Lecture Notes for 120 - UCLA Department of Mathematics
Lecture Notes for 120 - UCLA Department of Mathematics
Lecture Notes for 120 - UCLA Department of Mathematics
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4.4. THE FIRST FUNDAMENTAL FORM 88<br />
The first fundamental <strong>for</strong>m is the symmetric positive definite <strong>for</strong>m that comes<br />
from the matrix<br />
[I] = ⇥ ⇤<br />
@q t ⇥ @q<br />
⇤<br />
=<br />
=<br />
@q<br />
@u @v @u<br />
apple @q<br />
@u · @q @q<br />
@u @u · @q<br />
@v<br />
@q<br />
@v · @q @q<br />
@u @v · @q<br />
@v<br />
apple<br />
guu g uv<br />
g vu g vv<br />
For a curve the analogous term would simply be the square <strong>of</strong> the speed<br />
✓ ◆ t dq dq<br />
dt dt = dq<br />
dt · dq<br />
dt .<br />
The first fundamental <strong>for</strong>m dictates how one computes dot products <strong>of</strong> vectors<br />
tangent to the surface assuming they are expanded according to the basis @q<br />
@u , @q<br />
@v<br />
@q<br />
@v<br />
X = X u @q @q<br />
+ Xv<br />
@u @v = ⇥ @q<br />
@u<br />
Y = Y u @q<br />
@u + Y v @q<br />
@v = ⇥ @q<br />
@u<br />
@q<br />
@v<br />
@q<br />
@v<br />
⇤ apple X u<br />
X v<br />
⇤ apple Y u<br />
Y v<br />
I(X, Y ) = ⇥ X u X ⇤ apple apple v g uu g uv Y<br />
u<br />
g vu g vv Y v<br />
= ⇥ X u X v ⇤⇥ @q<br />
@u<br />
=<br />
✓ ⇥ @q<br />
@u<br />
= X t Y<br />
= X · Y<br />
@q<br />
@v<br />
⇤ apple X u<br />
X v<br />
@q<br />
@v<br />
⇤ t ⇥ @q<br />
@u<br />
◆ t ✓ ⇥ @q<br />
@u<br />
@q<br />
@v<br />
@q<br />
@v<br />
⇤ apple Y u<br />
Y v<br />
⇤ apple Y u<br />
In particular, we see that while the metric coefficients g w1w 2<br />
depend on our parametrization.<br />
The dot product I(X, Y ) <strong>of</strong> two tangent vectors remains the same if we change<br />
parameters. Note that I stands <strong>for</strong> the bilinear <strong>for</strong>m I(X, Y ) which does not depend<br />
on parametrizations, while [I] is the matrix representation <strong>for</strong> a fixed parametrization.<br />
Our first observation is that the normalization factor<br />
can be computed<br />
from [I] .<br />
Y v<br />
@q<br />
@u ⇥ @q<br />
@v<br />
Definition 4.4.1. The area <strong>for</strong>m <strong>of</strong> a parametrized surface is given by<br />
p<br />
det [I]<br />
◆<br />
The next Lemma shows that this is given by the area <strong>of</strong> the parallelogram<br />
spanned by @q<br />
@u , @q<br />
@v .<br />
Lemma 4.4.2. We have<br />
@q<br />
@u ⇥ @q<br />
@v<br />
2<br />
=det[I]=g uu g vv (g uv ) 2