How to Construct a Smooth Pullback Function on a 2-Sphere Manifold
Problem
Find g ∈ C∞(S²) such that f*α = gω₀, where α is a 2-form in R³ and f is a map from the 2-sphere to R³, with ω₀ being the standard volume form on the sphere
🎯 What You'll Learn
- Understand pullback of differential forms
- Apply coordinate transformations in topology
- Compute determinants on manifolds
Prerequisites: Differential geometry, Multivariate calculus, Linear algebra
💡 Quick Summary
This problem asks you to find a smooth function g that relates a pullback 2-form to the standard volume form on a 2-sphere. The key insight is that any 2-form on a 2-dimensional manifold can be uniquely written as a function times the volume form, so we need to find what that scaling function is. The approach involves pulling back a 2-form α from ℝ³ to the sphere S² via a map f, then expressing this pullback in terms of the sphere's natural volume form ω₀. The solution is beautifully simple: g(p) equals the pullback form divided by the standard volume form at each point, which essentially measures how the pullback "stretches" or "shrinks" the natural volume element of the sphere. This elegant result shows how differential geometry lets us compare geometric quantities across different spaces!
Step-by-Step Explanation
Hello! This is a beautiful problem that connects differential geometry, topology, and the theory of differential forms. Let's work through it together step by step!
1. What We're Solving:
We need to find a smooth function g on the 2-sphere S² such that when we pull back a 2-form α from ℝ³ via a map f: S² → ℝ³, the result equals g times the standard volume form ω₀ on the sphere.2. The Approach:
This problem is fundamentally about understanding how differential forms behave under pullbacks and how they relate to volume forms. The key insight is that any 2-form on a 2-dimensional manifold (like S²) can be written as a function times the volume form. We need to find what that function is!Think of it this way: we're asking "how does the pullback f*α compare to the natural volume element on the sphere?" The function g tells us the ratio between these two quantities at each point.
3. Step-by-Step Solution:
Step 1: Understand what we have
- f: S² → ℝ³ is our map from the sphere into 3-space
- α is a 2-form on ℝ³
- ω₀ is the standard volume form on S² (this gives us area measurements)
- f*α is the pullback of α to S²
Step 3: Set up coordinates Let's use spherical coordinates (θ, φ) on S². The standard volume form is: ω₀ = sin φ dθ ∧ dφ
Step 4: Express the pullback The pullback f*α will also be a 2-form on S², so we can write: f*α = h(θ,φ) dθ ∧ dφ
for some function h.
Step 5: Find the relationship Since f*α = gω₀, we have: h(θ,φ) dθ ∧ dφ = g(θ,φ) sin φ dθ ∧ dφ
Step 6: Solve for g Comparing coefficients: g(θ,φ) = h(θ,φ)/sin φ
4. The Answer:
The function g at any point p ∈ S² is given by:g(p) = (f*α)(p) / ω₀(p)
In coordinates: g(θ,φ) = [coefficient of dθ ∧ dφ in f*α] / sin φ
More conceptually: g measures the ratio between the "volume density" that α induces on the sphere (via the pullback) and the natural volume density of the sphere itself.
5. Memory Tip:
Remember this as the "volume ratio function" - g tells you how much the pullback form f*α stretches or shrinks the natural volume element of the sphere at each point. When g > 1, the pullback is "concentrating" more volume there; when g < 1, it's "diluting" it!This problem beautifully illustrates how pullbacks allow us to compare geometric quantities on different spaces. You're essentially asking: "If I project the 2-form α onto the sphere via f, how does it compare to the sphere's natural area element?" Pretty elegant! 🌟
⚠️ Common Mistakes to Avoid
- Incorrectly computing pullback of differential forms
- Misunderstanding coordinate transformations
- Failing to track sign changes in coordinate systems
This explanation was generated by AI. While we work hard to be accurate, mistakes can happen! Always double-check important answers with your teacher or textbook.

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