Skip to main content

Functions of Many Variables: Integration

  • Chapter
Mathematics for Natural Scientists

We’re sorry, something doesn't seem to be working properly.

Please try refreshing the page. If that doesn't work, please contact support so we can address the problem.

  • 4594 Accesses

Abstract

We recall that one-dimensional definite integral introduced in Sect. 4.1 is related to functions of a single variable. Here we shall generalise the idea of integration for functions of more than one variable. We start from the simplest case—integration of functions of two variables.

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

Chapter
USD 29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD 69.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

Notes

  1. 1.

    After all, in Sect. 4.2 we did not actually made use of the fact that what we sum corresponds to a one-dimensional integral; we simply considered the limit of an integral sum.

  2. 2.

    Note that on the left and right of the inequality prior to integration we had constant functions m kj and M kj which do not depend on x, so that integration simply corresponds to multiplying by \(\Delta y_{j}\) in either part.

  3. 3.

    We will use the following result: \(\int \sqrt{a^{2 } - t^{2}}dt = \frac{1} {2}\left [t\sqrt{a^{2 } - t^{2}} + a^{2}\arcsin \frac{t} {a}\right ] + C\), see Eq. ( 4.60).

  4. 4.

    Named after Carl Gustav Jacob Jacobi.

  5. 5.

    The corresponding indefinite integral cannot be represented by a combination of elementary analytical functions.

  6. 6.

    Once again, we need to use the integral of Eq. ( 4.60).

  7. 7.

    Although in this particular case, it does not affect the final zero result!

  8. 8.

    The strip was also discovered independently by Johann Benedict Listing.

  9. 9.

    Note that \(\mathbf{N} \sim \mathbf{r}\) as one would intuitively expect for the normal to a sphere!

  10. 10.

    Note that the Laplace equations here and in electrostatics differ by an unimportant factor of \(-4\pi\).

  11. 11.

    Note that it is customary in electrostatics to choose the minus sign when defining the potential.

Author information

Authors and Affiliations

Authors

Rights and permissions

Reprints and permissions

Copyright information

© 2016 Springer Science+Business Media, LLC

About this chapter

Cite this chapter

Kantorovich, L. (2016). Functions of Many Variables: Integration. In: Mathematics for Natural Scientists. Undergraduate Lecture Notes in Physics. Springer, New York, NY. https://doi.org/10.1007/978-1-4939-2785-2_6

Download citation

Publish with us

Policies and ethics