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Hamilton
Mathematician and Romantic
          Luke Drury
Why Hamilton?
 Hamilton is to Irish Science what Joyce is to
Irish literature - the preeminent figure whose
  global reputation transcends his Irishness.

      2005, the bicentenary of his
      birth, was declared to be the
       “Hamilton Year - celebrating
              Irish Science”
Hamilton with
one of his sons
  (circa 1845)
Hamilton presiding as president of the RIA
(from the Dublin University Magazine, June 1842)
Hamilton in middle age
Hamilton at age 54
  (after Graves)
Two stamps issued in 1943 (in the middle
 of the “emergency”!) to commemorate
     the discovery of quaternions.
Rather better in 2005!
Brief chronology
Born 3-4 August 1805 in Dominick Street
Father was Archibald Hamilton, lawyer and
estate agent for the patriot Archibald
Hamilton Rowan.
Mother was Sarah Hutton, from a family of
Dublin coachbuilders.
One Scottish, One French and two Irish
grandparents.
Sent at age 3 to his Uncle James
Hamilton, curate of Trim and master of
the Meath diocesan school housed in
Talbot’s castle (now marked with a
commemorative plaque).

Major educational influence - Uncle
James was a graduate of TCD with a
strong interest in education and
languages who believed in starting as
early as possible with a very broadly
based education and lots of hard work.
The myth of 13 languages by 13

WRH certainly was remarkably fluent in
Latin, Greek and Hebrew from a very
early age.

 He appears to have had a basic
 knowledge of Persian, Arabic, Syriac and
 some Sanskrit

 Impressive, but hardly 13. (NB no Irish!)

 In later life could read, but not speak,
 French, German and probably Italian.
Remarkably, little evidence of early
mathematical abilities!
Dec 14, 1815 to his sister Grace.

I have for some time been reading Lucian and Terence, the Hebrew
psalter on Sundays and on Saturdays some Sanskrit, Arabic and Persian.
I read at leisure hours Goldsmith’s Animated Nature and any new
history or poetry than falls my way. I like Walter Scott very much. In
arithmetic I have got as far as practice and I have done very near half
the first book of Euclid with my uncle.
I do the ancient and modern geography of the different countries
together. I do the second lesson every morning in the Greek
Testament and, on Sundays after church go over the scripture lessons
of the past week with Dodderidge’s Notes and Improvements, and
before church I read Secker on the Catechism, and in the evenings
Wells’ Scripture Geography, a very entertaining book.

       Extract from earliest surviving letter of WHR
Mother dies in 1817 (when he is 12).

Father dies in 1819

Meets Zerah Colburn, 1818 and 1820.

Develops increasing interest in
mathematics

1823 - comes first in TCD entrance
examination with special prize in Hebrew.
Wins virtually all prizes in TCD

Aug 17th 1824, meets Catherine Disney

May 5th 1825, Catherine is married to Rev
Barlow

April 27 1827, submits paper on Systems of
Rays to PRIA

June 16th 1827, appointed to Dunsink

Sep 15th 1827, first meeting with Wordsworth
Aug 1829, Wordsworth visits Dunsink

March 1832, visits Coleridge in London

22 Oct 1832 Predicts conical refraction

April 9 1833, marries Helen Bayly

April 10 1834, submits paper on General
Methods in Dynamics
June 1 1835, presents ideas on Algebra as
Science of Pure Time

Aug 15 1835, knighted at BAAS meeting

Dec 1837, elected president of RIA

1840 Helen leaves for two years

Oct 16 1843, discovers quaternions
Feb 11 1846, incapacitated at meeting of
the Geological Society - abstains for two
years.

Oct 1853, Catherine Disney/Barlow dies

Jan 9 1865, elected first foreign associate
of the NAS

Sep 2 1865, dies at Dunsink
Hamilton’s Optics
First part of system of rays deals with
rays reflected from arbitrary mirrors.
Extended to arbitrary refracting media in
part two.
Finally to anisotropic crystalline media in
third supplement.
Based on Fermat’s principle of least time
The actual path followed by light travelling from
 X to X’ via a reflection from the mirror surface
is the shortest such path, and thus the light travels
         from X to X’ in the shortest time.
Similarly for refraction - can show that
light takes path of shortest time
between two points if speed in media is
inversely proportional to the “index of
refraction” n.
                Z
            δ       n ds = 0
How lens works - light travels more slowly in glass
  than air so all light paths take the same time.
Hamilton then introduces his
“Characteristic function” V(x’,x) of a
general optical system as essentially
this minimum (more precisely
stationary) time for light to travel
from x’ to x through the system. All
the properties of the system are
contained in this one function!
                      Z x
       V (x , x) =
             0
                            nds
                       x0
The really important difference in
Hamilton’s approach is that he allows both
end points to vary as well. For isotropic
media this gives the “eikonal equations”
     ✓        ◆2    ✓      ◆2    ✓      ◆2
         ∂V          ∂V           ∂V
                   +            +            =n   2
         ∂x          ∂y           ∂z

    ✓         ◆2    ✓      ◆2    ✓      ◆2
        ∂V           ∂V           ∂V
                   +            +            =n   02
        ∂x0          ∂y0          ∂z0
For general anisotropic media the
refractive index depends on the direction
of propagation as well as position,

                              d xi
  n = n(xi, αi),         αi =
                              ds
But the direction cosines of the ray
are not independent quantities...

             αiα = 1
                  i
Hamilton however extends the refractive
 index to a homogeneous function of first
 order in the direction cosines treated as
 independent quantities. Then by Euler’s
 identity,

                      ∂n
               n = αi
                      ∂αi
(Easiest way to think of this is to take a
function defined on the unit sphere and
then scale it proportional to the radius for
points off the unit sphere)
Z       Z           Z
δ       n ds=   δn ds + n δds
            Z   ✓                   ◆      Z
                  ∂n        ∂n                   ∂n
           =          δxi +     δαi ds + αi         δds
                  ∂xi       ∂αi                 ∂αi
            Z                Z
                ∂n               ∂n
           =        δxi ds +        (δαi ds + αi δds)
            Z   ∂xi          Z  ∂αi
                ∂n               ∂n
           =        δxi ds +        δdxi
            Z
                ∂xi            ∂α
                               ✓ i◆                   x
                      ∂n d ∂n                  ∂n
           =    δxi                     ds +       δxi
                      ∂xi ds ∂αi               ∂αi     x0
This gives Hamilton’s starting point for
his geometrical optics of arbitrary
media;
           ✓      ◆
         d ∂n         ∂n
                          =0
         ds ∂αi       ∂xi

gives the equation of the ray, and the
variation of the characteristic function
when the end points move is given by
         ∂V   ∂n      ∂V       ∂n
            =    ,      0=
         ∂xi ∂αi      ∂xi      ∂α0i
Mechanics also can be expressed as
the principle of “least action”
                Z
            S=      Ldt
          δS=0
Thus Hamilton’s ideas carry over to
general mechanics. The equivalent
of the “eikonal” equation is the
Hamilton-Jacobi equation.
How (or why) can nature follow the path
of stationary action?? The only way to
know that the action is stationary is to
explore all the paths from an inital to a
final state.

This is precisely what happens in
quantum mechanics!
                           Z         2
         P(A ! B) =            eiS
QM removes the “unphysical” suspicion of
teleology from the principle of least
action (originally introduced on
theological grounds in 18th century!) but
at the expense of the `spookiness’ so
detested by Einstein and Schroedinger!
Perhaps not inappropriate for
Halloween....
Herr Nietsche said
"God is dead!"
Herr Drury said "that's crazy,
my reflection
on 'Least Action'
tells me He's just lazy!"

  (Iggy McGovern, personal communication, 2005)
Hamilton’s focus on the mathematical
structure of systems defined by
variational principles has remained at the
heart of theoretical physics since his day
and is still there! However precisely
because it is so fundamental and
universal it is not easy to convey to
nonspecialists just why it is so important.
Other major contribution was the
discovery of quaternions.

Hamilton “demystified” imaginary (or
complex) numbers by regarding them as
pairs of real numbers with appropriate
rules for addition, multiplication etc.


(a, b) + (c, d)=(a + c, b + d)
(a, b) ⇥ (c, d)=(ac bd, ad + bc)
Obvious question is can one extend this
idea to triples of real numbers?

Surprisingly no, but as Hamilton suddenly
realised it will work if one goes from
three to four real numbers! Hence the
quaternions.

But - multiplication is noncommutative!

               ab 6= ba
A general quaternion has the form

       a + bi + c j + dk
with a scalar part a and vector part
(b,c,d). Every nonzero element has an
inverse
      a bi c j dk
      a 2 + b2 + c2 + d 2
Important mainly for introducing the idea
of non-commutative multiplication
(another key idea in quantum mechanics!)

Never achieved the importance Hamilton
thought they would, but beautiful and
useful.

(Only four division algebras exist- the
reals, the complex numbers, quaternions
and octonions)
Hamilton also made important
contributions to graph theory
(Hamiltonian circuits), the theory of
fourier series and to Abel’s proof that
the general quintic was not soluble in
radicals.
His lasting fame however relies on his
fundamental formulation of optics and
mechanics into what is now called
canonical or Hamiltonian form, a form so
fundamental that it has survived the
transition from classical to quantum
mechanics!
Hamilton the romantic.

Highly idealistic he was a deep admirer
of the romantic poets and considered
poetry to be much superior to prose.

Also in his doomed and unhappy love for
Catherine he displayed a typically
romantic streak to his nature.

Was introduced to German idealism by
Coleridge - Kant was a major influence.
One reason his works are so hard to read
is that he sought to write a form of
mathematical poetry whereby the
maximum meaning is conveyed with the
minimum content - distilling out the
essence of each problem and presenting
it in the most general and abstract form.
But of course this is also why his
contributions are so fundamental.
Surely a lesson for us today - long term
impact comes from a focus on deep
problems and underlying structures, not
on immediate applications. Also we need
to see science as part of culture and as
a creative activity closely allied to the
creative arts.
Less Science and Technology, more
Science and Culture!

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Hamilton: Mathematician and Romantic - Prof. Luke Drury, President of Royal Irish Academy

  • 2. Why Hamilton? Hamilton is to Irish Science what Joyce is to Irish literature - the preeminent figure whose global reputation transcends his Irishness. 2005, the bicentenary of his birth, was declared to be the “Hamilton Year - celebrating Irish Science”
  • 3. Hamilton with one of his sons (circa 1845)
  • 4. Hamilton presiding as president of the RIA (from the Dublin University Magazine, June 1842)
  • 6. Hamilton at age 54 (after Graves)
  • 7. Two stamps issued in 1943 (in the middle of the “emergency”!) to commemorate the discovery of quaternions.
  • 9. Brief chronology Born 3-4 August 1805 in Dominick Street Father was Archibald Hamilton, lawyer and estate agent for the patriot Archibald Hamilton Rowan. Mother was Sarah Hutton, from a family of Dublin coachbuilders. One Scottish, One French and two Irish grandparents.
  • 10. Sent at age 3 to his Uncle James Hamilton, curate of Trim and master of the Meath diocesan school housed in Talbot’s castle (now marked with a commemorative plaque). Major educational influence - Uncle James was a graduate of TCD with a strong interest in education and languages who believed in starting as early as possible with a very broadly based education and lots of hard work.
  • 11.
  • 12. The myth of 13 languages by 13 WRH certainly was remarkably fluent in Latin, Greek and Hebrew from a very early age. He appears to have had a basic knowledge of Persian, Arabic, Syriac and some Sanskrit Impressive, but hardly 13. (NB no Irish!) In later life could read, but not speak, French, German and probably Italian.
  • 13. Remarkably, little evidence of early mathematical abilities! Dec 14, 1815 to his sister Grace. I have for some time been reading Lucian and Terence, the Hebrew psalter on Sundays and on Saturdays some Sanskrit, Arabic and Persian. I read at leisure hours Goldsmith’s Animated Nature and any new history or poetry than falls my way. I like Walter Scott very much. In arithmetic I have got as far as practice and I have done very near half the first book of Euclid with my uncle. I do the ancient and modern geography of the different countries together. I do the second lesson every morning in the Greek Testament and, on Sundays after church go over the scripture lessons of the past week with Dodderidge’s Notes and Improvements, and before church I read Secker on the Catechism, and in the evenings Wells’ Scripture Geography, a very entertaining book. Extract from earliest surviving letter of WHR
  • 14. Mother dies in 1817 (when he is 12). Father dies in 1819 Meets Zerah Colburn, 1818 and 1820. Develops increasing interest in mathematics 1823 - comes first in TCD entrance examination with special prize in Hebrew.
  • 15. Wins virtually all prizes in TCD Aug 17th 1824, meets Catherine Disney May 5th 1825, Catherine is married to Rev Barlow April 27 1827, submits paper on Systems of Rays to PRIA June 16th 1827, appointed to Dunsink Sep 15th 1827, first meeting with Wordsworth
  • 16.
  • 17. Aug 1829, Wordsworth visits Dunsink March 1832, visits Coleridge in London 22 Oct 1832 Predicts conical refraction April 9 1833, marries Helen Bayly April 10 1834, submits paper on General Methods in Dynamics
  • 18. June 1 1835, presents ideas on Algebra as Science of Pure Time Aug 15 1835, knighted at BAAS meeting Dec 1837, elected president of RIA 1840 Helen leaves for two years Oct 16 1843, discovers quaternions
  • 19. Feb 11 1846, incapacitated at meeting of the Geological Society - abstains for two years. Oct 1853, Catherine Disney/Barlow dies Jan 9 1865, elected first foreign associate of the NAS Sep 2 1865, dies at Dunsink
  • 20. Hamilton’s Optics First part of system of rays deals with rays reflected from arbitrary mirrors. Extended to arbitrary refracting media in part two. Finally to anisotropic crystalline media in third supplement. Based on Fermat’s principle of least time
  • 21. The actual path followed by light travelling from X to X’ via a reflection from the mirror surface is the shortest such path, and thus the light travels from X to X’ in the shortest time.
  • 22. Similarly for refraction - can show that light takes path of shortest time between two points if speed in media is inversely proportional to the “index of refraction” n. Z δ n ds = 0
  • 23. How lens works - light travels more slowly in glass than air so all light paths take the same time.
  • 24. Hamilton then introduces his “Characteristic function” V(x’,x) of a general optical system as essentially this minimum (more precisely stationary) time for light to travel from x’ to x through the system. All the properties of the system are contained in this one function! Z x V (x , x) = 0 nds x0
  • 25. The really important difference in Hamilton’s approach is that he allows both end points to vary as well. For isotropic media this gives the “eikonal equations” ✓ ◆2 ✓ ◆2 ✓ ◆2 ∂V ∂V ∂V + + =n 2 ∂x ∂y ∂z ✓ ◆2 ✓ ◆2 ✓ ◆2 ∂V ∂V ∂V + + =n 02 ∂x0 ∂y0 ∂z0
  • 26. For general anisotropic media the refractive index depends on the direction of propagation as well as position, d xi n = n(xi, αi), αi = ds But the direction cosines of the ray are not independent quantities... αiα = 1 i
  • 27. Hamilton however extends the refractive index to a homogeneous function of first order in the direction cosines treated as independent quantities. Then by Euler’s identity, ∂n n = αi ∂αi (Easiest way to think of this is to take a function defined on the unit sphere and then scale it proportional to the radius for points off the unit sphere)
  • 28. Z Z Z δ n ds= δn ds + n δds Z ✓ ◆ Z ∂n ∂n ∂n = δxi + δαi ds + αi δds ∂xi ∂αi ∂αi Z Z ∂n ∂n = δxi ds + (δαi ds + αi δds) Z ∂xi Z ∂αi ∂n ∂n = δxi ds + δdxi Z ∂xi  ∂α ✓ i◆  x ∂n d ∂n ∂n = δxi ds + δxi ∂xi ds ∂αi ∂αi x0
  • 29. This gives Hamilton’s starting point for his geometrical optics of arbitrary media; ✓ ◆ d ∂n ∂n =0 ds ∂αi ∂xi gives the equation of the ray, and the variation of the characteristic function when the end points move is given by ∂V ∂n ∂V ∂n = , 0= ∂xi ∂αi ∂xi ∂α0i
  • 30. Mechanics also can be expressed as the principle of “least action” Z S= Ldt δS=0 Thus Hamilton’s ideas carry over to general mechanics. The equivalent of the “eikonal” equation is the Hamilton-Jacobi equation.
  • 31. How (or why) can nature follow the path of stationary action?? The only way to know that the action is stationary is to explore all the paths from an inital to a final state. This is precisely what happens in quantum mechanics! Z 2 P(A ! B) = eiS
  • 32. QM removes the “unphysical” suspicion of teleology from the principle of least action (originally introduced on theological grounds in 18th century!) but at the expense of the `spookiness’ so detested by Einstein and Schroedinger! Perhaps not inappropriate for Halloween....
  • 33. Herr Nietsche said "God is dead!" Herr Drury said "that's crazy, my reflection on 'Least Action' tells me He's just lazy!" (Iggy McGovern, personal communication, 2005)
  • 34. Hamilton’s focus on the mathematical structure of systems defined by variational principles has remained at the heart of theoretical physics since his day and is still there! However precisely because it is so fundamental and universal it is not easy to convey to nonspecialists just why it is so important.
  • 35. Other major contribution was the discovery of quaternions. Hamilton “demystified” imaginary (or complex) numbers by regarding them as pairs of real numbers with appropriate rules for addition, multiplication etc. (a, b) + (c, d)=(a + c, b + d) (a, b) ⇥ (c, d)=(ac bd, ad + bc)
  • 36. Obvious question is can one extend this idea to triples of real numbers? Surprisingly no, but as Hamilton suddenly realised it will work if one goes from three to four real numbers! Hence the quaternions. But - multiplication is noncommutative! ab 6= ba
  • 37. A general quaternion has the form a + bi + c j + dk with a scalar part a and vector part (b,c,d). Every nonzero element has an inverse a bi c j dk a 2 + b2 + c2 + d 2
  • 38. Important mainly for introducing the idea of non-commutative multiplication (another key idea in quantum mechanics!) Never achieved the importance Hamilton thought they would, but beautiful and useful. (Only four division algebras exist- the reals, the complex numbers, quaternions and octonions)
  • 39. Hamilton also made important contributions to graph theory (Hamiltonian circuits), the theory of fourier series and to Abel’s proof that the general quintic was not soluble in radicals.
  • 40. His lasting fame however relies on his fundamental formulation of optics and mechanics into what is now called canonical or Hamiltonian form, a form so fundamental that it has survived the transition from classical to quantum mechanics!
  • 41.
  • 42. Hamilton the romantic. Highly idealistic he was a deep admirer of the romantic poets and considered poetry to be much superior to prose. Also in his doomed and unhappy love for Catherine he displayed a typically romantic streak to his nature. Was introduced to German idealism by Coleridge - Kant was a major influence.
  • 43. One reason his works are so hard to read is that he sought to write a form of mathematical poetry whereby the maximum meaning is conveyed with the minimum content - distilling out the essence of each problem and presenting it in the most general and abstract form. But of course this is also why his contributions are so fundamental.
  • 44. Surely a lesson for us today - long term impact comes from a focus on deep problems and underlying structures, not on immediate applications. Also we need to see science as part of culture and as a creative activity closely allied to the creative arts.
  • 45. Less Science and Technology, more Science and Culture!