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Pullback (differential geometry)

Pullback (differential geometry) 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 Pullback (differential geometry) rather than just read about it. In short: Let ϕ : M → N {\displaystyle \phi :M\to N} be a smooth map between smooth manifolds M {\displaystyle M} and N {\displaystyle N} . Then there is an associated linear map from the space of 1-forms on N {\displaystyle N} (the linear space of sections of the cotangent bundle) to the space of 1-forms on M {\displaystyle M} .

Key takeaways

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

Reference excerpt

Let ϕ : M → N {\displaystyle \phi :M\to N} be a smooth map between smooth manifolds M {\displaystyle M} and N {\displaystyle N} . Then there is an associated linear map from the space of 1-forms on N {\displaystyle N} (the linear space of sections of the cotangent bundle) to the space of 1-forms on M {\displaystyle M} . This linear map is known as the pullback (by ϕ {\displaystyle \phi } ), and is frequently denoted by ϕ ∗ {\displaystyle \phi ^{*}} . More generally, any covariant tensor field – in particular any differential form – on N {\displaystyle N} may be pulled back to M {\displaystyle M} using ϕ {\displaystyle \phi } . When the map ϕ {\displaystyle \phi } is a diffeomorphism, then the pullback, together with the pushforward, can be used to transform any tensor field from N {\displaystyle N} to M {\displaystyle M} or vice versa. In particular, if ϕ {\displaystyle \phi } is a diffeomorphism between open subsets of R n {\displaystyle \mathbb {R} ^{n}} and R n {\displaystyle \mathbb {R} ^{n}} , viewed as a change of coordinates (perhaps between different charts on a manifold M {\displaystyle M} ), then the pullback and pushforward describe the transformation properties of covariant and contravariant tensors used in more traditional (coordinate dependent) approaches to the subject. The idea behind the pullback is essentially the notion of precomposition of one function with another. However, by combining this idea in several different contexts, quite elaborate pullback operations can be constructed. This article begins with the simplest operations, then uses them to construct more sophisticated ones. Roughly speaking, the pullback mechanism (using precomposition) turns several constructions in differential geometry into contravariant functors.

Pullback of smooth functions and smooth maps Let ϕ : M → N {\displaystyle \phi :M\to N} be a smooth map between (smooth) manifolds M {\displaystyle M} and N {\displaystyle N} , and suppose f : N → R {\displaystyle f:N\to \mathbb {R} } is a smooth function on N {\displaystyle N} . Then the pullback of f {\displaystyle f} by ϕ {\displaystyle \phi } is the smooth function ϕ ∗ f {\displaystyle \phi ^{*}f} on M {\displaystyle M} defined by ( ϕ ∗ f ) ( x ) = f ( ϕ ( x ) ) {\displaystyle (\phi ^{*}f)(x)=f(\phi (x))} . Similarly, if f {\displaystyle f} is a smooth function on an open set U {\displaystyle U} in N {\displaystyle N} , then the same formula defines a smooth function on the open set ϕ − 1 ( U ) {\displaystyle \phi ^{-1}(U)} . (In the language of sheaves, pullback defines a morphism from the sheaf of smooth functions on N {\displaystyle N} to the direct image by ϕ {\displaystyle \phi } of the sheaf of smooth functions on M {\displaystyle M} .) More generally, if f : N → A {\displaystyle f:N\to A} is a smooth map from N {\displaystyle N} to any other manifold A {\displaystyle A} , then ( ϕ ∗ f ) ( x ) = f ( ϕ ( x ) ) {\displaystyle (\phi ^{*}f)(x)=f(\phi (x))} is a smooth map from M {\displaystyle M} to A {\displaystyle A} .

… excerpt ends here. Continue reading the full article.

Worked examples

Example 1 — a first encounter with Pullback (differential geometry)

Start with the simplest possible case. Write down what Pullback (differential geometry) 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 Pullback (differential geometry) 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 Pullback (differential geometry) 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 Pullback (differential geometry)

In research
Pullback (differential geometry) 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 Pullback (differential geometry) 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
Pullback (differential geometry) is common in secondary-school and first-year university syllabi. It links to neighbouring topics Differential geometry, Tensors, so understanding it makes those chapters shorter.
In everyday life
Look for Pullback (differential geometry) 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 Pullback (differential geometry) in 20 minutes

  1. Read the reference excerpt below once, without taking notes.
  2. Close the page and write down what Pullback (differential geometry) 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 Pullback (differential geometry) out loud to somebody else — or to Teacher Smith in the lgStudy chat.

Frequently asked questions

What is Pullback (differential geometry) in simple terms?

Let ϕ : M → N {\displaystyle \phi :M\to N} be a smooth map between smooth manifolds M {\displaystyle M} and N {\displaystyle N} . Then there is an associated linear map from the space of 1-forms on N {\displaystyle N} (the linear space of sections of the cotangent bundle) to the space of 1-forms on…

Why does Pullback (differential geometry) 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 Pullback (differential geometry)?

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 Pullback (differential geometry).

Tags

  • Differential geometry
  • Tensors

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