๐‰๐’•๐’๐’•๐’‚๐’ in a one dimensional channel References and Proofs in Eisenberg (2019) Kirchhoff's Law can be Exact. arXiv: 1905.13574 Eisenberg, Gold, Song, and Huang (2018) What Current Flows Through a Resistor? arXiv:1805.04814
  • 65. April 11, 2021 65 Turn from Biophysics to Electricity and Electronics And then Back to Biology Kirchhoffโ€™s Current Law Should be for TOTAL CURRENT References and Proofs in Eisenberg (2019) Kirchhoff's Law can be Exact. arXiv: 1905.13574 Eisenberg, Gold, Song, and Huang (2018) What Current Flows Through a Resistor? arXiv:1805.04814
  • 66. April 11, 2021 66 It is NOT necessary in our computers to know all the charges! Kirchhoffโ€™s law is (almost) enough Source: textbooks and internet Source: textbooks and internet
  • 67. April 11, 2021 67 Integrated Circuits are Designed with Kirchhoffโ€™s Current Law and little else!!! Hard as that is to believe Source: textbooks and internet
  • 68. Usual Derivation of Kirchhoffโ€™s law is on Long Time Scale โ‰ซ ๐Ÿ๐ŸŽโˆ’๐Ÿ” sec NOT AT ALL at ๐Ÿ๐ŸŽโˆ’๐Ÿ๐ŸŽ sec
  • 69. Usual Derivation of Kirchhoffโ€™s law is about fluxes BUT FLUXES ARE NOT CONSERVED according to experiment or Maxwell equations NOT AT ALL at ๐Ÿ๐ŸŽโˆ’๐Ÿ๐ŸŽ sec
  • 70. April 11, 2021 70 Maxwell div ๐‰๐’•๐’๐’•๐’‚๐’ = ๐ŸŽ and Kirchhoff div ๐‰ โ‰  ๐ŸŽ DISAGREE in usual derivation of Kirchhoff using flux ๐‰ of charges
  • 71. ๐‘น๐‘ช = charging time = ๐Ÿ๐ŸŽโˆ’๐Ÿ๐Ÿ farads ร— ๐Ÿ๐ŸŽ๐Ÿ‘ ohm = ๐Ÿ๐ŸŽโˆ’๐Ÿ— ๐ฌ๐ž๐œ FLUXES ๐‰ ARE NOT CONSERVED I๐ข๐ง ๐‘ฝ๐’๐’–๐’• = ๐‘ฐ๐’Š๐’ ๐Ÿ โˆ’ ๐’†โˆ’๐’• ๐‘น๐‘ช
  • 72. April 11, 2021 72 Kirchhoffโ€™s Laws Describe TOTAL CURRENT ๐‰๐’•๐’๐’•๐’‚๐’ Not flux ๐‰ Valid whenever branched network is valid And Maxwellโ€™s Core Equations are Valid References and Proofs in Eisenberg (2019) Kirchhoff's Law can be Exact. arXiv: 1905.13574 Eisenberg, Gold, Song, and Huang (2018) What Current Flows Through a Resistor? arXiv:1805.04814
  • 73. April 11, 2021 73 Deriving Kirchhoffโ€™s Laws from Maxwell Equations and conservation of current is Trivial if you use Total Current ๐‰๐’•๐’๐’•๐’‚๐’ References and Proofs in Eisenberg (2019) Kirchhoff's Law can be Exact. arXiv: 1905.13574 Eisenberg, Gold, Song, and Huang (2018) What Current Flows Through a Resistor? arXiv:1805.04814
  • 74. April 11, 2021 74 All is obvious to a fine practicing engineer and old friend โ€œBob, why do you need all that math? Everyone knows how to use Kirchhoff. Everyone knows you have to include the displacement current. No one would try to keep track of all the chargesโ€ Paraphrase of email exchange, with permission Alan Finkel Co-designer* of AxoPatch Amplifier Founder Axon Instruments, Recently Chief Scientist Australian Goverment *with Eisenberg, Levis, and Rae
  • 75. April 11, 2021 75 Conservation of Total Current is important in Biology
  • 76. April 11, 2021 76 Conservation of Current is Practically Important in Understanding Transporters Oxidative Phosphorylation Photosynthesis main processes in life
  • 77. Applying Maxwell to Transporters ๐๐ข๐ฏ ๐‰ ๐‘ฅ, ๐‘ก + ๐œ€0 ๐œ•๐„ ๐‘ฅ, ๐‘ก ๐œ•๐‘ก = ๐ŸŽ Sum of Currents in a Transporter = zero in โ€˜small cellโ€™, mitochondrion, HHK, etc. so Currents are Coupled in a Transporter in a โ€˜small cellโ€™ Currents are NOT coupled by Conservation of Current in standard bilayer setup Conservation of Total Current Source internet Liu, Hsieh, and Eisenberg (2016) J Phys Chem B 120:2658-2669
  • 78. Bilayer Setup โ€˜voltage clampโ€™ Inhomogeneous Dirichlet Condition for Classic Voltage Clamp Hodgkin Huxley 1952 Natural Setup: small cell, etc. Homogeneous Neumann Boundary Condition for total current Fig. 10 of Hodgkin Huxley Katz 1952 Na+ Ca++ Na+ Ca++ ๐ผ = ๐ผ๐‘๐‘Ž + ๐ผ๐ถ๐‘Ž = ๐ŸŽ ๐ผ๐‘๐‘Ž = โˆ’๐ผ๐ถ๐‘Ž ๐ผ๐‘๐‘Ž ๐ผ๐ถ๐‘Ž Independent Currents
  • 79. 79 Biophysical Prediction Eisenberg (2020) Electrodynamics Correlates Knock-on and Knock-off: Current is Spatially Uniform in Ion Channels. Preprint on arXiv at https://arxiv.org/abs/2002.09012.
  • 80. Applying Maxwell To Mitochondrion Depends on Conservation of Current Source Internet
  • 81. April 11, 2021 81 Without Conservation of Current Need to Know ALL charges at all times!! Hopeless in large systems where all ions interact with each other! NOTE Chemical Kinetics does not conserve current, in its usual form Does Molecular Dynamics conserve current?
  • 82. April 11, 2021 82 With Conservation of Current no more difficult than large circuit problems
  • 83. April 11, 2021 83 Any Questions?
  • 84. April 11, 2021 84 Extra Slides
  • 85. April 11, 2021 85 Polarization of Matter ฮตr โˆ’ 1 ฮต0 ๐œบ๐’“ involves all movements of matter that do not translate mass, roughly speaking ๐œบ๐’“ โˆ’ ๐Ÿ ๐œบ๐ŸŽ is as complex as the motion of matter itself. Seems hopeless to make a general theory What are the problems with textbook Maxwell Equations? ๐œบ๐’“๐œบ๐ŸŽ is a hybrid
  • 86. ๐๐‘ฌ ๐๐’• creating ๐‘ฉ field in a vacuum is Mysterious
  • 87. Electric & Magnetic Fields takes on the Value that Conserves Current Details and PROOF including quantum mechanics at https://arxiv.org/abs/1609.09175 Specifically, ๐„ & ๐ moves atoms Creates the โ€˜etherealโ€™ current ฮต๐ŸŽ ๐๐„ ๐๐’• So total current ๐‰ + ฮต๐ŸŽ ๐๐„ ๐๐’• is always conserved
  • 88. April 11, 2021 88 Profound Implications of One Dimensional Systems for atomic view of ion channels Spatial Variable does NOT appear in description of current in a one dimensional channel
  • 89. April 11, 2021 89 Spatial Variable does NOT appear in description of current in a one dimensional channel
  • 90. April 11, 2021 90 Hopping Model is COMPLETELY INAPPROPRIATE for current that is uniform in ๐’™
  • 91. April 11, 2021 91 Spatial Variable does appear in description of ion movement in a one dimensional channel
  • 92. April 11, 2021 92 Spatial Variable does NOT appear in description of current in a one dimensional channel
  • 93. April 11, 2021 93 Spatial Variable does NOT appear in description of current in a one dimensional channel We need a Molecular Dynamics that 1) conserves current 2) has one dielectric constant 3) extends to biological time scales
  • 94. April 11, 2021 94 Spatial Variable does NOT appear in description of current in a one dimensional channel Quasi-particle for current CONDUCTON left over is DIFFUSON + POLARON. ๐šบ = PERMION* *Elber, Chen, Rojewska, and Eisenberg. 1995. Sodium in gramicidin: An example of a permion. Biophys. J. 68:906-924.
  • 95. April 11, 2021 95 With Conservation of Current mitochondria are no more difficult than large circuit problems
  • 96. Applying Maxwell to Mitochondria Seems Hopeless Source: textbooks and internet But Stay Tuned for Future Work
  • 97. Applying Maxwell To Mitochondrion Depends on Conservation of Current and depends on collaboration of Oscar Juarez, Chun Liu, and Bob Eisenberg
  • 98. April 11, 2021 98 With Conservation of Current no more difficult than large circuit problems
  • 99. April 11, 2021 99 Spatial Variable does NOT appear in description of current in a one dimensional channel Another way is to include equality of current as a constraint in time averaging schemes e.g., of Ma and Liu Ma, Li, and Liu. 2016.. arXiv:1605.04886. Ma, Li, and Liu. 2016. arXiv:1606.03625.
  • 100. Derivation of Kirchhoffโ€™s Law is at DC Derivation of Kirchhoffโ€™s law is about fluxes How can that work in a computer at ๐Ÿ๐ŸŽโˆ’๐Ÿ๐ŸŽ sec? References and Proofs in Eisenberg (2019) Kirchhoff's Law can be Exact. arXiv: 1905.13574 Eisenberg, Gold, Song, and Huang (2018) What Current Flows Through a Resistor? arXiv:1805.04814
  • 101. April 11, 2021 101 Traditional Form of Maxwell Equations Cannot be Used Maxwellโ€™s equations do not deal with Diffusion Convection Complex materials Complicated dielectric properties Eisenberg, 2019. Dielectric Dilemma. arXxiv: 1901.10805.
  • 102. April 11, 2021 102 It is necessary to update Maxwellโ€™s Equations to see how Kirchhoffโ€™s law & Conservation of Current apply to Complex Liquids and Complex Biological Systems Eisenberg, R. S. 2019. Updating Maxwell with Electrons, Charge, and More Realistic Polarization. arXiv 1904.09695 . Eisenberg, Oriols, and Ferry. 2017. Dynamics of Current, Charge, and Mass. Molecular Based Mathematical Biology 5:78-115 and arXiv preprint 1708.07400.
  • 103. April 11, 2021 103 It is necessary to update Maxwellโ€™s Equations https://arxiv.org/abs/1904.09695 Not just my opinion This is the opinion* of Nobel Prize winners in Physics, Richard Feynman (quantum electrodynamics) and Edward Purcell (nuclear magnetic resonance) *p. 10-7 of Feynman, Leighton, and Sands. 1963. Mainly Electromagnetism and Matter *p. 506 of Purcell and Morin. 2013. Electricity and Magnetism
  • 104. April 11, 2021 104 Maxwellโ€™s equations do not deal with Diffusion Convection Complex materials Complicated dielectric properties Indeed, Maxwellโ€™s original equations do not include ions or electrons or their movement! Textbook treatments do not deal with other forces like diffusion or convection at all. What are the PHYSICAL problems with traditional Maxwell Equations? Eisenberg, 2019. Dielectric Dilemma. arXxiv: 1901.10805.
  • 105. 105 NOT hopeless, Maxwell Predicts Important Biophysics Independent of details of the Mitochondrion if a branched One-dimensional Formulation is appropriate
  • 106. April 11, 2021 106 Inside Channels PROFOUND SIMIPLIFICATION If we can figure out how to exploit it
  • 107. April 11, 2021 107 Profound Implications of One Dimensional Systems for atomic view of ion channels Current is equal everywhere in a channel At all times and under all conditions that the Maxwell Equations Apply
  • 109. April 11, 2021 109 Polarization of Matter ฮตr โˆ’ 1 ฮต0 ๐œบ๐’“ involves all movements of matter that do not translate mass, roughly speaking ๐œบ๐’“ โˆ’ ๐Ÿ ๐œบ๐ŸŽ is as complex as the motion of matter itself. Seems hopeless to make a general theory What are the problems with textbook Maxwell Equations? ๐œบ๐’“๐œบ๐ŸŽ is a hybrid
  • 110. April 11, 2021 110 Continuity of Current is Exact in Kelvinโ€™s Submarine Telegraph ๐’Š๐๐ž๐ฐ๐Ÿ๐จ๐ฎ๐ง๐๐ฅ๐š๐ง๐ = ๐’Š๐ˆ๐ซ๐ž๐ฅ๐š๐ง๐ How can that possibly be true?
  • 111. April 11, 2021 111 It is NOT necessary to know the charges to understand one crucial property of current. Total Current is conserved independent of any property of charge or matter Conservation of Current ๐๐ข๐ฏ ๐‰๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ = 0
  • 112. Applying Maxwell to Transporters 1) Sum of Currents in a Transporter is zero in โ€˜small cellโ€™, mitochondrion, etc. 2) Currents are Coupled in a Transporter in a natural setting by Maxwell 3) Bilayer set up does NOT require currents to sum to zero. Bilayer setup sets voltage across transporter, currents are not controlled. 4) So transporter currents are NOT coupled by Conservation of Current in standard bilayer setup Natural Setting Experimental Setting
  • 113. Polarization of Electron Orbitals April 11, 2021 113 Source Internet