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math105-s22:hw:hw11

HW 11

This weeks material is mostly conceptual, although the statement and proof in Pugh are all based on concrete formula.

  • Consider the generalized angular forms Ωn1\Omega_{n-1} defined on Rn\0\R^n \RM 0
    • For n=2n=2, we define Ω1=x2(x1dx2x2dx1)\Omega_1 = |x|^{-2} (x_1 dx_2 - x_2 dx_1)
    • For n=3n=3, we define Ω2=x3(x1dx2dx3x2dx1dx3+x3dx1dx2)\Omega_2 = |x|^{-3} (x_1 dx_2 \wedge dx_3 - x_2 dx_1 \wedge dx_3 + x_3 dx_1 \wedge dx_2)
    • Can you prove that dΩ1=0d \Omega_1=0, dΩ2=0d \Omega_2=0?
    • Can you write down the expression for the general nn? Or just prove the general case?
    • Consider the following 2-cell in R3\R^3 (it parametrized the unit sphere), γ:[0,1]2R3,(s,t)(sin(πs)cos(2πt),sin(πs)sin(2πt),cosπs)\gamma: [0,1]^2 \to \R^3, \quad (s,t) \mapsto (\sin (\pi s) \cos (2\pi t), \sin (\pi s) \sin (2\pi t), \cos \pi s) What is γΩ2\int_\gamma \Omega_2?
    • Suppose we use a different parametrization of S2S^2, the stereographic projection γ:R2R3,(a,b)(2a1+a2+b2,2b1+a2+b2,1+a2+b21+a2+b2) \gamma: \R^2 \mapsto \R^3, \quad (a,b) \mapsto (\frac{2a}{1+a^2+b^2}, \frac{2b}{1+a^2+b^2}, \frac{-1+a^2+b^2}{1+a^2+b^2}) Can you explain why γΩ2\int_{\gamma} \Omega_2 is the same as the previous one?
  • (Optional) Let γ1,γ2,[0,1]R3\gamma_1, \gamma_2, [0,1] \to \R^3 be two smooth loops, i.e. γi(0)=γi(1)\gamma_i(0)=\gamma_i(1) and γi(0)=γi(1)\gamma_i'(0) = \gamma_i'(1). Suppose they have disjoint images. Define a 2-cell ϕ:[0,1]2R3\phi: [0,1]^2 \to \R^3 by ϕ(s,t)=γ1(s)γ2(t)\phi(s,t) = \gamma_1(s) - \gamma_2(t). Prove that (4π)1ϕΩ2(4\pi)^{-1} \int_\phi \Omega_2 is an integer (hence insensitive to small perturbation of γ1,γ2\gamma_1, \gamma_2). This is called the linking number of two knots, and is a topological invariant of links. Can you compute some examples? Can you see its topological meaning?
    • Here is one example (maybe a bit degenerate): imagine two loops with very large radiu, one is lying on the xy plane, one is lying on the xz plane. Say, γ1\gamma_1 is given by z=0,(x+R1)2+y2=R2z=0, (x+R-1)^2 + y^2 = R^2; and γ2\gamma_2 is given by y=0,(xR+1)2+z2=R2y=0, (x-R+1)^2+z^2 = R^2. Can you compute the linking number? Can you picture what happens to the two circles if RR \to \infty?
    • That wasn't very easy to compute. Here is a simpler one: γ1\gamma_1 has the image of a loop z=0,x2+y2=r2z=0, x^2 + y^2 = r^2, with rr very small. And γ2\gamma_2 is the circle y=0,(xR)2+z2=R2y=0, (x-R)^2 + z^2 = R^2, with RR very large.
math105-s22/hw/hw11.txt · Last modified: 2022/04/15 16:27 by pzhou