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Keller–Osserman conditions

Keller–Osserman conditions is a mathematics topic covered in the lgStudy science library. This page brings together a partial reference excerpt, illustrations, worked examples, real-world applications and a short study plan, so you can understand Keller–Osserman conditions rather than just read about it. In short: In differential geometry and partial differential equations, the Keller–Osserman conditions are conditions on a single-variable function f that preclude the existence of solutions to the elliptic partial differential equation (PDE) Δ u = f ( u ) . {\displaystyle \Delta u=f(u).} In particular, the fast growth and monotonicity of f is incompatible with the existence of global solutions. For example, the conditions imp…

Key takeaways

  • Keller–Osserman conditions belongs to mathematics; place it in that map before memorising details.
  • Learn the definition first, then one example that makes the definition concrete.
  • Connect Keller–Osserman conditions to a quantity you can measure, compute or draw — that is where exam questions come from.
  • Reproduce the core statement of Keller–Osserman conditions from memory before moving on to harder problems.

Reference excerpt

In differential geometry and partial differential equations, the Keller–Osserman conditions are conditions on a single-variable function f that preclude the existence of solutions to the elliptic partial differential equation (PDE)

Δ u = f ( u ) . {\displaystyle \Delta u=f(u).}

In particular, the fast growth and monotonicity of f is incompatible with the existence of global solutions. For example, the conditions imply that there is no twice-differentiable function u : R n → R {\displaystyle u:\mathbb {R} ^{n}\to \mathbb {R} } such that

∂ 2 u ∂ x 1 2 + ⋯ + ∂ 2 u ∂ x n 2 ≥ e u . {\displaystyle {\frac {\partial ^{2}u}{\partial x_{1}^{2}}}+\cdots +{\frac {\partial ^{2}u}{\partial x_{n}^{2}}}\geq e^{u}.}

They were found independently in 1957 by Joseph Keller and Robert Osserman.

Motivation, applications and generalization Keller's motivation for this problem was based in application to electrohydrodynamics. Osserman's motivation, by contrast, was from differential geometry, with the observation that the scalar curvature of the Riemannian metric e2u(dx2 + dy2) on the plane is given by

− e − 2 u ( ∂ 2 u ∂ x 2 + ∂ 2 u ∂ y 2 ) . {\displaystyle -e^{-2u}{\Big (}{\frac {\partial ^{2}u}{\partial x^{2}}}+{\frac {\partial ^{2}u}{\partial y^{2}}}{\Big )}.}

An application of Osserman's non-existence theorem then shows that any simply-connected two-dimensional smooth Riemannian manifold whose scalar curvature is negative and bounded away from zero is not conformally equivalent to the standard plane. Osserman's method was to construct special solutions of the PDE which would facilitate application of the maximum principle. In particular, he showed that for any real number a there exists a rotationally symmetric solution on some ball which takes the value a at the center and diverges to infinity near the boundary. The maximum principle shows, by the monotonicity of f, that a hypothetical global solution u would satisfy u(x) < a for any x and any a, which is impossible. By a different maximum principle-based method, Shiu-Yuen Cheng and Shing-Tung Yau generalized the Keller–Osserman non-existence result, in part by a generalization to the setting of a Riemannian manifold. This was, in turn, an important piece of one of their resolutions of the Calabi–Jörgens problem on rigidity of affine hyperspheres with nonnegative mean curvature.

References

Further reading Osserman, Robert (1957). "On the inequality Δu≥f(u)". Pacific Journal of Mathematics. 7 (4): 1641–1647. doi:10.2140/pjm.1957.7.1641. Ghergu, Marius and Radulescu, Vicentiu. Nonlinear PDEs: Mathematical models in biology, chemistry and population genetics. Springer Science & Business Media, 2011. ISBN 978-3642269844 Alías, Luis J.; Mastrolia, Paolo; and Rigoli, Marco. Maximum principles and geometric applications. Cham: Springer International Publishing, 2016. ISBN 978-3319796055

Worked examples

Example 1 — a first encounter with Keller–Osserman conditions

Start with the simplest possible case. Write down what Keller–Osserman conditions claims or describes in one sentence, then invent the smallest concrete situation in which that sentence is true. In mathematics, the smallest case is usually a single object, a single equation or a single measurement. Check that every symbol or term in your sentence has a meaning in that case.

Example 2 — changing one variable

Take the situation from Example 1 and change exactly one quantity: double it, halve it, or set it to zero. Predict what should happen to Keller–Osserman conditions before you calculate. Comparing your prediction with the result is the fastest way to find out whether you understand the idea or only the words.

Example 3 — an exam-style question

Typical questions about Keller–Osserman conditions ask you to (a) state it precisely, (b) apply it to given data, and (c) explain a limitation. Practise writing all three answers in under five minutes; the third part is what separates a full-mark answer from an average one.

Applications of Keller–Osserman conditions

In research
Keller–Osserman conditions appears in mathematics research whenever the underlying quantities have to be modelled precisely. Papers usually cite it as a starting assumption and then explore where it breaks down.
In technology and industry
Engineering practice reuses Keller–Osserman conditions in design rules, simulations and safety margins. Knowing the idea lets you read a specification sheet and understand why the numbers look the way they do.
In the classroom
Keller–Osserman conditions is common in secondary-school and first-year university syllabi. It links to neighbouring topics Differential geometry, Electrodynamics, Partial differential equations, so understanding it makes those chapters shorter.
In everyday life
Look for Keller–Osserman conditions outside the textbook — in sport, cooking, traffic, electronics or the sky above you. An example you found yourself is remembered far longer than one you were given.
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How to study Keller–Osserman conditions in 20 minutes

  1. Read the reference excerpt below once, without taking notes.
  2. Close the page and write down what Keller–Osserman conditions means in your own words.
  3. Compare your version with the excerpt and mark what you missed.
  4. Work through the three examples above with pen and paper.
  5. Explain Keller–Osserman conditions out loud to somebody else — or to Teacher Smith in the lgStudy chat.

Frequently asked questions

What is Keller–Osserman conditions in simple terms?

In differential geometry and partial differential equations, the Keller–Osserman conditions are conditions on a single-variable function f that preclude the existence of solutions to the elliptic partial differential equation (PDE) Δ u = f ( u ) . {\displaystyle \Delta u=f(u).} In particular, the f…

Why does Keller–Osserman conditions matter?

Because it connects several mathematics ideas at once: it gives you a definition you can apply, a quantity you can calculate, and a way to check whether a result is plausible.

How should I study Keller–Osserman conditions?

Read the excerpt, restate it from memory, then work through the examples and applications listed on this page. The five-step study plan above takes about twenty minutes.

What does this page cover?

It gives you a compact reference excerpt plus original lgStudy explanations, examples, applications and study material on Keller–Osserman conditions.

Tags

  • Differential geometry
  • Electrodynamics
  • Partial differential equations

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