Differential geometry: Difference between revisions

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Differential geometry arose and developed as a result of and in connection to the mathematical analysis of curves and surfaces.<ref>http://www.encyclopediaofmath.org/index.php/Differential_geometry be referred to</ref> Mathematical analysis of curves and surfaces had been developed to answer some of the nagging and unanswered questions that appeared in [[calculus]], like the reasons for relationships between complex shapes and curves, series and analytic functions. These unanswered questions indicated greater, hidden relationships.
Differential geometry arose and developed as a result of and in connection to the mathematical analysis of curves and surfaces.<ref>http://www.encyclopediaofmath.org/index.php/Differential_geometry be referred to</ref> Mathematical analysis of curves and surfaces had been developed to answer some of the nagging and unanswered questions that appeared in [[calculus]], like the reasons for relationships between complex shapes and curves, series and analytic functions. These unanswered questions indicated greater, hidden relationships.

The general idea of natural equations for obtaining curves from local curvature appears to have been first considered by [[Leonhard Euler]] in 1736, and many examples with fairly simple behavior were studied in the 1800's.<ref>{{cite book|last=Wolfram|first=Stephen|title=A New Kind of Science|publisher=Wolfram Media, Inc.|year=2002|page=1009|isbn=1-57955-008-8}}</ref>


When curves, surfaces enclosed by curves, and points on curves were found to be quantitatively, and generally, related by mathematical forms, the formal study of the nature of curves and surfaces became a field of study in its own right, with [[Gaspard Monge#Work|Monge]]'s paper in 1795, and especially, with [[Carl Friedrich Gauss|Gauss]]'s publication of his article, titled 'Disquisitiones Generales Circa Superficies Curvas', in ''Commentationes Societatis Regiae Scientiarum Gottingesis Recentiores'' in 1827.<ref>'Disquisitiones Generales Circa Superficies Curvas' (literal translation from Latin: General Investigations of Curved Surfaces), ''Commentationes Societatis Regiae Scientiarum Gottingesis Recentiores'' (literally, Recent Perspectives, Gottingen's Royal Society of Science). Volume VI, pp. 99–146. A translation of the work, by A.M.Hiltebeitel and J.C.Morehead, titled, "General Investigations of Curved Surfaces" was published 1965 by Raven Press, New York. A digitised version of the same is available at http://quod.lib.umich.edu/u/umhistmath/abr1255.0001.001 for free download, for non-commercial, personal use. In case of further information, the library could be contacted.
When curves, surfaces enclosed by curves, and points on curves were found to be quantitatively, and generally, related by mathematical forms, the formal study of the nature of curves and surfaces became a field of study in its own right, with [[Gaspard Monge#Work|Monge]]'s paper in 1795, and especially, with [[Carl Friedrich Gauss|Gauss]]'s publication of his article, titled 'Disquisitiones Generales Circa Superficies Curvas', in ''Commentationes Societatis Regiae Scientiarum Gottingesis Recentiores'' in 1827.<ref>'Disquisitiones Generales Circa Superficies Curvas' (literal translation from Latin: General Investigations of Curved Surfaces), ''Commentationes Societatis Regiae Scientiarum Gottingesis Recentiores'' (literally, Recent Perspectives, Gottingen's Royal Society of Science). Volume VI, pp. 99–146. A translation of the work, by A.M.Hiltebeitel and J.C.Morehead, titled, "General Investigations of Curved Surfaces" was published 1965 by Raven Press, New York. A digitised version of the same is available at http://quod.lib.umich.edu/u/umhistmath/abr1255.0001.001 for free download, for non-commercial, personal use. In case of further information, the library could be contacted.

Revision as of 18:50, 1 May 2018

hyperbolic paraboloid), as well as two diverging ultraparallel lines
.

Differential geometry is a

formed the basis for development of differential geometry during the 18th century and the 19th century.

Since the late 19th century, differential geometry has grown into a field concerned more generally with the geometric structures on differentiable manifolds. Differential geometry is closely related to differential topology and the geometric aspects of the theory of differential equations. The differential geometry of surfaces captures many of the key ideas and techniques endemic to this field.

History of development

Differential geometry arose and developed as a result of and in connection to the mathematical analysis of curves and surfaces.[1] Mathematical analysis of curves and surfaces had been developed to answer some of the nagging and unanswered questions that appeared in calculus, like the reasons for relationships between complex shapes and curves, series and analytic functions. These unanswered questions indicated greater, hidden relationships.

The general idea of natural equations for obtaining curves from local curvature appears to have been first considered by Leonhard Euler in 1736, and many examples with fairly simple behavior were studied in the 1800's.[2]

When curves, surfaces enclosed by curves, and points on curves were found to be quantitatively, and generally, related by mathematical forms, the formal study of the nature of curves and surfaces became a field of study in its own right, with Monge's paper in 1795, and especially, with Gauss's publication of his article, titled 'Disquisitiones Generales Circa Superficies Curvas', in Commentationes Societatis Regiae Scientiarum Gottingesis Recentiores in 1827.[3]

Initially applied to the Euclidean space, further explorations led to non-Euclidean space, and metric and topological spaces.

Branches

Riemannian geometry

Riemannian geometry studies

first order of approximation. Various concepts based on length, such as the arc length of curves, area of plane regions, and volume of solids all possess natural analogues in Riemannian geometry. The notion of a directional derivative of a function from multivariable calculus is extended in Riemannian geometry to the notion of a covariant derivative of a tensor
. Many concepts and techniques of analysis and differential equations have been generalized to the setting of Riemannian manifolds.

A distance-preserving

Riemannian symmetric spaces, whose curvature is not necessarily constant. These are the closest analogues to the "ordinary" plane and space considered in Euclidean and non-Euclidean geometry
.

Pseudo-Riemannian geometry

positive-definite
. A special case of this is a
Lorentzian manifold, which is the mathematical basis of Einstein's general relativity theory of gravity
.

Finsler geometry

Banach norm
defined on each tangent space. Riemannian manifolds are special cases of the more general Finsler manifolds. A Finsler structure on a manifold M is a function F : TM → [0,∞) such that:

  1. F(x, my) = |m|F(x,y) for all x, y in TM,
  2. F is infinitely differentiable in TM − {0},
  3. The vertical Hessian of F2 is positive definite.

Symplectic geometry

non-degenerate skew-symmetric bilinear form on each tangent space, i.e., a nondegenerate 2-form
ω, called the symplectic form. A symplectic manifold is an almost symplectic manifold for which the symplectic form ω is closed: dω = 0.

A

.

By contrast with Riemannian geometry, where the

G.D. Birkhoff in 1912. It claims that if an area preserving map of an annulus twists each boundary component in opposite directions, then the map has at least two fixed points.[4]

Contact geometry

Contact geometry deals with certain manifolds of odd dimension. It is close to symplectic geometry and like the latter, it originated in questions of classical mechanics. A contact structure on a (2n + 1) – dimensional manifold M is given by a smooth hyperplane field H in the tangent bundle that is as far as possible from being associated with the level sets of a differentiable function on M (the technical term is "completely nonintegrable tangent hyperplane distribution"). Near each point p, a hyperplane distribution is determined by a nowhere vanishing 1-form , which is unique up to multiplication by a nowhere vanishing function:

A local 1-form on M is a contact form if the restriction of its exterior derivative to H is a non-degenerate two-form and thus induces a symplectic structure on Hp at each point. If the distribution H can be defined by a global one-form then this form is contact if and only if the top-dimensional form

is a volume form on M, i.e. does not vanish anywhere. A contact analogue of the Darboux theorem holds: all contact structures on an odd-dimensional manifold are locally isomorphic and can be brought to a certain local normal form by a suitable choice of the coordinate system.

Complex and Kähler geometry

Complex differential geometry is the study of

complex manifolds
. An almost complex manifold is a real manifold , endowed with a
almost complex structure
)

, such that

It follows from this definition that an almost complex manifold is even-dimensional.

An almost complex manifold is called complex if , where is a tensor of type (2, 1) related to , called the

Nijenhuis tensor
(or sometimes the torsion). An almost complex manifold is complex if and only if it admits a holomorphic coordinate atlas. An
Riemannian metric
g, satisfying the compatibility condition

.

An almost Hermitian structure defines naturally a differential two-form

.

The following two conditions are equivalent:

where is the Levi-Civita connection of . In this case, is called a

Hodge manifolds) is given by all the smooth complex projective varieties
.

CR geometry

CR geometry is the study of the intrinsic geometry of boundaries of domains in complex manifolds
.

Differential topology

Differential topology is the study of global geometric invariants without a metric or symplectic form.

Differential topology starts from the natural operations such as Lie derivative of natural vector bundles and de Rham differential of forms. Beside Lie algebroids, also Courant algebroids start playing a more important role.

Lie groups

A Lie group is a group in the category of smooth manifolds. Beside the algebraic properties this enjoys also differential geometric properties. The most obvious construction is that of a Lie algebra which is the tangent space at the unit endowed with the Lie bracket between left-invariant vector fields. Beside the structure theory there is also the wide field of representation theory.

Bundles and connections

The apparatus of vector bundles, principal bundles, and connections on bundles plays an extraordinarily important role in modern differential geometry. A smooth manifold always carries a natural vector bundle, the tangent bundle. Loosely speaking, this structure by itself is sufficient only for developing analysis on the manifold, while doing geometry requires, in addition, some way to relate the tangent spaces at different points, i.e. a notion of parallel transport. An important example is provided by affine connections. For a surface in R3, tangent planes at different points can be identified using a natural path-wise parallelism induced by the ambient Euclidean space, which has a well-known standard definition of metric and parallelism. In Riemannian geometry, the Levi-Civita connection serves a similar purpose. (The Levi-Civita connection defines path-wise parallelism in terms of a given arbitrary Riemannian metric on a manifold.) More generally, differential geometers consider spaces with a vector bundle and an arbitrary affine connection which is not defined in terms of a metric. In physics, the manifold may be the space-time continuum and the bundles and connections are related to various physical fields.

Intrinsic versus extrinsic

From the beginning and through the middle of the 18th century, differential geometry was studied from the extrinsic point of view:

theorema egregium, to the effect that Gaussian curvature
is an intrinsic invariant.

The intrinsic point of view is more flexible. For example, it is useful in relativity where space-time cannot naturally be taken as extrinsic (what would be "outside" of it?). However, there is a price to pay in technical complexity: the intrinsic definitions of curvature and connections become much less visually intuitive.

These two points of view can be reconciled, i.e. the extrinsic geometry can be considered as a structure additional to the intrinsic one. (See the

shape operator.[5]

Applications

Below are some examples of how differential geometry is applied to other fields of science and mathematics.

See also

References

  1. ^ http://www.encyclopediaofmath.org/index.php/Differential_geometry be referred to
  2. .
  3. ^ 'Disquisitiones Generales Circa Superficies Curvas' (literal translation from Latin: General Investigations of Curved Surfaces), Commentationes Societatis Regiae Scientiarum Gottingesis Recentiores (literally, Recent Perspectives, Gottingen's Royal Society of Science). Volume VI, pp. 99–146. A translation of the work, by A.M.Hiltebeitel and J.C.Morehead, titled, "General Investigations of Curved Surfaces" was published 1965 by Raven Press, New York. A digitised version of the same is available at http://quod.lib.umich.edu/u/umhistmath/abr1255.0001.001 for free download, for non-commercial, personal use. In case of further information, the library could be contacted. Also, the Wikipedia article on Gauss's works in the year 1827 at could be looked at.
  4. ^ The area preserving condition (or the twisting condition) cannot be removed. If one tries to extend such a theorem to higher dimensions, one would probably guess that a volume preserving map of a certain type must have fixed points. This is false in dimensions greater than 3.
  5. ^ Hestenes, David (2011). "The Shape of Differential Geometry in Geometric Calculus". In Dorst, L.; Lasenby, J. (eds.). Guide to Geometric Algebra in Practice. Springer Verlag. pp. 393–410. {{cite book}}: External link in |chapterurl= (help); Unknown parameter |chapterurl= ignored (|chapter-url= suggested) (help) There is also a pdf available of a scientific talk on the subject
  6. .
  7. doi:10.1109/ICASSP.2005.1416480. {{cite web}}: Missing or empty |url= (help
    )
  8. .
  9. ^ Micheli, Mario (May 2008). The Differential Geometry of Landmark Shape Manifolds: Metrics, Geodesics, and Curvature (PDF) (Ph.D.). Archived from the original (PDF) on June 4, 2011.
  10. ^ Joshi, Anand A. (August 2008). Geometric Methods for Image Processing and Signal Analysis (PDF) (Ph.D.).
  11. doi:10.1109/TIT.2003.817466.{{cite journal}}: CS1 maint: multiple names: authors list (link
    )

Further reading

External links