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Taha Sochi - Solutions of Exercises of Principles of Tensor Calculus

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Taha Sochi Solutions of Exercises of Principles of Tensor Calculus
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This book contains the solutions of all the exercises of my book: Principles of Tensor Calculus. These solutions are sufficiently simplified and detailed for the benefit of readers of all levels particularly those at introductory levels.

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Preface
This book contains the solutions of all the exercises of my book:Principles of Tensor Calculus. These solutions are sufficientlysimplified and detailed for the benefit of readers of all levelsparticularly those at introductory levels.
Taha Sochi
London, September 2018
Table of Contents
Nomenclature
In the following list, we define the commonsymbols, notations and abbreviations which are used in the book as aquick reference for the reader.
nabla differential operator
; and ;covariant and contravariant differential operators
fgradient of scalar f
Adivergence of tensor A
Acurl of tensor A
, ii , iiLaplacian operator
v , ivjvelocity gradient tensor
, (subscript)partial derivative with respect to following index(es)
; (subscript)covariant derivative with respect to following index(es)
hat (e.g. Ai , Ei )physical representation or normalized vector
bar (e.g. ui , Ai )transformed quantity
inner or outer product operator
perpendicular to
1D, 2D, 3D, n Done-, two-, three-, n -dimensional
tabsolute derivative operator with respect to t
i and ipartial derivative operator with respect to ith variable
;icovariant derivative operator with respect to ith variable
[ij,k]Christoffel symbol of 1st kind
Aarea
B , BijFinger strain tensor
B1 , Bij1Cauchy strain tensor
Ccurve
Cnof class n
d , didisplacement vector
detdeterminant of matrix
diag [ ]diagonal matrix with embraced diagonal elements
drdifferential of position vector
dslength of infinitesimal element of curve
darea of infinitesimal element of surface
dvolume of infinitesimal element of space
eiith vector of orthonormal vector set (usually Cartesian basis set)
er,e,ebasis vectors of spherical coordinate system
err,er,,eunit dyads of spherical coordinate system
e,e,ezbasis vectors of cylindrical coordinate system
e,e,,ezzunit dyads of cylindrical coordinate system
E , Eijfirst displacement gradient tensor
Ei , Eiith covariant and contravariant basis vectors
iith orthonormalized covariant basis vector
Eq./Eqs.Equation/Equations
gdeterminant of covariant metric tensor
gmetric tensor
gij , gij , g jicovariant, contravariant and mixed metric tensor or its components
g11,g12,gnncoefficients of covariant metric tensor
g11,g12,gnncoefficients of contravariant metric tensor
hiscale factor for ith coordinate
iffif and only if
JJacobian of transformation between two coordinate systems
JJacobian matrix of transformation between two coordinate systems
J1inverse Jacobian matrix of transformation
Llength of curve
n , ninormal vector to surface
Ppoint
P(n,k)k -permutations of n objects
qiith coordinate of orthogonal coordinate system
qiith unit basis vector of orthogonal coordinate system
rposition vector
Ricci curvature scalar
Rij , R ijRicci curvature tensor of 1st and 2nd kind
Rijkl , R ijklRiemann-Christoffel curvature tensor of 1st and 2nd kind
r,,coordinates of spherical coordinate system
Ssurface
S , Sijrate of strain tensor
S , Sijvorticity tensor
ttime
T (superscript)transposition of matrix
T , Titraction vector
trtrace of matrix
uiith coordinate of general coordinate system
v , vivelocity vector
Vvolume
wweight of relative tensor
xi , xiith Cartesian coordinate
x i , xiith Cartesian coordinate of particle at past and present times
x,y,zcoordinates of 3D space (mainly Cartesian)
, ijinfinitesimal strain tensor
rate of strain tensor
kijChristoffel symbol of 2nd kind
Kronecker delta tensor
ij , ij , jicovariant, contravariant and mixed ordinary Kronecker delta
ijkl , ijklmn , i1inj1jngeneralized Kronecker delta in 2D, 3D and n D space
, ijsecond displacement gradient tensor
ij , ijk , i1incovariant relative permutation tensor in 2D, 3D and n D space
ij , ijk , i1incontravariant relative permutation tensor in 2D, 3D and n D space
ij , ijk , i1incovariant absolute permutation tensor in 2D, 3D and n D space
ij , ijk , i1incontravariant absolute permutation tensor in 2D, 3D and n D space
,coordinates of plane polar coordinate system
,,zcoordinates of cylindrical coordinate system
, ijstress tensor
vorticity tensor
region of space
Note: due to the restrictions on the availability and visibilityof symbols in the mobi format, as well as similar formatting issues, weshould draw the attention of the ebook readers to the following points:
1. Bars over symbols, which are used in theprinted version, were replaced by tildes. However, for convenience wekept using the terms barred and unbarred in the text to refer tothe symbols with and without tildes.
2. The square root symbol in mobi is ( ) where the argument is contained inside the parentheses. For example, the square root of g is symbolized as ( g ) .
3. In the mobi format, superscripts areautomatically displayed before subscripts unless certain measures aretaken to force the opposite which may distort the look of the symboland may not even be the required format when the superscripts andsubscripts should be side by side which is not possible in the mobitext and live equations. Therefore, for convenience and aestheticreasons we only forced the required order of the subscripts andsuperscripts or used imaged symbols when it is necessary; otherwise weleft the symbols to be displayed according to the mobi choice althoughthis may not be ideal like displaying the Christoffel symbols of thesecond kind as: ijk or the generalized Kronecker delta as:
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