Siméon Denis Poisson: Difference between revisions

From Physics Book
Jump to navigation Jump to search
No edit summary
No edit summary
 
(16 intermediate revisions by the same user not shown)
Line 1: Line 1:
Created by Benjamin Bierbaum
Created by Benjamin Bierbaum


Christian Doppler was an Austrian physicist and mathematician best known for his namesake scientific phenomenon - the Doppler Effect.
Siméon Poisson was a French mathematician best known for his work on definite integrals and electromagnetic theory.
[[File:Simeon Poisson.jpg|thumb|250px|Simeon Poisson]]
[[File:Simeon Poisson.jpg|thumb|250px|Siméon Poisson]]


==The Main Idea==
==Personal Life==


State, in your own words, the main idea for this topic
===Early Life===


Poisson was born in Pithiviers, Loiret, France on June 21, 1781. The son of a soldier, he showed great promise in mathematics and science and started at Paris' École Polytechnique as first in his class. His focus was on mathematics, and at 18 was published in the esteemed journal ''Recueil des savants étrangers'' for his writings on finite difference equations. He was a teaching assistant at the school and later a full professor. During his career he was published over 300 times.
Poisson is most remembered for his work involving the application of mathematics to electricity, magnetism, mechanics, and other areas of physics. He is known for Poisson's equation, which is a partial differential equation that is useful in electrostatics, mechanical engineering and theoretical physics. For example, it can be used to describe the potential energy field caused by a given charge.
===Family Life===
Poisson married Nancy de Bardi in 1817. Together they had four children.
===Death and Legacy===
Poisson's health was weak throughout his lifetime - he had several older siblings that died during childhood, and he was entrusted to a nurse during his early life. His health declined rapidly in 1840, and although extremely impaired, he continued to attend meetings of the French Academy of Sciences.
Poisson died on April 25, 1840. Attendees of his funeral included numerous French scientists, as well as the youngest son of King Louis Philippe I, who studied under Poisson.
Poisson was President of the French Academy of Sciences at the time of his death, and was also a member of the Royal Society of London. His name is inscribed on the Eiffel Tower in Paris alongside 71 other prominent French scientists, mathematicians, and engineers.
==Scientific Contributions==


===A Mathematical Model===
===A Mathematical Model===


What are the mathematical equations that allow us to model this topic.  For example <math>{\frac{d\vec{p}}{dt}}_{system} = \vec{F}_{net}</math> where '''p''' is the momentum of the system and '''F''' is the net force from the surroundings.
Solving the Poisson equation lets one find the electric potential φ for a charge distribution ''<math>\rho_f</math>''. Poisson's equation is:
 
:<math>\Delta\varphi=f</math>


===A Computational Model===
and can also be written as:


How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]
:<math>\nabla^2 \varphi = f.</math>


==Examples==
===Electrostatics===


Be sure to show all steps in your solution and include diagrams whenever possible
Assuming that the magnetic field is not changing with time, Poisson's equation for electrostatics is:


===Simple===
:<math>{\nabla}^2 \varphi = -\frac{\rho_f}{\varepsilon}.</math>
===Middling===
===Difficult===


==Connectedness==
Solving for the potential using Poisson's equation necessitates knowledge of the charge density distribution. If the charge density comes out to be zero, then you get Laplace's equation, another differential equation named after Pierre-Simon Laplace.
#How is this topic connected to something that you are interested in?
#How is it connected to your major?
#Is there an interesting industrial application?


==History==
The potential at a distance ''r'' from a point charge ''Q'' is:
:<math>\varphi(r)  = \dfrac {Q}{4 \pi \varepsilon r}.</math>


Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.
==Connectedness==
Poisson's accomplishments in this field highlight the ability for other schools of thought to assist each other in the collective further understanding of science. Poisson was traditionally a mathematician, but he decided to apply his knowledge to physics and was able to discover a new way of doing things.


== See also ==
== See also ==


Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?
[[Electric Potential]]


===Further reading===
===Further reading===
Line 43: Line 59:


===External links===
===External links===
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]
[https://www.encyclopediaofmath.org/index.php/Poisson_equation]
 
[http://planetmath.org/poissonsequation]


==References==
==References==


#https://upload.wikimedia.org/wikipedia/commons/thumb/b/b7/Simeon_Poisson.jpg/800px-Simeon_Poisson.jpg
#https://upload.wikimedia.org/wikipedia/commons/thumb/b/b7/Simeon_Poisson.jpg/800px-Simeon_Poisson.jpg
#http://eqworld.ipmnet.ru/en/solutions/lpde/lpde302.pdf
#http://www.britannica.com/biography/Simeon-Denis-Poisson
#http://www.encyclopedia.com/topic/Simeon_Denis_Poisson.aspx


[[Category:Which Category did you place this in?]]
[[Category:Notable Scientists]]
[[Category:Notable Scientists]]

Latest revision as of 19:53, 5 December 2015

Created by Benjamin Bierbaum

Siméon Poisson was a French mathematician best known for his work on definite integrals and electromagnetic theory.

Siméon Poisson

Personal Life

Early Life

Poisson was born in Pithiviers, Loiret, France on June 21, 1781. The son of a soldier, he showed great promise in mathematics and science and started at Paris' École Polytechnique as first in his class. His focus was on mathematics, and at 18 was published in the esteemed journal Recueil des savants étrangers for his writings on finite difference equations. He was a teaching assistant at the school and later a full professor. During his career he was published over 300 times.

Poisson is most remembered for his work involving the application of mathematics to electricity, magnetism, mechanics, and other areas of physics. He is known for Poisson's equation, which is a partial differential equation that is useful in electrostatics, mechanical engineering and theoretical physics. For example, it can be used to describe the potential energy field caused by a given charge.

Family Life

Poisson married Nancy de Bardi in 1817. Together they had four children.

Death and Legacy

Poisson's health was weak throughout his lifetime - he had several older siblings that died during childhood, and he was entrusted to a nurse during his early life. His health declined rapidly in 1840, and although extremely impaired, he continued to attend meetings of the French Academy of Sciences.

Poisson died on April 25, 1840. Attendees of his funeral included numerous French scientists, as well as the youngest son of King Louis Philippe I, who studied under Poisson.

Poisson was President of the French Academy of Sciences at the time of his death, and was also a member of the Royal Society of London. His name is inscribed on the Eiffel Tower in Paris alongside 71 other prominent French scientists, mathematicians, and engineers.

Scientific Contributions

A Mathematical Model

Solving the Poisson equation lets one find the electric potential φ for a charge distribution [math]\displaystyle{ \rho_f }[/math]. Poisson's equation is:

[math]\displaystyle{ \Delta\varphi=f }[/math]

and can also be written as:

[math]\displaystyle{ \nabla^2 \varphi = f. }[/math]

Electrostatics

Assuming that the magnetic field is not changing with time, Poisson's equation for electrostatics is:

[math]\displaystyle{ {\nabla}^2 \varphi = -\frac{\rho_f}{\varepsilon}. }[/math]

Solving for the potential using Poisson's equation necessitates knowledge of the charge density distribution. If the charge density comes out to be zero, then you get Laplace's equation, another differential equation named after Pierre-Simon Laplace.

The potential at a distance r from a point charge Q is:

[math]\displaystyle{ \varphi(r) = \dfrac {Q}{4 \pi \varepsilon r}. }[/math]

Connectedness

Poisson's accomplishments in this field highlight the ability for other schools of thought to assist each other in the collective further understanding of science. Poisson was traditionally a mathematician, but he decided to apply his knowledge to physics and was able to discover a new way of doing things.

See also

Electric Potential

Further reading

Books, Articles or other print media on this topic

External links

[1] [2]

References

  1. https://upload.wikimedia.org/wikipedia/commons/thumb/b/b7/Simeon_Poisson.jpg/800px-Simeon_Poisson.jpg
  2. http://eqworld.ipmnet.ru/en/solutions/lpde/lpde302.pdf
  3. http://www.britannica.com/biography/Simeon-Denis-Poisson
  4. http://www.encyclopedia.com/topic/Simeon_Denis_Poisson.aspx