Topology and Geometry of Manifolds Assignment 8 for Math 546, Assignments of Mathematics

Math 546 assignment #8 for the topology and geometry of manifolds course, due on may 19, 2000. The assignment includes required and optional problems. Required problems involve showing the relationship between linear dependence of covectors and their wedge product, proving a lemma, and computing forms in cartesian and spherical coordinates. Optional problems outline an abstract approach to alternating tensors.

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Math 546 Topology and Geometry of Manifolds Spring 2000
Assignment #8
Due 5/19/2000
I. Required problems.
1. Let Vbe an n-dimensional vector space.
(a) Show that covectors ω1,...,ω
kon Vare linearly dependent if and only if
ω1∧···∧ωk=0.
(b) Suppose {ω1,...,ω
k}and {η1,...,η
k}are two collections of independent cov-
ectors on V. Show that the collections have the same span if and only if for
some nonzero constant c,
ω1∧···∧ ωk=
1∧···∧ηk.
(c) If ωΛkV,ωis said to be decomposable if ωcan be written ω=σ1∧···σk,
where each σiis a covector. Is every 2-covector on Vdecomposable? Your
answer will depend on the dimension of V. Give proof or counterexample.
2. Prove Lemma 11.10.
3. Define a 2-form on R3by
Ω=xdydz +ydzdx +zdxdy.
(a) Compute in spherical coordinates (ρ, ϕ, θ) (see Example 3.3).
(b) Compute d in both Cartesian and spherical coordinates and verify that both
expressions represent the same 3-form.
(c) Compute the restriction |S2=ιΩ, using coordinates (ϕ, θ), on the open
subset where these coordinates are defined.
(d) Show that |S2is nowhere zero.
II. Optional problems.
4. Let Vbe a finite-dimensional vector space. We have two ways to think about the
tensor space TkV: concretely, as the space of k-multilinear functionals on V;and
abstractly, as the tensor product space V⊗···⊗V. However, we have defined
alternating and symmetric tensors only in terms of the concrete definition. This
problem outlines an abstract approach to alternating tensors.
Let Adenote the subspace of V⊗···Vspanned by all elements of the form
αξξβfor covectors ξand arbitrary tensors α, β,andletAkVdenote
the quotient vector space V⊗···⊗ V/A. Define a wedge product on AkVby
ωη=π(eωeη), where π:V⊗···⊗V AkVis the projection, and eω,eηare
arbitrary tensors such that π(eω)=ω,π(eη)=η. Show that this wedge product is
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Math 546 Topology and Geometry of Manifolds Spring 2000 Assignment # Due 5/19/

I. Required problems.

  1. Let V be an n-dimensional vector space. (a) Show that covectors ω^1 ,... , ωk^ on V are linearly dependent if and only if ω^1 ∧ · · · ∧ ωk^ = 0. (b) Suppose {ω^1 ,... , ωk} and {η^1 ,... , ηk} are two collections of independent cov- ectors on V. Show that the collections have the same span if and only if for some nonzero constant c,

ω^1 ∧ · · · ∧ ωk^ = c η^1 ∧ · · · ∧ ηk.

(c) If ω ∈ ΛkV , ω is said to be decomposable if ω can be written ω = σ^1 ∧ · · · ∧ σk^ , where each σi^ is a covector. Is every 2-covector on V decomposable? Your answer will depend on the dimension of V. Give proof or counterexample.

  1. Prove Lemma 11.10.
  2. Define a 2-form Ω on R^3 by

Ω = x dy ∧ dz + y dz ∧ dx + z dx ∧ dy.

(a) Compute Ω in spherical coordinates (ρ, ϕ, θ) (see Example 3.3). (b) Compute dΩ in both Cartesian and spherical coordinates and verify that both expressions represent the same 3-form. (c) Compute the restriction Ω|S^2 = ι∗Ω, using coordinates (ϕ, θ), on the open subset where these coordinates are defined. (d) Show that Ω|S 2 is nowhere zero.

II. Optional problems.

  1. Let V be a finite-dimensional vector space. We have two ways to think about the tensor space T kV : concretely, as the space of k-multilinear functionals on V ; and abstractly, as the tensor product space V ∗^ ⊗ · · · ⊗ V ∗. However, we have defined alternating and symmetric tensors only in terms of the concrete definition. This problem outlines an abstract approach to alternating tensors. Let A denote the subspace of V ∗^ ⊗ · · · ⊗ V ∗^ spanned by all elements of the form α ⊗ ξ ⊗ ξ ⊗ β for covectors ξ and arbitrary tensors α, β, and let AkV denote the quotient vector space V ∗^ ⊗ · · · ⊗ V ∗/A. Define a wedge product on AkV by ω ∧ η = π(˜ω ⊗ η˜), where π : V ∗^ ⊗ · · · ⊗ V ∗^ −→ AkV is the projection, and ˜ω, η˜ are arbitrary tensors such that π(˜ω) = ω, π(˜η) = η. Show that this wedge product is

well defined, and that there is a unique isomorphism F : ΛkV −→ AkV such that the following diagram commutes:

ΛkV - AkV, F

T kV - V ∗^ ⊗ · · · ⊗ V ∗

?

Alt

?

π

and show that F takes the wedge product on ΛkV (defined by the Alt convention) to the wedge product on AkV. [This is another reason why the Alt convention for the wedge product is more natural than the determinant convention.]