Justin Solomon MIT, Spring 2017
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1 Justin Solomon MIT, Spring 2017 Some materials from Stanford CS 468, spring 2013 (Butscher & Solomon)
2 What is a curve?
3 A function?
4 Not a curve
5 Jams on accelerator
6
7 A curve is a set of points with certain properties. It is not a function.
8 Set of points that locally looks like a line.
9
10 Now this is OK!
11 Trace of parameterized curve Component functions
12 Geometric measurements should be invariant to changes of parameter.
13 On the board: Effect on velocity and acceleration.
14 On the board: Independence of parameter
15 Constant-speed parameterization
16
17 Differential geometry should be coordinate-invariant. Referring to x and y is a hack! (but sometimes convenient )
18 How do you characterize shape without coordinates?
19 On the board: Use coordinates from the curve to express its shape!
20
21 Fundamental theorem of the local theory of plane curves: k(s) characterizes a planar curve up to rigid motion.
22 Fundamental theorem of the local theory of plane curves: k(s) characterizes a planar curve up to rigid motion. Statement shorter than the name!
23 Image from DDG course notes by E. Grinspun Provides intuition for curvature
24 Binormal: T N Curvature: In-plane motion Torsion: Out-of-plane motion
25 Fundamental theorem of the local theory of space curves: Curvature and torsion characterize a 3D curve up to rigid motion.
26 Suspicion: Application to time series analysis? ML? C. Jordan, 1874 Gram-Schmidt on first n derivatives
27 What do these calculations look like in software?
28 Piecewise smooth approximations
29 What is the arc length of a cubic Bézier curve?
30 What is the arc length of a cubic Bézier curve?
31 Sad fact: Closed-form expressions rarely exist. When they do exist, they usually are messy.
32
33 Piecewise linear
34 Boring differential structure
35 THEOREM: As Δh 0, [insert statement].
36 THEOREM: As Δh 0, [insert statement].
37 Convergence to continuous theory Discrete behavior
38 Examine discrete theories of differentiable curves.
39 Examine discrete theories of differentiable curves.
40 Normal map from curve to S 1
41
42
43
44 A global theorem!
45
46
47
48
49 ( ) Total change in curvature
50 ( ) Total change in curvature
51 ( ) Total change in curvature
52 Same integrated curvature
53 Same integrated curvature
54 ( ) Total change in curvature
55 )( )( )( )( )( )( )(
56 decreases length the fastest.
57
58 Same behavior in the limit
59 Does discrete curvature converge in limit?
60 Does discrete curvature converge in limit? Questions: Type of convergence? Sampling? Class of curves?
61 Different discrete behavior Same convergence
62 Curves in 3D
63
64 NMR scanner Kinked alpha helix Structure Determination of Membrane Proteins Using Discrete Frenet Frame and Solid State NMR Restraints Achuthan and Quine Discrete Mathematics and its Applications, ed. M. Sethumadhavan (2006)
65 Discrete Frenet frame Bond and torsion angles (derivatives converge to κ and τ, resp.) Discrete frame introduced in: The resultant electric moment of complex molecules Eyring, Physical Review, 39(4): , 1932.
66 Discrete construction that works for fractal curves and converges in continuum limit. Discrete Frenet Frame, Inflection Point Solitons, and Curve Visualization with Applications to Folded Proteins Hu, Lundgren, and Niemi Physical Review E 83 (2011)
67
68 Discrete Elastic Rods Bergou, Wardetzky, Robinson, Audoly, and Grinspun SIGGRAPH
69
70 Normal part encodes twist
71 Punish turning the steering wheel
72 Punish turning the steering wheel
73 Punish non-tangent change in material frame
74 Punish non-tangent change in material frame Swapping m 1 and m 2 does not affect E twist!
75
76 Most relaxed frame
77 No twist ( parallel transport ) Most relaxed frame
78 Degrees of freedom for elastic energy: Shape of curve Twist angle θ
79 Upper index: dual Lower index: primal
80 Tangent unambiguous on edge
81 Turning angle Yet another curvature! Integrated curvature
82 Yet another curvature! Orthogonal to osculating plane, norm κ i Darboux vector
83 Convert to pointwise and integrate
84 Map tangent to tangent Preserve binormal Orthogonal
85
86 Note θ 0 can be arbitrary
87 \omit{physics}
88
89
90 One curve, three curvatures.
91 Easy theoretical object, hard to use.
92 Proper frames and DOFs go a long way.
93 Surfaces
94 Justin Solomon MIT, Spring 2017 Some materials from Stanford CS 468, spring 2013 (Butscher & Solomon)
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