- #1
atwood
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Homework Statement
A two dimensional space has a metric tensor field
[tex]g=dq^1 \otimes dq^1 + 2 dq^1 \otimes dq^2 + 2dq^2 \otimes dq^1 + 3dq^2 \otimes dq^2[/tex].
With the help of g, find the covariant components of the contravariant vector field
[tex]\textbf{v}=3\partial _1 -4\partial _2[/tex]
The Attempt at a Solution
Not much here as I don't really understand how this works.
g11=1, g12=2, g21=2, g22=3
[tex]\begin{center}G=\left(\begin{array}{ll} 1 & 2 \\ 2 & 3 \end{array}\right) \Rightarrow
G^{-1}=\left(\begin{array}{ll} {-3} & \ 2 \\ \ 2 & {-1} \end{array}\right)\end{center}[/tex]
g11=-3, g12=2, g21=2, g22=-1
Now the covariant components ai of v are given from the contravariant components ai like this:
a1=a1g11+a1g12=3*(-3)+3*2=-3
a2=a2g21+a2g22=(-4)*2+(-4)*(-1)=-4
So [tex]\textbf{v}=-3dq^1 -4dq^2[/tex]
Does this make any sense at all?