468 CHAPTER 25. CURVILINEAR COORDINATES

The proof of the remaining formula in 25.10 is similar.To verify 25.11,

gi jg jk = ei ·e je j ·ek =((ei ·e j)e j

)·ek = ei ·ek = δ

ik.

This shows the two determinants in 25.12 are non zero because the two matrices are in-verses of each other. It only remains to verify that one of these is greater than zero. Lettingei = a j

i i j = biji

j, we see that since i j = i j,a ji = bi

j. Therefore,

ei ·e j = ari ir ·b j

kik = ar

i bjkδ

kr = ak

i b jk = ak

i akj.

It follows that for G the matrix whose i jth entry is ei ·e j, G = AAT where the ikth entry ofA is ak

i . Therefore, det(G) = det(A)det(AT)= det(A)2 > 0. It follows from 25.11 that if

H is the matrix whose i jth entry is gi j, then GH = I and so H = G−1 and

det(G)det(G−1)= det

(gi j)det(G) = 1.

Therefore, det(G−1

)> 0 also. ■

Note that det(AAT

)≥ 0 always, because the eigenvalues are nonnegative.

As noted above, we have the following definition.

Definition 25.1.7 The matrix (gi j) = G is called the metric tensor.

25.2 Exercises1. Let e1 = i+j,e2 = i−j,e3 = j+k. Find e1,e2,e3, (gi j) ,

(gi j). If

v = i+2j+k, find vi and v j, the contravariant and covariant components of thevector.

2. Let e1 = 2i+j,e2 = i−2j,e3 = k. Find e1,e2,e3, (gi j) ,(gi j). If

v = 2 i− 2j+k, find vi and v j, the contravariant and covariant components of thevector.

3. Suppose e1,e2,e3 have the property that ei ·e j = 0 whenever i ̸= j. Show the sameis true of the dual basis and that in fact, ei is a multiple of ei.

4. Let e1,· · · ,e3 be a basis for Rn and let v = viei = viei,w= w je j = w je

j be twovectors. Show

v ·w= gi jviw j = gi jviw j.

5. Show if {ei}3i=1 is a basis in R3

e1 =e2×e3

e2×e3 ·e1, e2 =

e1×e2

e1×e3 ·e2, e3 =

e1×e2

e1×e2 ·e3.

6. Let {ei}ni=1 be a basis and define

e∗i ≡ei

|ei|, e∗i ≡ ei |ei| .

Show e∗i ·e∗j = δij.

468 CHAPTER 25. CURVILINEAR COORDINATESThe proof of the remaining formula in 25.10 is similar.To verify 25.11,gig =e! -ele;-ex = ((e'-e/)e;)-eg =e -E = 5j..This shows the two determinants in 25.12 are non zero because the two matrices are in-verses of each other. It only remains to verify that one of these is greater than zero. Lettinge; = aji; = bit, we see that since 1; = i/,a/ = bi. Therefore,e;-e; = ahi, -bli® = ath] 5 = akb] = dja',.It follows that for G the matrix whose ij‘” entry is e;-e j,G=AA! where the ik'” entry ofA is a‘. Therefore, det (G) = det (A) det (A?) = det (A)* > 0. It follows from 25.11 that ifH is the matrix whose ij’” entry is g’/, then GH =/ and so H = G~! anddet (G) det (G~') = det (g’/) det(G) = 1.Therefore, det (G~') > 0 also. llNote that det (AA‘) > 0 always, because the eigenvalues are nonnegative.As noted above, we have the following definition.Definition 25.1.7 The matrix (g;;) = G is called the metric tensor.25.2 Exercises1. Lete; =t+J,e, =1—j,e3; =j +k. Find e!,e7,e°, (gif); (g'/) Ifv=1+2j +k, find v' and v;, the contravariant and covariant components of thevector.2. Let e! = %+j,e = i-2j,e° =k. Find €1,€2,€3, (gi;) ; (g'/) Ifv = 21-23 +k, find v’ and v;, the contravariant and covariant components of thevector.3. Suppose e€),€2,e3 have the property that e;-e; = 0 whenever i 4 j. Show the sameis true of the dual basis and that in fact, e' isa multiple of e;.4. Let e1,---,e3 be a basis for R” and let v = vie; = vje!,w = wie; = w el be twovectors. Showvw = gijvw! = 8" yw.5. Show if {e;}?_, is a basis in R31 e2 X €&3 2 e,; xe2 e- e; xe2= e= = ——.e€7 X €3-e]” e€; X€3-€)" e€, X €2:e36. Let {e;}/_, be a basis and definee; . F=—,e"=e'le;|.*ejlei|Show e*?. e; = 5i.