Scientific Technical Review,Vol.LVII,No.3-4,2007
3
UDK: 512.514. 53:929
COSATI: 12-02
Leonhard Euler (1707-1783)
and Rigid Body Dynamics
Edited by Katica (Stevanovi
Ä
) Hedrih, PhD (Eng)
1)
The introductory test of this volume is dedicated to the 300th anniversary of the birth of Leonhard Euler, one of the
most distinguished scientists of the 18th century in the fields of mathematics and mechanics. Born on 15 April 1707 in
Basel, Switzerland, he devoted his life to mathematics instead to theology, much against his father wish and owing to
famous Bernoulli. Although the majority of his work concerned elementary mathematics, he also contributed
significantly to astronomy and physics.
Partially blind in his late twenties and totally blind in his late years, Euler was nonetheless exceptionally productive in
his studies â 500 titles appeared during his lifetime and 400 more were published after his death. Laplace used to tell
his students: âRead Euler, read Euler! He is the teacher of us all!â
1)
Faculty of Mechanical Engineering University of NiĆĄ, Mathematical Institute SANU, Aleksandra Medvedeva 14, 18000 Nis, SERBIA
Introduction
statement attributed to Pierre-Simon Laplace
expresses Euler's influence on mathematics: "
Read
Euler, read Euler, he is the teacher (master) of us all
".
The Euler Committee of the Swiss Academy of Sciences
was founded in 1907 with the task to publish all scientific
books, papers and the correspondence of Leonhard Euler
(1707-1783) in a scientific edition.
Euler was one of the leading and most famous scien-
tists in the mathematics as well as in the mechanics of
the 18th century.
Euler's books and papers are edited in the Series I-III, the
correspondence in the Series IV. In the last 90 years 71
volumes of the Series I-III have been published. The last
three volumes are in preparation and should appear shortly.
The Series IV with Euler's scientific correspondence will
contain 10 volumes. Four volumes have been published and
three volumes are in preparation.
Fugure 1.
Aleksandr Mikhailovich Lyapunov (1857 â 1918) Editor of two
volumes of
Eulerâs collected works
.
This huge endeavor can only succeed with the aid of
internationally acclaimed scientists as coworkers and with
the financial support of the Swiss National Science
Foundation, the Swiss Academy of Sciences and many
long-term substantial contributions from Swiss industrial
corporations.
A. M. Lyapunov opened a new page in the history of
global science. He also contributed as an editor of two
volumes of
Euler's collected works
. He took part in the
publication of Euler's Selected Works and was the editor of
the 18th and 19th part of this miscellany.
The âEuler phenomenonâ
Three factors go a long way towards explaining the
âEuler phenomenonâ: First of all, his - perhaps unique -
gifted memory. He seemed to have remembered whatever
he had heard, seen, thought, or written in his whole life, as
countless contemporaries confirmed. For example, in his
advanced age he was able to delight his relatives, friends,
and acquaintances with a literal (Latin) recitation of any
song from Virgilâs Aeneis, and he could reproduce by heart
the minutes of the academy meetings decades later, not
mentioning his memory concerning mathematics.
Furthermore, Eulerâs prodigious memory went hand in
hand with a rare ability to concentrate. Noise and bustle in
his immediate environment hardly disturbed his thinking:
âA child on his knees, a cat on his back - this is how he
wrote his immortal works,â reported ThiĂ©bault, his
colleague from the Berlin academy. The third factor in the
âEuler mysteryâ is, quite simply, constant, meticulous
work.
Reputation
Leonhard Eulerâs influence and reputation were already
impressive during his lifetime. For almost two decades he
was (according to Andreas Speiser) the intellectual leader
of the Protestant part of Germany, and (according to Eduard
Winter) he performed inestimable services as the âgolden
bridge between two academiesâ. The 10 volumes of his
correspondence testify to this role, as does the fact that,
during his Berlin years, Euler published 109 papers in the
A
4
K.S.HEDRIH: LEONHARD EULER (1707-1783) AND RIGID BODY DYNAMICS
Petersburger Kommentare and 119 papers in the MĂ©moires
of the Berlin academy. And although Eulerâs energy was
sufficient for him to keep up his activities at both
institutions, the institutions themselves could not easily
cope with the almost inexhaustible tide of Eulerâs
productivity. To judge simply from the extent of his work,
Euler is in the company of the most prolific members of the
human race, e.g, Voltaire, Leibniz, Telemann or Goethe.
The directory of Eulerâs writings published by G. Eneström
(1910-1913) takes up an entire volume and contains almost
900 titles, some 40 books among them.
Productivity
The following table summarizes the extent of Eulerâs
writings specified by him as ready for publication, arranged
according to decades (not included are a few dozen works
that have not yet been dated):
Year Works
%
1725â1734
35
5
1735â1744
50
10
1745â1754
150
19
1755â1764
110
14
1765â1774
145
18
1775â1783
270
34
Specific disciplines
With respect to specific disciplines, the writings are
classified approximately as follows:
â
Algebra, number theory, analysis
40%
â
Mechanics and other physics
8%
â
Geometry, including trigonometry
18%
â
Astronomy
11%
â
Ship theory, artillery, architecture
2%
â
Philosophy, music theory, theology,
and anything else not included above
1%
The classification of Eulerâs purely mathematical works is
approximately as follows:
â
Algebra, combination and probability theory 10%
â
Number
theory
13%
â
Fundamental analysis and differential calculus 7%
â
Infinite
series
13%
â
Integral
calculus
20%
â
Differential
equations
13%
â
Calculus
of
variations
7%
â
Geometry, including differential geometry
17%
Awards
Leonhard Euler won 12 international academy prizes,
not counting the prizes of his sons Johann Albrecht (7) and
Karl (1), which can essentially also be credited to Eulerâs
account. The French King Louis XVI awarded Euler 1000
rubles for his âsecond ship theoryâ, and the Russian
empress Catherine II gave him double that amount so that
the blind doyen of Petersburg could receive a
supplementary salary in 1773.
Influence
As far as Euler is concerned, the opinions of the most
important mathematicians are unanimous. Laplace used to
say to his students: âRead Euler, read Euler! He is the
master of us all!â and Gauss explained emphatically: âThe
study of Eulerâs works remains the best instruction in the
various areas of mathematics and can be replaced by no
other.â Indeed, through his books, which are consistently
characterized by the highest striving for clarity and
simplicity and which represent the first actual textbooks in
a modern sense, Euler became the premier teacher of
Europe not only of his time but well into the 19
th
century.
Formation and Training
1707 Born on 15 April in Basel, the son of the Protestant
minister Paul Euler and Margaretha Brucker.
Leonhard Eulerâs father was Paul Euler who studied
theology at the University of Basel and attended Jacob
Bernoulliâs lectures there. In fact Paul Euler and Johann
Bernoulli both lived in Jacob Bernoulliâs house while they
were undergraduates at Basel. Leonhard Euler was born in
Basel, but the family moved to Riehen when he was one
year old and it was in Riehen, not far from Basel, that
Leonard was brought up. Paul Euler had some
mathematical training and he was able to teach his son
elementary mathematics along with other subjects.
Eulerâs father wanted his son to follow him into the
church and sent him to the University of Basel to prepare
for the ministry. He entered the University in 1720, at the
age of 14, first to obtain a general education before going
on to more advanced studies. Johann Bernoulli soon
discovered Eulerâs great potential for mathematics in
private tuition that Euler himself engineered.
In 1720 Leonhard entered Basel University, which was
founded in 1460. Initially he studied theology, Oriental
languages and history, but soon switched to mathematics under
Johann Bernoulli (1667-1748), who became the world's most
cited mathematician following the death of Isaac Newton
(1643-1727). Quick to recognize Euler's mathematical genius,
Bernoulli challenged him by having him read the works of the
masters, and especially by instructing him personally in
contemporary mathematical research.
In 1723 Euler completed his Masterâs degree in
philosophy having compared and contrasted the
philosophical ideas of Descartes and Newton. He began his
study of theology in the autumn of 1723, following his
fatherâs wishes, but, although he was to be a devout
Christian all his life, he could not find the enthusiasm for
the study of theology, Greek and Hebrew that he found in
mathematics. Euler obtained his fatherâs consent to change
to mathematics after Johann Bernoulli had used his
persuasion. The fact that Eulerâs father had been a friend of
Johann Bernoulliâs in their undergraduate days undoubtedly
made the task of persuasion much easier.
Nicolaus Bernoulli
(1623-1708)
Jakob Bernoulli
(1654â1705)
Nicolaus I Bernoulli
(1687-1759)
Nicolaus Bernoulli
(1662â1716)
Johann Bernoulli
(1667â1748)
Nicolaus II Bernoulli
(1695â1726)
Johann III Bernoulli
(1744â1807)
Daniel Bernoulli (1700â
1782)
Johann II Bernoulli
(1710â1790)
Nicolaus Bernoulli
(1623-1708)
Daniel II Bernoulli
(1751â1834)
Figure 2.
Family tree of the Bernoulli family
Euler completed his studies at the University of Basel in
1726. He studied many mathematical works during his time
in Basel, and Calinger reconstructed many of the works that
Euler read following the advice of Johann Bernoulli. They
include works by Varignon, Descartes, Newton, Galileo,
van Schooten, Jacob Bernoulli, Hermann, Taylor and
Wallis. By 1726 Euler had already a paper in print, a short
article on isochronous curves in a resisting medium. In
K.S.HEDRIH: LEONHARD EULER (1707-1783) AND RIGID BODY DYNAMICS
5
1727 he published another article on reciprocal trajectories
and submitted an entry for the 1727 Grand Prize of the
Paris Academy on the best arrangement of masts on a ship.
In 1727, Catherine I of Russia invited Euler to join the
faculty of the Academy of Sciences in St. Petersburg. He
became chairman of mathematics there in 1733, replacing
Daniel Bernoulli. In 1735, he lost sight in one eye while
working around the clock for three days to solve a
mathematic problem that took other mathematicians months
to solve. While in Russia, he prepared some 90 papers for
publication and wrote the two-volume book Mechanics. He
collaborated with Daniel Bernoulli in the field of fluid
mechanics and derived the equation that related velocity
and pressure, which became known as Bernoulli's equation.
He also conceived of pressure as something that could
change from point to point throughout a fluid.
Figure 3.
Methodus inveniendi - Leonhard Euler
The cover page of Euler's Methodus inveniendi lineas curvas.
In 1741, at the urging of Frederick the Great, Euler
moved to Berlin and became professor of mathematics at
the Berlin Academy of Sciences, which he turned into a
major academy. Over the next 25 years, Euler prepared at
least 380 papers for publication. After his relationship with
Frederick deteriorated, he accepted the invitation from
Catherine the Great to return to St. Petersburg in 1766
where he became director of the Academy of Sciences.
Soon after his return, he became almost totally blind.
Nevertheless, he excelled at solving complex calculations
in his head. While in St. Petersburg, he worked on
developing a better theory of lunar motion that involved the
interactions of the Sun, Moon, and Earth.
Euler contributed to the subjects of geometry, calculus,
trigonometry, and number theory. He standardized
mathematical notation using Greek symbols that continue to
be used today. He also contributed to the fields of
astronomy, mechanics, optics, and acoustics, and made a
major contribution to theoretical aerodynamics. He derived
the continuity equation and the equations for the motion of
an in viscid, incompressible fluid.
Euler suffered a stroke and died on September 18, 1783
in St. Petersburg.
First Petersburg period
1727 Euler's thesis entitled De Sono (On Acoustics)
formed the basis for his application for a post as professor
of physics in Basel, but he was passed over on account of
his youth. Through the help of the Bernoullis, he was
offered a position in St. Petersburg at the Academy of
Science, founded by Peter the Great in 1725. There he
worked first as an assistant professor, then from 1730 as a
professor and member of the academy (he had no teaching
commitments, though he did write a textbook on
elementary mathematics). The principal contributions of
this early Petersburg period include a two-volume work on
mechanics, a book on music theory and Scientia navalis
(about hydrodynamics, shipbuilding and navigation), which
was eventually published in 1749.
1734 At the beginning of January, Euler married
Katharina Gsell, a daughter of a Swiss painter George
Gsell, who was working in St. Petersburg. Euler's son
Johann Albrecht was born at the end of November, the only
one of his offspring to follow in his footsteps as a
mathematician and member of the Academy. Only three of
Euler's thirteen children would survive him. He had twenty-
one grandchildren.
1738 As a result of a severe abscess, Euler lost the sight
of his right eye.
Berlin years
1741 Conscious of the political turmoil in the Russian
empire, Euler accepted Frederick II's offer of a
professorship at a newly established Prussian Academy
("Berlin Academy") and settled with his family in Berlin.
There he held a position as director of the mathematics
department. Maupertuis, who in 1736 made a name for
himself in a famous expedition to Lapland (the purpose of
which was to determine whether the Earth was indeed an
oblate spheroid) became president of the Academy, though
as a scientist, he ranked far below Euler.
In addition to hundreds of treatises written during the
Berlin period, Euler produced major works on the calculus
of variations, the theory of special functions, differential
equations, astronomy as well as a second masterpiece on
mechanics and a popular work on physics and philosophy
titled Lettres Ă une princesse d'Allemagne. The basic
outline of his celebrated work on algebra also dates from
the Berlin period. During this time, Euler maintained active
connections with the Petersburg Academy, and he helped to
promote interactions between the two internationally
renowned academies. Euler was a member of all the
important academies of his time and received many awards.
Second Petersburg period
1766 Frederick II's bumbling was influential in Euler's
accepting an offer from Catherine the Great to return to St.
Petersburg, where he remained until his death.
1771 In the aftermath of a failed cataract operation,
Euler lost the sight of his remaining good eye and soon
became nearly completely blind. During the great St.
Petersburg fire, he was saved from his burning house at the
last moment by the Basler artisan Peter Grimm. Yet,
amazingly, his productivity increased: approximately half
of his prodigious output occurred during this second
Petersburg period, including three-volume works on
6
K.S.HEDRIH: LEONHARD EULER (1707-1783) AND RIGID BODY DYNAMICS
integral calculus and optics (Institutiones calculi integralis
and Dioptrica) as well as the authoritative version of his
work on algebra.
1773 Following the death of his wife Katherina, in 1776
Euler married her half-sister Abigail Gsell.
1783 On 18 September Euler suffered a stroke and died
quickly and painlessly.
Euler's contributions to mathematics cover a wide range,
including analysis and the theory of numbers. He also
investigated many topics in geometry.
Rigid body Kinematics
Euler's contributions to mathematics cover a wide range,
including analysis and the theory of numbers. He also
investigated many topics in geometry with application to the
.kinematics. Euler equations in the area of rigid body
kinematics - rotation about a fixed point - are very important
and applicable in future development in dynamics.
Figure 4.
Sphere geometry of rotation
Figure 5.
Kinematics of the rigid body rotation around a fixed point- Eulerâs
angles:
Ï
angle of precession,
Ï
angle of nutation
Ï
angle of 8 self rotation)
New Vector to Rigid body rotation around a fixed point and
instantaneous axis through a fixed point
Let us consider the special case of rotation around the
fixed point
O
and around the moving axis oriented by the
unit vector
n
r
with the rotation around the fixed point
O
using Eulerâs angles: angles
Ï
of precession , angle
Ï
of
nutation an angle
Ï
of self rotation as well as the mass
moment vectors conected by the fixed point
O
and the
rotating axis, also around the fixed point.
Using Eulerâs angles
(
)
, ,
Ï Ï Ï
, the Euler angular
velocities are defined as follows:
Ï
&
- anglular velocity of
precession, is defined by
k
Ï
Ï
Ï
=
r
r
&
in the direction of
k
r
,
Ξ
&
- angular velocity of nutation is defined by
e
Ï
Ï
Ï
=
r
r
&
in the
direction of
e
r
(knot axis) and
Ï
&
-angular velocity of self
rotation is defined by
k
Ï
Ï
Ï âČ
=
r
r
&
in the direction of
k
âČ
r
(axis
of body self rotation). Overall instantaneous angular
velocity of the body rotation around the fixed point is:
( )
[ ]
[
]
dm
r
n
r
J
d
n
O
r
r
r
r
r
,
,
=
[ ]
[
]
( )
n
O
O
J
d
dm
r
r
L
d
r
r
r
r
r
r
Ï
Ï
=
=
,
,
R
r
r
n
r
[ ]
[
]
r
r
dm
dm
S
O
r
r
r
r
,
,
2
Ï
=
On
dJ
( )
n
O
D
d
r
r
O
( )
dm
v
t
p
d
r
r
=
[ ]
r
v
r
r
r
,
Ï
=
dm
( )
r
N
r
A
AN
F
r
An
F
r
F
r
P
r
r
P
G
C
r
r
C
L
n
r
r
Ï
Ï
=
Figure 6.
Rigid body dynamics around the fixed point. Mass moment vectors
coupled for the fixed point and the instantaneous axis and Linear momentum
and angular momentum for the fixed point and the rigid body dynamics
e
k
k
Ï Ï
Ï
Ï
âČ
=
+
+
r
r
r
r
&
&
&
,
with the components in the fixed coordinate system
Oxyz
(see Fig.7):
A
O
âĄ
Ï
r
v
r
p
d
r
F
I
d
r
x
y
z
Ο
η
ζ
dm
r
r
Ï
Ï
Ï
&
Ï
Ï
&
Ï
Ï
&
Ï
e
r
Ï
d
r
c
r
a*
A
O
âĄ
Ï
r
â
v
r
â
p
d
r
â
F
I
d
r
â
x
y
z
Ο
η
ζ
dm
r
r
Ï
â
Ï
â
Ï
&
â
Ï
â
Ï
&
â
Ï
â
Ï
&
â
Ï
â
e
r
Ï
â
d
r
c
r
b
â
Figure 7.
a
â
and b
â
Dynamics of the rigid body rotation around the fixed
point- Eulerâs angles:
Ï
- roll,
Ï
- pitch and
Ï
- yaw.
(
Ï
angle of precession ,
Ï
angle of nutation an
Ï
angle of self rotation)
K.S.HEDRIH: LEONHARD EULER (1707-1783) AND RIGID BODY DYNAMICS
7
(
)
cos
sin sin
x
i
Ï
Ï
Ï Ï
Ï
Ï
=
+
r
r
&
&
,
(
)
sin
cos sin
y
j
Ï
Ï
Ï Ï
Ï
Ï
=
â
r
r
&
&
,
(
)
cos
z
k
Ï
Ï Ï
Ï
=
+
r
r
&
&
.
or in the scalar form
cos
sin sin
x
Ï
Ï
Ï Ï
Ï
Ï
=
+
&
&
cos
sin cos
y
Ï
Ï
Ï Ï
Ï
Ï
=
â
&
&
cos
z
Ï
Ï Ï
Ï
= +
&
&
The components of the instantaneous angular velocity in
the moving coordinate system
O
Οηζ
fixed with the rigid
body are (see Fig.7):
(
)
cos
sin sin
i
Ο
Ï
Ï
Ï Ï
Ï
Ï
âČ
=
â
r
r
&
&
,
(
)
sin
cos sin
j
η
Ï
Ï
Ï Ï
Ï
Ï
=
+
r
r
&
&
,
(
)
cos
k
ζ
Ï
Ï Ï
Ï
âČ
=
+
r
r
&
&
or in the scalar form
cos
sin sin
Ο
Ï
Ï
Ï Ï
Ï
Ï
=
â
&
&
sin
cos sin
η
Ï
Ï
Ï Ï
Ï
Ï
=
+
&
&
cos
ζ
Ï
Ï Ï
Ï
= +
&
&
The linear momentum (impuls of the motion) and the
angular momentum (kinetic moment of the motion) of the
body rotation around the fixed point
O
expressed by the
body mass moment vectors are in the following forms:
â
â
The linear momentum (impulse of the body mass mo-
tion)
( )
p t
r
of motion of a material system, or a rigid
body rotating around a fixed axis
n
r
with the angular ve-
locity
n
Ï Ï
=
r
r
is given in the following form:
( )
[ ]
[
]
( )
0
,
,
n
C
V
p t
n r dm
n r
M
S
Ï
Ï
Ï
=
=
=
â«â«â«
r
r
r
r r
r r
,
where
( )
[ ]
0
,
n
V
S
n r dm
=
â«â«â«
r
r
r r
.
( )
0
n
S
r
r
is the mass linear moment of the body with respect to
the pole
O
and for the axis oriented by the unit vector
n
r
,
passing through the point
O
(see Refs. Hedrih 1991, 1992,
1993a,b, 1998a,b,c, 2001,2007).
â
â
Angular momentum
0
r
L
for the rigid body rotating
around the fixed axis oriented by the unit vector
n
r
,
through the pole
O
, with the angular velocity
n
Ï Ï
=
r
r
is
in the following form:
[ ]
[
]
( )
0
0
, ,
n
V
r n r
dm
Ï
Ï
=
=
â«â«â«
r
r
r
r r r
L
J
where we introduce the following notation
( )
[ ]
[
]
J
, ,
def
n
O
V
r n r
dm
=
â«â«â«
r
r
r r r
for the mass inertia moment vector
( )
0
J
n
r
r
for the pole
O
and
the fixed axis oriented by the unit vector
n
r
.
The mass inertia moment vector
( )
0
J
n
r
r
has two
components: one component
0
n
J
is in the rotation axis
direction and corresponds to the axial body mass inertia
moment and the second component
( )
0
n
D
r
r
is orthogonal to
the rotation axis and is the deviational component in the
deviational plane.
( )
0
n
J
r
r
can be expressed in the following
form (see Refs. Hedrih 1998a,b,c, 2001,2007):
( )
( )
(
)
( )
( )
0
0
0
0
0
,
,
,
n
n
n
n
n
O
n J
n
n
n
J n
âĄ
â€
âĄ
â€
=
+
=
+
âŁ
âŠ
âŁ
âŠ
J
J
D
r
r
r
r
r
r
r
r
r
r
r
r
r
.
Kinetic energy for that case of the model motion is:
(
)
[ ]
[
]
(
)
( )
(
)
[ ]
( )
2
2
0
0
2
2
2
0
,
, , ,
, J
,
2
n
V
n
k
n
V
n r n r
dm
n
n r
dm
J
E
Ï
Ï
Ï
Ï
Ï
=
=
=
=
=
â«â«â«
â«â«â«
r
r
r
r
r
r r r r
r
r r
L
.
For obtaining the necessary mass moment vector
( )
0
n
J
r
r
for the rotation axis oriented by the unit vector
n
r
through
the pole
O
, or the mass moment vector
( )
n
C
J
r
r
for the parallel
axis oriented by same unit vector
n
r
through the rigid body
mass center
C
, we can use the following vector
expressions:
( )
[ ]
[
]
( )
( )
( )
0
0
0
0
, ,
cos
cos
cos
k
i
j
n
C
V
r n r
dm
α
α
Îł
=
=
+
+
â«â«â«
J
J
J
J
r
r
r
r
r
r
r
r r r
( )
[
]
[
]
( )
( )
( )
0
, ,
cos
cos
cos
k
i
j
n
C
C
C
C
V
n
dm
Ï
Ï
α
α
Îł
=
=
+
+
â«â«â«
J
J
J
J
r
r
r
r
r
r
r
r
r
r
( )
( )
[
]
[
]
0
, ,
n
n
C
C
C
r
n r
M
=
+
J
J
r
r
r
r
r r r
where cos
α
,
cos
ÎČ
and
cos
Îł
are cosines of the direction of
the unit vector
n
r
rotating axis orientation with respect to the
corresponding system coordinates,
M
is the rigid body mass,
and
C
r
r
is the vector position of the rigid body mass center.
For this considered case of the material system model
rotation around the fixed point, it is necessary to point out that
both vectors of mass moments are changeable with respect to
the fixed point and instantaneous axis of rotation. This happens
because the instantaneous axis and the rigid body change their
relative positions and the relation to each other during the body
rotation motion around the fixed point.
Euler equations in the vector form, using the mass
moment vectors coupled to the fixed point and the
instantaneous axis are:
( )
( )
( )
( )
0
0
0
1
,
S
n
n
n
k
AN
An
k
dp t
S
S
S
F
G
F
F
dt
Ï
Ï
Ï Ï
=
âĄ
â€
=
+
+
=
+ +
+
âŁ
âŠ
â
r
r
r
r
r
r
r
r
r
r
r
r
&
&
( )
( )
( )
*
0
0
0
0
1
J
J
, J
,
,
S
n
n
n
k
k
C
k
d
r F
r G
dt
Ï
Ï
Ï Ï
=
âĄ
â€
âĄ
â€
âĄ
â€
=
+
+
=
+
âŁ
⊠âŁ
âŠ
âŁ
âŠ
â
L
r
r
r
r
r
r
r
r
r
r
r
r
&
, (A)
as well as
*
0
0
0
1
L
L
, L
,
,
S
k
k
C
k
d
r F
r G
dt
Ï
=
âĄ
â€
âĄ
â€
âĄ
â€
= +
=
+
=
âŁ
âŠ
âŁ
⊠âŁ
âŠ
â
r
r
r
r
r
r
r
r
r
M
, (B)
This previous vector equation (B) is equation of the
8
K.S.HEDRIH: LEONHARD EULER (1707-1783) AND RIGID BODY DYNAMICS
motion and it is possible to express it in the scalar form by
three differential equations of Eulerâs type:
(
)
(
)
(
)
0
0
0
0
0
1
,
.
,
,
,
S
k
k
C
k
L
L
L
r F
i
r G
i
i
Ο
η
ζ
ζ
η
Ο
Ï
Ï
=
+
â
=
âĄ
â€
âĄ
†âČ
âČ
âČ
=
+
=
=
âŁ
âŠ
âŁ
âŠ
â
&
r
r
r
r
r
r
r
r
M
M
(
)
(
)
(
)
0
0
0
0
0
1
L
L
L
,
,
,
,
M ,
M
S
k
k
C
k
r F
j
r G
j
j
η
ζ
Ο
Ο
ζ
η
Ï
Ï
=
+
â
=
âĄ
â€
âĄ
†âČ
âČ
âČ
=
+
=
=
âŁ
âŠ
âŁ
âŠ
â
&
r
r
r
r
r
r
r
(
)
(
)
(
)
0
0
0
0
0
1
,
,
,
,
,
S
k
k
C
k
L
L
L
r F
k
r G
k
k
ζ
Ο
η
η
Ο
ζ
Ï
Ï
=
+
â
=
âĄ
â€
âĄ
†âČ
âČ
âČ
=
+
=
=
âŁ
âŠ
âŁ
âŠ
â
&
r
r
r
r
r
r
r
r
M
M
or: in the following shorter form:
0
0
0
0
L
L
L
Ο
η
ζ
ζ
η
Ο
Ï
Ï
+
â
=
&
M
,
0
0
0
0
L
L
L
η
ζ
Ο
Ο
ζ
η
Ï
Ï
+
â
=
&
M
,
0
0
0
0
L
L
L
ζ
Ο
η
η
Ο
ζ
Ï
Ï
+
â
=
&
M
.
For the case in which the coordinate axes of the moving
coordinate system fixed to the rigid body are body principal
mass inertia moment axes, from the previous Euler system
of differential equations we have:
(
)
1 01
2 3
02
03
01
J
J
J
Ï
Ï Ï
â
â
=
&
M
,
(
)
2 02
1 3
02
01
02
J
J
J
Ï
Ï Ï
â
â
=
&
M
,
(
)
3 03
1 2
01
02
03
J
J
J
Ï
Ï Ï
â
â
=
&
M
.
The first vector equation from the system (A) of the
vector equations is possible to obtain kinetic pressure to the
fixed point (bearing, or to kinetic reaction or necessary
action by the body).
Citations
* The most cited mathematician of all times
* Over 20 formulae of elementary mathematics bear Eulerâs
name
* An even greater number of formulas and notions of
advanced mathematics bears his name.
* The most fruitful mathematician of all times
(800 pages per year)
Some elementary Euler formulae and theorems
Figure 16.
Eulerâs line
Figure 8.
Eulerâs line
cos
sin
ix
e
x
i
x
=
+
Figure 9.
Eulerâs formula
Graph theory
Figure 10.
The problem of seven Koenigsberg bridges
If all nodes are even, the graph can be drawn by starting
from each of them (1736).
A graph with more than two odd nodes cannot be drawn
in a single stroke.
Figure 11.
Examples of graphs.
K.S.HEDRIH: LEONHARD EULER (1707-1783) AND RIGID BODY DYNAMICS
9
Concluding Remarks
Euler's program for mechanics presented in the treatise
(Mechanics or the analytical representation of the science
of motion) paved the way for a successful development of
mechanics in the 18th century. In contrast to Newton's
geometry-related procedure in the Principia, Euler
formulated mechanical laws preferentially in terms of the
differential calculus. Euler claimed that ''those laws of
motion which a body observes when left to itself in
continuing either rest or motion pertain properly to
infinitely small bodies''. Geometrically, these bodies can be
considered as points, but mechanically they are less than
any extended body, but different from mathematical points
due to their finite mass. Analytically, motion is described in
terms of infinitesimal time intervals whereas,
geometrically, it is related to straight lines and planes as
basic elements.
In fluid dynamics, the
Euler equations
govern the
compressible, in viscid flow. They correspond to the
Navier-Stokes equations with zero viscosity and heat
conduction terms. They are usually written in the
conservation form shown below to emphasize that they
directly represent conservation of mass, momentum, and
energy.
Momentum Equation for Frictionless Flow: Eulerâs
Equation
Eulerâs Equation
DV
g
p
Dt
Ï
Ï
=
â â
v
v
In the Cartesian coordinate system
x
p
u
u
u
u
u
v
w
g
t
x
y
z
x
Ï
Ï
â
â
â
â
â
â
â
=
+
+
+
=
â
â
â
â
â
â
â
â
â
â
z
p
u
w
g
t
x
y
z
z
Ï
Ï
Ï
Ï
Ï
Ï
Ï
â
â
â
â
â
â
â
=
+
+
+
=
â
â
â
â
â
â
â
â
â
â
z
p
w
w
w
w
u
w
g
t
x
y
z
z
Ï
Ï
Ï
â
â
â
â
â
â
â
=
+
+
+
=
â
â
â
â
â
â
â
â
â
â
In the cylindrical coordinate system
2
r
r
r
r
r
r
z
r
p
V
V
V
V
V
V
a
V
V
g
t
r
r
z
r
r
Ξ
Ξ
Ï
Ï
Ï
Ξ
â
â
â
â
â
â
â
=
+
+
+
â
=
â
â
â
â
â
â
â
â
â
â
1
r
r
z
V
V
V
V
V V
V
a
V
V
t
r
r
z
r
p
g
r
Ξ
Ξ
Ξ
Ξ
Ξ
Ξ
Ξ
Ξ
Ï
Ï
Ξ
Ï
Ξ
â
â
â
â
â
â
=
+
+
+
â
â
â
â
â
â
â
â
â
â
=
â
â
z
z
z
z
z
r
z
z
p
V
V
V
V
V
a
V
V
g
t
r
r
z
z
Ξ
Ï
Ï
Ï
Ξ
â
â
â
â
â
â
â
=
+
+
+
=
â
â
â
â
â
â
â
â
â
â
Continuity
0
V
â â =
r
Euler's contributions to Rational or Mathematical Fluid
Mechanics are important contributions as well as his
contribution to the General Theory of the Motion of Fluids.
Euler's generalization of the stream function concept to a pair
of stream functions or stream surfaces is also the result of his
research. Euler's Potential had been formulated about 100
years before a similar detailed mathematical exposure was
formulated by Jacobi and Clebsch around 1844. Furthermore,
Euler's work initiated the establishment of naval science in
Russia and influenced the art of building naval ships in
Russia in the 18th century in particular. An overview about
Euler's accomplishments in Naval Architecture and Ship
Hydrodynamics at Russia's St. Petersburg Academy of
Sciences is also an important contribution to world science
and to mechanical engineering.
The theory of magnetism for which he was awarded the
Paris Academy Prize in 1744 is also very well known. Euler
began with Descartes' idea that all magnetic phenomena are
elicited from the circulation of imperceptible conduits
throughout the corpuscular magnetic body. Euler imagined
that the magnetic body possessed pores which formed
continuous piping, parallel and bristling, similar to veins or
valves and so narrow as to only allow passage for the most
subtle parts of the ether, the elasticity of which pushes the
relaxed parts into the magnet pores. Then the force causes it
to bend onto itself at the exit only to return again and form
a type of vortex. Through this ingenious idea which was
developed after much thought, Euler was able to explain
magnetic phenomenon. The hypothesis was proved out by
experiments and these conformed to natural laws which in
turn ensured its ultimate probability.
The Opera Omnia
"Read Euler, read Euler, he is the teacher (master) of us all".
Pierre-Simon, marquis de Laplace (March 23, 1749 - March 5, 1827)
Published by Birkhauser and the
Euler Commission
of
Switzerland, the
Opera Omnia
is the definitive printed
source for Euler's works. The publication began in 1911,
and to date 76 volumes have been published, comprising
almost all of Euler's works.
Principle:
â
Mathematicians do not have biography, they have
bibliography
â
References
The URL of this page is:
http://www-history.mcs.st-andrews.ac.uk/Biographies/Euler.html
http://www.leonhard-euler.ch/
For more information about the Euler Commission please contact Herr
Prof.Dr.Hanspeter Kraft President of the Euler Commission
Hanspeter.kraft@unibas.ch
10
K.S.HEDRIH: LEONHARD EULER (1707-1783) AND RIGID BODY DYNAMICS
[1]
FINKEL,B.F. (1897).:
Biography - Leonard Euler
, The American
Mathematical Monthly 4 (12): 300.
[2]
IOAN,J.(2002):
Remarkable Mathematicians: From Euler to von
Neumann
, Cambridge, 2. ISBN 0-521-52094-0.
[3]
CALINGER,R. (1996):
Leonhard Euler: The First St. Petersburg
Years (1727â1741)
, Historia Mathematica 23 (2): 156.
[4]
CALINGER,R. (1996):
Leonhard Euler: The First St. Petersburg
Years (1727â1741)
, Historia Mathematica 23 (2): 125.
[5]
CALINGER,R. (1996):
Leonhard Euler: The First St. Petersburg
Years (1727â1741)
, Historia Mathematica 23 (2): 127.
[6]
CALINGER,R. (1996):
Leonhard Euler: The First St. Petersburg
Years (1727â1741)
, Historia Mathematica 23 (2): 128â129.
[7]
HOME,R.W. (1988):
Leonhard Euler's 'Anti-Newtonian' Theory of
Light
, Annals of Science 45 (5): 521â533.
[8]
O'CONNOR,J., EDMUND,J., ROBERTSON,F.: "Leonhard Euler".
MacTutor History of Mathematics archive
.
[9]
Leonhard Euler at the Mathematics Genealogy Project
[10]
WEISSTEIN,E.W.: Euler, Leonhard (1707â1783) at ScienceWorld.
How Euler did it Website containing columns explaining how Euler solved
various problems.
[11]
GLADYSHEV,G.,P. (2007): âLeonhard Eulerâs methods and ideas
live on in the thermodynamic hierarchical theory of biological
evolution,â
International Journal of Applied Mathematics &
Statistics
(IJAMAS), Special Issue on Leonhard Paul Eulerâs:
Mathematical Topics and Applications (M. T. A.), Vol. 11, Nu. N07,
November, 2007.
[12]
CONDORCET,M.J.:
Eulogy for Euler
(See this link).
[13]
G DU PASQUIER:
Leonhard Euler et ses amis
(Paris, 1927).
[14]
SPEISS,O.:
Leonhard Euler
(1929).
[15]
THIELE,R.:
Leonhard Euler
(Leipzig,1982).
[16]
YUSHKEVICH,A.P., WINTER,E. (eds.): Leonhard Euler and
Christian Goldbach: Briefwechsel 1729-1764 (Berlin, 1965).
[17]
ANDREWS,G.E.:
Euler's pentagonal number theorem
, Math. Mag.
56 (5) (1983), 279-284.
[18]
ANTROPOV,A.A.:
On Euler's partition of forms into genera
,
Historia Math. 22 (2) (1995), 188-193.
[19]
Chobanov,G., Chobanov,I.: Lagrange or Euler? I. The past,
Annuaire
Univ. Sofia Fac. Math. MĂ©c.
73 (1979), 13-51.
[20]
CHOBANOV,G., CHOBANOV,I.: Lagrange or Euler? II. The
present,
Annuaire Univ.
Sofia Fac
.
Math. Inform
.
82 (2) (1988), 5-62.
[21]
CHOBANOV,G., CHOBANOV,I.: Lagrange or Euler? III. The
future,
Annuaire Univ. Sofia Fac. Math. Inform.
82 (2) (1988), 63-
109.
[22]
DAVIS,P.J.: Leonhard Euler's integral: A historical profile of the
gamma function,
Amer. Math. Monthly
66
(1959), 849-869.
[23]
FELLMANN,E.A.: Leonhard Euler 1707-1783 : Schlaglichter auf
sein Leben und Werk,
Helv. Phys. Acta
56
(6) (1983), 1099-1131.
[24]
FINKEL,B.F.: Biography. Leonard Euler,
Amer. Math. Monthly
4
(1897), 297-302.
[25]
FRASER,C.G.: The origins of Euler's variational calculus,
Arch.
Hist. Exact Sci.
47 (2) (1994), 103-141.
[26]
GRAU,C.: Leonhard Euler und die Berliner Akademie der
Wissenschaften, in
Ceremony and scientific conference on the
occasion of the 200th anniversary of the death of Leonhard Euler
(Berlin, 1985), 139-149.
[27]
GRAY,J.: Leonhard Euler 1707-1783,
Janus: archives
internationales pour l'histoire de la medecine et pour la geographie
medicale
72 (1985), 171-192.
[28]
GRAY,J.: Leonhard Euler: 1707-1783, Janus 72 (1-3) (1985), 171-192.
[29]
HOLLINGDALE,S.H.: Leonhard Euler (1707-1783):
a bicentennial
tribute
, Bull. Inst. Math. Appl. 19 (5-6) (1983), 98-105.
[30]
HOME,R.W.:
Leonhard Euler's 'anti-Newtonian' theory of light
,
Ann. of Sci. 45 (5) (1988), 521-533.
[31]
KNOBLOCH,E.:
Leibniz and Euler: problems and solutions
concerning infinitesimal geometry and calculus
, Conference on the
History of Mathematics (Rende, 1991), 293-313.
[32]
Loeffel,H.: Leonhard Euler (1707-1783),
Mitt.
Verein. Schweiz
.
Versicherungsmath. (1) (1984), 19-32.
[33]
MIKHAILOV,G.K.:
Leonhard Euler and his contribution to the
development of rational mechanics
(Russian), Adv. in Mech. 8 (1)
(1985), 3-58.
[34]
SAMELSON,H.:
In defense of Euler
, Enseign. Math
.
(2) 42 (3-4)
(1996), 377-382.
[35]
TREDER,H-J.:
Euler und die Gravitationstheorie
, in Ceremony and
scientific conference on the occasion of the 200th anniversary of the
death of Leonhard Euler (Berlin, 1985), 112-119.
[36]
TRUESDELL,C.:
Euler's contribution to the theory of ships and
mechanics
, Centaurus 26 (4) (1982/83), 323-335.
[37]
TRUESDELL,C.: Prefaces to volumes of Euler's Opera Omnia.
[38]
TYULINA,I.A.:
Euler's hydraulic studies
(Russian), in Investigations
in the history of mechanics 'Nauka' (Moscow, 1983), 167-177.
[39]
MAANEN,J.A.: Leonhard Euler (1707-1783):
man, worker, migrant
,
genius (Dutch), Nieuw Tijdschr. Wisk. 71 (1) (1983/84) 1-11.
[40]
VELDKAMP,G.R.: Leonhard Euler (Dutch), Nieuw Tijdschr. Wisk.
71 (2) (1983), 47-54.
[41]
YUSHKEVICH,A.P.:
Leonhard Euler and mathematical education
in Russia
(Russian), Mat. v Shkole (5) (1983), 71-74.
[42]
YUSHKEVICH,A.P.:
Life and mathematical achievement of Leonard
Euler
(Russian), Uspekhi Mat. Nauk (N.S.) 12 4(76) (1957), 3-28.
[43]
YUSHKEVICH,A.P.: Leonhard Euler :
Life and work
(Russian), in
Development of the ideas of Leonhard Euler and modern science
âNaukaâ (Moscow, 1988), 15-46.
[44]
RAĆ KOVI
Ä
,D.,
Dinamika
, Nau
Ä
na knjiga, Beograd, 1956.
[45]
HEDRIH,S.K. (2001): V
ector Method of the Heavy Rotor Kinetic
Parameter Analysis and Nonlinear Dynamics
, University of NiĆĄ
2001,Monograph, pp.252. (in English), YU ISBN 86-7181-046-1.
[46]
KECHRIS,K.: Leinhar Euler
[47]
http://en.wikipedia.org/wiki/Template:Bernoulli_family
[48]
www.mathematik.ch
[49]
http://en.wikipedia.org/wiki/Leonhard_Euler
[50]
http://www-groups.dcs.st-and.ac.uk/~history/Biographies/Euler.html
[51]
HEDRIH,S.K. (1991): A
nalogy between models of stress state, strain
state and state of the body mass inertia moments
, Facta Universitatis,
Series Mechanics, Automatic Control and Robotics, NiĆĄ, vol.1, N 1,
1991, pp.105-120.
[52]
HEDRIH,S.K. (1992):
On some interpretations of the rigid bodies
kinetic parameters
, XVIIIth ICTAM HAIFA, Abstracts, pp.73-74.
[53]
HEDRIH,S.K. (1993a):
The mass moment vectors at n-dimensional
coordinate system
, Tensor, Japan, Vol.54 (1993), pp.83-87.
[54]
HEDRIH,S.K. (1993b):
Same vectorial inter-pretations of the kinetic
parameters of solid material lines
, ZAMM. Angew. Math. Mech.
73(1993) 4-5, T153-T156.
[55]
HEDRIH,S.K. (1998a):
Vectors of the Body Mass Moments
,
Monograph paper, Topics from Mathematics and Mechanics,
Mathematical institute SANU, Belgrade, Zbornik radova 8(16), 1998,
pp.45-104.
[56]
HEDRIH,S.K. (1998b):
Vector method of the kinetic parameters
analysis of the rotor with many axes and nonlinear dynamics
, Parallel
General Lecture, Third International Conference on Nonlinear
Mechanics, August 17-20, 1998, Shanghai, China, pp.42-47.
[57]
HEDRIH,S.K. (1998c):
Derivatives of the Mass Moments Vectors
with Applications
, Invited Lecture, Proceedings, 5th National
Congress on Mechanics, Ioannina, 1998, pp.694-705
[58]
HEDRIH,S.K. (2001): Vector Method of the Heavy Rotor Kinetic
Parameter Analysis and Nonlinear Dynamics, University of NiĆĄ
2001, Monograph, pp.252. (in English), YU ISBN 86-7181-046-1.
[59]
HEDRIH,S.K. (2001): Derivatives of the Mass Moment Vectors at
the Dimensional Coordinate System N, dedicated to memory of
Professor D. Mitrinovi
Ä
, Facta Universitatis Series Mathematics and
Informatics, 13 (1998), pp. 139-150. (1998, published in 2001. Edited
by Milovanovi
Ä
,G.).
[60]
HEDRIH,S.K. (2007):
For optimal time of study: vector and tensor
methods in classical mechanics
, Plenary Lecture, Proceedings
Nonlinear Dynamics, Dedicated to the 150th Anniversary of A.M.
Lyapunov, Polytechnic Kharkov, 2008. pp.98-107.
Received: 15.05.2007.
K.S.HEDRIH: LEONHARD EULER (1707-1783) AND RIGID BODY DYNAMICS
11
Leonardo Ojler (1707-1783) i mehanika krutog tela
Uvodni tekst ovog broja
Ä
asopisa posve
Ä
en 300. godiĆĄnjici od ro
Ä
enja Leonarda Ojlera, jednog od najpoznatijih
nau
Ä
nika XVIII veka iz oblasti matematike i mehanike. Ro
Ä
en je 15. aprila 1707 godine u Bazelu, Ć vajcarska.
Zahvaljuju
Ä
i znamenitom Bernuliju, koji je uticao na njegovog oca da promeni svoju odluku, posvetio se matematici
umesto teologiji. Iako je ve
Ä
i deo njegovog rada bio iz oblasti elementarne matematike dao je zna
Ä
ajan nau
Ä
ni
doprinos i u oblasti astronomije i fizike.
U svojim radnim dvadesetim godinama Ojler je izgubio oko. Kasnije je ostao i bez drugog oka, ali je uprkos tome bio
vrlo produktivan. Tokom ĆŸivota objavio je oko 500 knjiga i radova, a joĆĄ oko 400 radova objavljeno je posthumno.
Laplas je govorio svojim studentima: "
Ä
itajte Ojlera,
Ä
itajte Ojlera! on je gospodar sviju nas"
Leonhard Euler (1707-1783) et la mécanique du corps solide
LâĂ©ditorial de ce numĂ©ro est dĂ©diĂ© au 300
iĂšme
anniversaire de la naissance de Leonhard Euler, savant célÚbre du 18
iĂšme
siÚcle, trÚs connu pour ces travaux en mathématique et mécanique. Il est né le 15 avril 1707 à Bùle, en Suisse. Il devait,
selon le désir de son pÚre, étudier la théologie, mais grùce à célÚbre savant Bernoulli qui a influencé le pÚre de
Leonhard, celui-ci a pu se consacrer aux mathématiques. Bien que la majeure partie de son travail concerne les
mathĂ©matiques Ă©lĂ©mentaires, sa contribution est considĂ©rable en astronomie et en physique. A lâĂąge de vingt ans
Euler a perdu un Ćil; plus tard il a perdu son autre Ćil, mais malgrĂ© cela il Ă©tait trĂšs productif. Au cours de sa vie il a
publié environ 500 livres et travaux; aprÚs sa mort, on a publié encore 400 travaux. Laplace disait souvent à ses
Ă©tudiants: "Lisez Euler, lisez Euler! Il est maĂźtre de nous tous".
12
K.S.HEDRIH: LEONHARD EULER (1707-1783) AND RIGID BODY DYNAMICS
Leonhard Euler