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NPTEL โ€“ Physics โ€“ Mathematical Physics - 1
Lecture 16
Symmetric, Skew Symmetric and orthogonal Matrices
Page 4 of 17
Joint initiative of IITs and IISc โ€“ Funded by MHRD
1) ๐ด๐‘‡ = ๐ด
2) ๐ด๐‘‡ = โˆ’๐ด
3) ๐ด๐‘‡ = ๐ดโˆ’1
โˆถ Symmetric
โˆถ Skew Symmetric
โˆถ Orthognal
Symmetric matrix : A square matrix A is said to be symmetric if ๐ด๐‘–๐‘— = ๐ด๐‘—๐‘– for all i and j
where (๐‘–, ๐‘—)๐‘กโ„Ž element of the matrix denotes the intersection of ๐‘–๐‘กโ„Ž and ๐‘—๐‘กโ„Ž column
and similarly ๐ด๐‘—๐‘– denotes the intersection of ๐‘—๐‘กโ„Ž row and ๐‘–๐‘กโ„Ž column of the matrix A.
Example of such a matrix is,
1 2 5
[๐ด] = [2 5 โˆ’ 7]
5 โˆ’ 7 3
Here ๐ด12 = ๐ด21 = 2; ๐ด13 = ๐ด31 = 5, ๐ด23 = ๐ด32 = โˆ’7
Similarly an example of a skew symmetric matrix is given as
0 โˆ’ 5 4
[๐ด] = [5 0 โˆ’ 1]
โˆ’4 1 0
Here ๐ด๐‘–๐‘— = โˆ’๐ด๐‘—๐‘–
It can easily be shown that ๐ด๐‘‡ = โˆ’๐ด
Similarly the example of an orthogonal matrix is
๐ด = 2โ„3
โ„3 โˆ’ โ„3 โ„3
โˆ’ 1โ„3
( 2
3
2โ„3
1โ„3 )
1 2 2
โˆ’ 2โ„3 .
โ„
One can check ๐ด๐‘‡๐ด = 1
Or ๐ด๐‘‡ = ๐ดโˆ’1
NPTEL โ€“ Physics โ€“ Mathematical Physics - 1
Properties of different matrices
1. Every skew symmetric matrix has all the main diagonal elements zero.
๐ด๐‘‡ = โˆ’๐ด.
๐ด + ๐ด๐‘‡ = 0. โ‡’ ๐ด๐‘–๐‘— + ๐ด๐‘—๐‘– = 0.
For ๐‘— = ๐‘–, ๐ด๐‘–๐‘— = 0
2.Any real square matrix A may be written as a sum of a symmetric matrix R and a
skew-symmetric matrix S, where,
๐‘… = 1
(๐ด + ๐ด๐‘‡), ๐‘† = 1
(๐ด โˆ’ ๐ด๐‘‡)
2 2
๐ด = ๐‘… + ๐‘†.
3.Consider a square matrix A that satisfies a matrix equation of the form,
๐ด๐‘ฃ๐‘– = ๐œ†๐‘– ๐‘ฃ๐‘–
where ๐œ†๐‘–โ€™s are called the eigenvalue and ๐‘ฃ๐‘– are eigenvector. Here ๐‘ฃ๐‘– โ‰  0, though ๐œ†
๐‘– can be zero. Further the eigenvectors are invariant for every power of A, Or in other
words,
๐ด๐‘›๐‘ฃ๐‘– = ๐œ†๐‘–
๐‘›
๐‘ฃ๐‘–
which can easily be shown as follows,
๐ด๐‘ฃ๐‘– = ๐œ†๐‘–๐‘ฃ๐‘–
๐ด(๐ด๐‘ฃ๐‘–) = ๐ด(๐œ†๐‘–๐‘ฃ๐‘–) = ๐œ†๐‘–๐ด๐‘ฃ๐‘– = ๐œ†๐‘–
2
๐‘ฃ๐‘–
The proof follows by induction.
The determination of the eigenvalues will be done shortly.
Page 5 of 17
Joint initiative of IITs and IISc โ€“ Funded by MHRD
Page 6 of 17
Joint initiative of IITs and IISc โ€“ Funded by MHRD
NPTEL โ€“ Physics โ€“ Mathematical Physics - 1
4. The eigenvalues of a symmetric matrix are real. The eigenvalues of
a skew symmetric matrix are pure imaginary or zero.
Example The matrix [ ]
3 4
1 3
๐‘‘๐‘’๐‘ก | 3 โˆ’ ๐œ† | = 0
1 3 โˆ’ ๐œ†
4
(3โˆ’๐œ†)2 = 4.
3 โˆ’๐œ† = ยฑ2 โ‡’ ๐œ† = 1,5 ; that is, they are real. But the matrix is not
symmetric.
So the above statement is true only in one direction. i.e. all symmetric
matrices have real eigenvalues, but all matrices with real eigenvalues
are not necessarily symmetric especially if they have same diagonal
entries.
Example
In another example, one can show that for skew symmetric matrices, the
eigenvalues are purely imaginary.
๐ด = [ 0 1 ]
โˆ’1 0
det(๐ด โˆ’ ๐œ†๐ผ) = 0
๐œ† = ยฑ๐‘–

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NPTEL Physics Mathematical Properties Matrices

  • 1. NPTEL โ€“ Physics โ€“ Mathematical Physics - 1 Lecture 16 Symmetric, Skew Symmetric and orthogonal Matrices Page 4 of 17 Joint initiative of IITs and IISc โ€“ Funded by MHRD 1) ๐ด๐‘‡ = ๐ด 2) ๐ด๐‘‡ = โˆ’๐ด 3) ๐ด๐‘‡ = ๐ดโˆ’1 โˆถ Symmetric โˆถ Skew Symmetric โˆถ Orthognal Symmetric matrix : A square matrix A is said to be symmetric if ๐ด๐‘–๐‘— = ๐ด๐‘—๐‘– for all i and j where (๐‘–, ๐‘—)๐‘กโ„Ž element of the matrix denotes the intersection of ๐‘–๐‘กโ„Ž and ๐‘—๐‘กโ„Ž column and similarly ๐ด๐‘—๐‘– denotes the intersection of ๐‘—๐‘กโ„Ž row and ๐‘–๐‘กโ„Ž column of the matrix A. Example of such a matrix is, 1 2 5 [๐ด] = [2 5 โˆ’ 7] 5 โˆ’ 7 3 Here ๐ด12 = ๐ด21 = 2; ๐ด13 = ๐ด31 = 5, ๐ด23 = ๐ด32 = โˆ’7 Similarly an example of a skew symmetric matrix is given as 0 โˆ’ 5 4 [๐ด] = [5 0 โˆ’ 1] โˆ’4 1 0 Here ๐ด๐‘–๐‘— = โˆ’๐ด๐‘—๐‘– It can easily be shown that ๐ด๐‘‡ = โˆ’๐ด Similarly the example of an orthogonal matrix is ๐ด = 2โ„3 โ„3 โˆ’ โ„3 โ„3 โˆ’ 1โ„3 ( 2 3 2โ„3 1โ„3 ) 1 2 2 โˆ’ 2โ„3 . โ„ One can check ๐ด๐‘‡๐ด = 1 Or ๐ด๐‘‡ = ๐ดโˆ’1
  • 2. NPTEL โ€“ Physics โ€“ Mathematical Physics - 1 Properties of different matrices 1. Every skew symmetric matrix has all the main diagonal elements zero. ๐ด๐‘‡ = โˆ’๐ด. ๐ด + ๐ด๐‘‡ = 0. โ‡’ ๐ด๐‘–๐‘— + ๐ด๐‘—๐‘– = 0. For ๐‘— = ๐‘–, ๐ด๐‘–๐‘— = 0 2.Any real square matrix A may be written as a sum of a symmetric matrix R and a skew-symmetric matrix S, where, ๐‘… = 1 (๐ด + ๐ด๐‘‡), ๐‘† = 1 (๐ด โˆ’ ๐ด๐‘‡) 2 2 ๐ด = ๐‘… + ๐‘†. 3.Consider a square matrix A that satisfies a matrix equation of the form, ๐ด๐‘ฃ๐‘– = ๐œ†๐‘– ๐‘ฃ๐‘– where ๐œ†๐‘–โ€™s are called the eigenvalue and ๐‘ฃ๐‘– are eigenvector. Here ๐‘ฃ๐‘– โ‰  0, though ๐œ† ๐‘– can be zero. Further the eigenvectors are invariant for every power of A, Or in other words, ๐ด๐‘›๐‘ฃ๐‘– = ๐œ†๐‘– ๐‘› ๐‘ฃ๐‘– which can easily be shown as follows, ๐ด๐‘ฃ๐‘– = ๐œ†๐‘–๐‘ฃ๐‘– ๐ด(๐ด๐‘ฃ๐‘–) = ๐ด(๐œ†๐‘–๐‘ฃ๐‘–) = ๐œ†๐‘–๐ด๐‘ฃ๐‘– = ๐œ†๐‘– 2 ๐‘ฃ๐‘– The proof follows by induction. The determination of the eigenvalues will be done shortly. Page 5 of 17 Joint initiative of IITs and IISc โ€“ Funded by MHRD
  • 3. Page 6 of 17 Joint initiative of IITs and IISc โ€“ Funded by MHRD NPTEL โ€“ Physics โ€“ Mathematical Physics - 1 4. The eigenvalues of a symmetric matrix are real. The eigenvalues of a skew symmetric matrix are pure imaginary or zero. Example The matrix [ ] 3 4 1 3 ๐‘‘๐‘’๐‘ก | 3 โˆ’ ๐œ† | = 0 1 3 โˆ’ ๐œ† 4 (3โˆ’๐œ†)2 = 4. 3 โˆ’๐œ† = ยฑ2 โ‡’ ๐œ† = 1,5 ; that is, they are real. But the matrix is not symmetric. So the above statement is true only in one direction. i.e. all symmetric matrices have real eigenvalues, but all matrices with real eigenvalues are not necessarily symmetric especially if they have same diagonal entries. Example In another example, one can show that for skew symmetric matrices, the eigenvalues are purely imaginary. ๐ด = [ 0 1 ] โˆ’1 0 det(๐ด โˆ’ ๐œ†๐ผ) = 0 ๐œ† = ยฑ๐‘–