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Abstract

This important chapter is devoted to integration on smooth manifolds.

The basic concept here, the surface area, is introduced in Sect. 8.2, where we discuss its basic properties (including the one-dimensional case of the length of a curve) and different approaches to the definition of the area of a surface (Schwarz lantern).

In Sects. 8.3 and 8.4, we establish formulas for computing the area of a surface and integrals over it, including the Kronrod–Federer theorem.

We discuss the preservation of a surface under bendings and the uniqueness of the Borel measure on a sphere, invariant under rotations. The exposition is accompanied by examples, in particular, we consider the “measure concentration effect” on a sphere.

Section 8.6 devoted to the Gauss–Ostrogradski formula (the divergence formula), which is established under very general assumptions. We discuss particular cases of this formula in the case of functions of two variables (the Green formula, the Cauchy integral theorem).

In Sect. 8.7, we use the results obtained and discuss the important class of harmonic functions in detail. We establish their basic properties (the mean value theorem, Harnack’s inequality, etc.). We also consider the Dirichlet problems for a ball and a half-plane.

In Sect. 8.8, we extend the results obtained in the case of smooth manifolds to the Lipschitz manifolds. Here, in particular, we prove that the area on Lipschitz manifolds is semicontinuous.

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Notes

  1. 1.

    The reader familiar with the theory of manifolds will note that, except in the case of dimension one, we consider only manifolds without a boundary.

  2. 2.

    In reality, the International Date Line is determined by special agreements and does not coincide with this meridian completely.

  3. 3.

    Ernest Leonhard Lindelöf (1870–1946)—Finnish mathematician.

  4. 4.

    Karl Hermann Amandus Schwarz (1843–1921)—German mathematician.

  5. 5.

    More precisely, of its restriction to \(\mathfrak{B}^{k}\).

  6. 6.

    James Clerk Maxwell (1831–1879)—Scottish physicist.

  7. 7.

    Alexandr Semenovich Kronrod (1921–1986)—Russian mathematician.

  8. 8.

    Herbert Federer (1920–2010)—American mathematician.

  9. 9.

    August Ferdinand Möbius (1790–1868)—German mathematician.

  10. 10.

    We leave the reader to deduce this formula using the intuitively clear properties of the flow and the general scheme considered in Sect. 6.3.

  11. 11.

    Mikhail Vasil’evich Ostrogradski (1801–1862)—Russian mathematician.

  12. 12.

    Blaise Pascal (1623–1662)—French philosopher, mathematician, and physicist.

  13. 13.

    George Green (1793–1841)—English mathematician and physicist.

  14. 14.

    William Thomson, Lord Kelvin (1824–1907)—English physicist and mathematician.

  15. 15.

    Carl Gustav Axel Harnack (1851–1888)—German mathematician.

References

  1. Boltyansky, V.G.: Curve Length and Surface Area. Encyclopaedia of Elementary Mathematics. Geometry, vol. 5. Nauka, Moscow (1966) [in Russian]. 8.8.5

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  2. Burago, Yu.D., Zalgaller, V.A.: Geometric Inequalities. Springer, Berlin (1988). 2.8.1

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  3. Evans, L.C., Gariepy, R.F.: Measure Theory and Fine Properties of Functions. CRC Press, Boca Raton (1992). 6.2.1, 8.4.2, 8.4.5

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  4. Federer, H.: Geometric Measure Theory. Springer, New York (1969). 2.8.1, 8.2.2, 8.4.4, 8.8.1, 10.3 (Ex. 5), 13.2.3

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  5. Vladimirov, V.S.: Equations of Mathematical Physics. Marcel Dekker, New York (1971). 8.7.9

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© 2013 Springer-Verlag London

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Makarov, B., Podkorytov, A. (2013). Surface Integrals. In: Real Analysis: Measures, Integrals and Applications. Universitext. Springer, London. https://doi.org/10.1007/978-1-4471-5122-7_8

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