Engineering Mathematics Formulas for GATE Exam

# Engineering Mathematics Formulas for GATE Exam | Engineering Mathematics - Civil Engineering (CE) PDF Download

``` Page 1

If i, j, k are orthonormal vectors and A = A
x
i + A
y
j + A
z
k thenjAj
2
= A
2
x
+ A
2
y
+ A
2
z
. [Orthonormal vectors
orthogonal unit vectors.]
Scalar product
A B =jAjjBj cos where is the angle between the vectors
= A
x
B
x
+ A
y
B
y
+ A
z
B
z
= [ A
x
A
y
A
z ]
2
4
B
x
B
y
B
z
3
5
Scalar multiplication is commutative: A B = B A.
Equation of a line
A point r (x, y, z) lies on a line passing through a point a and parallel to vector b if
r = a +b
with a real number.
Vector Algebra
Page 2

If i, j, k are orthonormal vectors and A = A
x
i + A
y
j + A
z
k thenjAj
2
= A
2
x
+ A
2
y
+ A
2
z
. [Orthonormal vectors
orthogonal unit vectors.]
Scalar product
A B =jAjjBj cos where is the angle between the vectors
= A
x
B
x
+ A
y
B
y
+ A
z
B
z
= [ A
x
A
y
A
z ]
2
4
B
x
B
y
B
z
3
5
Scalar multiplication is commutative: A B = B A.
Equation of a line
A point r (x, y, z) lies on a line passing through a point a and parallel to vector b if
r = a +b
with a real number.
Vector Algebra
Equation of a plane
A point r (x, y, z) is on a plane if either
(a) r
b
d =jdj, where d is the normal from the origin to the plane, or
(b)
x
X
+
y
Y
+
z
Z
= 1 where X, Y, Z are the intercepts on the axes.
Vector product
AB = njAjjBj sin, where is the angle between the vectors and n is a unit vector normal to the plane containing
A and B in the direction for which A, B, n form a right-handed set of axes.
A B in determinant form

i j k
A
x
A
y
A
z
B
x
B
y
B
z

A B in matrix form
2
4
0 A
z
A
y
A
z
0 A
x
A
y
A
x
0
3
5
2
4
B
x
B
y
B
z
3
5
Vector multiplication is not commutative: A B =B A.
Scalar triple product
A B C = A B C =

A
x
A
y
A
z
B
x
B
y
B
z
C
x
C
y
C
z

=A C B, etc.
Vector triple product
A (B C) = (A C)B (A B)C, (A B) C = (A C)B (B C)A
Non-orthogonal basis
A = A
1
e
1
+ A
2
e
2
+ A
3
e
3
A
1
= 
0
 A where 
0
=
e
2
 e
3
e
1
 (e
2
 e
3
)
Similarly for A
2
and A
3
.
Summation convention
a = a
i
e
i
implies summation over i = 1 . . . 3
a b = a
i
b
i
(a b)
i
="
i jk
a
j
b
k
where"
123
= 1; "
i jk
="
ik j
"
i jk
"
klm
=
il

jm

im

jl
Page 3

If i, j, k are orthonormal vectors and A = A
x
i + A
y
j + A
z
k thenjAj
2
= A
2
x
+ A
2
y
+ A
2
z
. [Orthonormal vectors
orthogonal unit vectors.]
Scalar product
A B =jAjjBj cos where is the angle between the vectors
= A
x
B
x
+ A
y
B
y
+ A
z
B
z
= [ A
x
A
y
A
z ]
2
4
B
x
B
y
B
z
3
5
Scalar multiplication is commutative: A B = B A.
Equation of a line
A point r (x, y, z) lies on a line passing through a point a and parallel to vector b if
r = a +b
with a real number.
Vector Algebra
Equation of a plane
A point r (x, y, z) is on a plane if either
(a) r
b
d =jdj, where d is the normal from the origin to the plane, or
(b)
x
X
+
y
Y
+
z
Z
= 1 where X, Y, Z are the intercepts on the axes.
Vector product
AB = njAjjBj sin, where is the angle between the vectors and n is a unit vector normal to the plane containing
A and B in the direction for which A, B, n form a right-handed set of axes.
A B in determinant form

i j k
A
x
A
y
A
z
B
x
B
y
B
z

A B in matrix form
2
4
0 A
z
A
y
A
z
0 A
x
A
y
A
x
0
3
5
2
4
B
x
B
y
B
z
3
5
Vector multiplication is not commutative: A B =B A.
Scalar triple product
A B C = A B C =

A
x
A
y
A
z
B
x
B
y
B
z
C
x
C
y
C
z

=A C B, etc.
Vector triple product
A (B C) = (A C)B (A B)C, (A B) C = (A C)B (B C)A
Non-orthogonal basis
A = A
1
e
1
+ A
2
e
2
+ A
3
e
3
A
1
= 
0
 A where 
0
=
e
2
 e
3
e
1
 (e
2
 e
3
)
Similarly for A
2
and A
3
.
Summation convention
a = a
i
e
i
implies summation over i = 1 . . . 3
a b = a
i
b
i
(a b)
i
="
i jk
a
j
b
k
where"
123
= 1; "
i jk
="
ik j
"
i jk
"
klm
=
il

jm

im

jl
Unit matrices
The unit matrix I of order n is a square matrix with all diagonal elements equal to one and all off-diagonal elements
zero, i.e., (I)
i j
=
i j
. If A is a square matrix of order n, then AI = IA = A. Also I = I
1
.
I is sometimes written as I
n
if the order needs to be stated explicitly.
Products
If A is a (n l) matrix and B is a (l m) then the product AB is dened by
(AB)
i j
=
l
?
k=1
A
ik
B
k j
In general AB6= BA.
Transpose matrices
If A is a matrix, then transpose matrix A
T
is such that (A
T
)
i j
= (A)
ji
.
Inverse matrices
If A is a square matrix with non-zero determinant, then its inverse A
1
is such that AA
1
= A
1
A = I.
(A
1
)
i j
=
transpose of cofactor of A
i j
jAj
where the cofactor of A
i j
is (1)
i+ j
times the determinant of the matrix A with the j-th row and i-th column deleted.
Determinants
If A is a square matrix then the determinant of A,jAj ( det A) is dened by
jAj =
?
i, j,k,...

i jk...
A
1i
A
2 j
A
3k
. . .
where the number of the sufxes is equal to the order of the matrix.
22 matrices
If A =

a b
c d

then,
T
=

a c
b d

A
1
=
1
jAj

d b
c a

Product rules
(AB . . . N)
T
= N
T
. . . B
T
A
T
(AB . . . N)
1
= N
1
. . . B
1
A
1
(if individual inverses exist)
jAB . . . Nj =jAjjBj . . .jNj (if individual matrices are square)
Orthogonal matrices
An orthogonal matrix Q is a square matrix whose columns q
i
form a set of orthonormal vectors. For any orthogonal
matrix Q,
Q
1
= Q
T
, jQj =1, Q
T
is also orthogonal.
Matrix Algebra
Page 4

If i, j, k are orthonormal vectors and A = A
x
i + A
y
j + A
z
k thenjAj
2
= A
2
x
+ A
2
y
+ A
2
z
. [Orthonormal vectors
orthogonal unit vectors.]
Scalar product
A B =jAjjBj cos where is the angle between the vectors
= A
x
B
x
+ A
y
B
y
+ A
z
B
z
= [ A
x
A
y
A
z ]
2
4
B
x
B
y
B
z
3
5
Scalar multiplication is commutative: A B = B A.
Equation of a line
A point r (x, y, z) lies on a line passing through a point a and parallel to vector b if
r = a +b
with a real number.
Vector Algebra
Equation of a plane
A point r (x, y, z) is on a plane if either
(a) r
b
d =jdj, where d is the normal from the origin to the plane, or
(b)
x
X
+
y
Y
+
z
Z
= 1 where X, Y, Z are the intercepts on the axes.
Vector product
AB = njAjjBj sin, where is the angle between the vectors and n is a unit vector normal to the plane containing
A and B in the direction for which A, B, n form a right-handed set of axes.
A B in determinant form

i j k
A
x
A
y
A
z
B
x
B
y
B
z

A B in matrix form
2
4
0 A
z
A
y
A
z
0 A
x
A
y
A
x
0
3
5
2
4
B
x
B
y
B
z
3
5
Vector multiplication is not commutative: A B =B A.
Scalar triple product
A B C = A B C =

A
x
A
y
A
z
B
x
B
y
B
z
C
x
C
y
C
z

=A C B, etc.
Vector triple product
A (B C) = (A C)B (A B)C, (A B) C = (A C)B (B C)A
Non-orthogonal basis
A = A
1
e
1
+ A
2
e
2
+ A
3
e
3
A
1
= 
0
 A where 
0
=
e
2
 e
3
e
1
 (e
2
 e
3
)
Similarly for A
2
and A
3
.
Summation convention
a = a
i
e
i
implies summation over i = 1 . . . 3
a b = a
i
b
i
(a b)
i
="
i jk
a
j
b
k
where"
123
= 1; "
i jk
="
ik j
"
i jk
"
klm
=
il

jm

im

jl
Unit matrices
The unit matrix I of order n is a square matrix with all diagonal elements equal to one and all off-diagonal elements
zero, i.e., (I)
i j
=
i j
. If A is a square matrix of order n, then AI = IA = A. Also I = I
1
.
I is sometimes written as I
n
if the order needs to be stated explicitly.
Products
If A is a (n l) matrix and B is a (l m) then the product AB is dened by
(AB)
i j
=
l
?
k=1
A
ik
B
k j
In general AB6= BA.
Transpose matrices
If A is a matrix, then transpose matrix A
T
is such that (A
T
)
i j
= (A)
ji
.
Inverse matrices
If A is a square matrix with non-zero determinant, then its inverse A
1
is such that AA
1
= A
1
A = I.
(A
1
)
i j
=
transpose of cofactor of A
i j
jAj
where the cofactor of A
i j
is (1)
i+ j
times the determinant of the matrix A with the j-th row and i-th column deleted.
Determinants
If A is a square matrix then the determinant of A,jAj ( det A) is dened by
jAj =
?
i, j,k,...

i jk...
A
1i
A
2 j
A
3k
. . .
where the number of the sufxes is equal to the order of the matrix.
22 matrices
If A =

a b
c d

then,
T
=

a c
b d

A
1
=
1
jAj

d b
c a

Product rules
(AB . . . N)
T
= N
T
. . . B
T
A
T
(AB . . . N)
1
= N
1
. . . B
1
A
1
(if individual inverses exist)
jAB . . . Nj =jAjjBj . . .jNj (if individual matrices are square)
Orthogonal matrices
An orthogonal matrix Q is a square matrix whose columns q
i
form a set of orthonormal vectors. For any orthogonal
matrix Q,
Q
1
= Q
T
, jQj =1, Q
T
is also orthogonal.
Matrix Algebra Solving sets of linear simultaneous equations
If A is square then Ax = b has a unique solution x = A
1
b if A
1
exists, i.e., ifjAj6= 0.
If A is square then Ax = 0 has a non-trivial solution if and only ifjAj = 0.
An over-constrained set of equations Ax = b is one in which A has m rows and n columns, where m (the number
of equations) is greater than n (the number of variables). The best solution x (in the sense that it minimizes the
errorjAx bj) is the solution of the n equations A
T
Ax = A
T
b. If the columns of A are orthonormal vectors then
x = A
T
b.
Hermitian matrices
The Hermitian conjugate of A is A
y
= (A

)
T
, where A

is a matrix each of whose components is the complex
conjugate of the corresponding components of A. If A = A
y
then A is called a Hermitian matrix.
Eigenvalues and eigenvectors
The n eigenvalues
i
and eigenvectors u
i
of an n n matrix A are the solutions of the equation Au = u. The
eigenvalues are the zeros of the polynomial of degree n, P
n
() = jAIj. If A is Hermitian then the eigenvalues

i
are real and the eigenvectors u
i
are mutually orthogonal. jAIj = 0 is called the characteristic equation of the
matrix A.
Tr A =
?
i

i
, alsojAj =
?
i

i
.
If S is a symmetric matrix, is the diagonal matrix whose diagonal elements are the eigenvalues of S, and U is the
matrix whose columns are the normalized eigenvectors of A, then
U
T
SU = and S = UU
T
.
If x is an approximation to an eigenvector of A then x
T
Ax=(x
T
x) (Rayleigh's quotient) is an approximation to the
corresponding eigenvalue.
Commutators
[A, B]  AB BA
[A, B] =[B, A]
[A, B]
y
= [B
y
, A
y
]
[A + B, C] = [A, C] + [B, C]
[AB, C] = A[B, C] + [A, C]B
[A, [B, C]] + [B, [C, A]] + [C, [A, B]] = 0
Hermitian algebra
b
y
= (b

1
, b

2
, . . .)
Matrix form Operator form Bra-ket form
Hermiticity b

 A c = (A b)

 c
Z


O =
Z
(O )

h jOji
Eigenvalues, real Au
i
=
(i)
u
i
O
i
=
(i)

i
Ojii =
i
jii
Orthogonality u
i
 u
j
= 0
Z


i

j
= 0 hij ji = 0 (i6= j)
Completeness b =
?
i
u
i
(u
i
 b)  =
?
i

i

Z


i


=
?
i
jiihiji
Rayleigh?Ritz
Lowest eigenvalue 
0

b

 A b
b

 b

0

Z


O
Z



h jOj i
h j i
Page 5

If i, j, k are orthonormal vectors and A = A
x
i + A
y
j + A
z
k thenjAj
2
= A
2
x
+ A
2
y
+ A
2
z
. [Orthonormal vectors
orthogonal unit vectors.]
Scalar product
A B =jAjjBj cos where is the angle between the vectors
= A
x
B
x
+ A
y
B
y
+ A
z
B
z
= [ A
x
A
y
A
z ]
2
4
B
x
B
y
B
z
3
5
Scalar multiplication is commutative: A B = B A.
Equation of a line
A point r (x, y, z) lies on a line passing through a point a and parallel to vector b if
r = a +b
with a real number.
Vector Algebra
Equation of a plane
A point r (x, y, z) is on a plane if either
(a) r
b
d =jdj, where d is the normal from the origin to the plane, or
(b)
x
X
+
y
Y
+
z
Z
= 1 where X, Y, Z are the intercepts on the axes.
Vector product
AB = njAjjBj sin, where is the angle between the vectors and n is a unit vector normal to the plane containing
A and B in the direction for which A, B, n form a right-handed set of axes.
A B in determinant form

i j k
A
x
A
y
A
z
B
x
B
y
B
z

A B in matrix form
2
4
0 A
z
A
y
A
z
0 A
x
A
y
A
x
0
3
5
2
4
B
x
B
y
B
z
3
5
Vector multiplication is not commutative: A B =B A.
Scalar triple product
A B C = A B C =

A
x
A
y
A
z
B
x
B
y
B
z
C
x
C
y
C
z

=A C B, etc.
Vector triple product
A (B C) = (A C)B (A B)C, (A B) C = (A C)B (B C)A
Non-orthogonal basis
A = A
1
e
1
+ A
2
e
2
+ A
3
e
3
A
1
= 
0
 A where 
0
=
e
2
 e
3
e
1
 (e
2
 e
3
)
Similarly for A
2
and A
3
.
Summation convention
a = a
i
e
i
implies summation over i = 1 . . . 3
a b = a
i
b
i
(a b)
i
="
i jk
a
j
b
k
where"
123
= 1; "
i jk
="
ik j
"
i jk
"
klm
=
il

jm

im

jl
Unit matrices
The unit matrix I of order n is a square matrix with all diagonal elements equal to one and all off-diagonal elements
zero, i.e., (I)
i j
=
i j
. If A is a square matrix of order n, then AI = IA = A. Also I = I
1
.
I is sometimes written as I
n
if the order needs to be stated explicitly.
Products
If A is a (n l) matrix and B is a (l m) then the product AB is dened by
(AB)
i j
=
l
?
k=1
A
ik
B
k j
In general AB6= BA.
Transpose matrices
If A is a matrix, then transpose matrix A
T
is such that (A
T
)
i j
= (A)
ji
.
Inverse matrices
If A is a square matrix with non-zero determinant, then its inverse A
1
is such that AA
1
= A
1
A = I.
(A
1
)
i j
=
transpose of cofactor of A
i j
jAj
where the cofactor of A
i j
is (1)
i+ j
times the determinant of the matrix A with the j-th row and i-th column deleted.
Determinants
If A is a square matrix then the determinant of A,jAj ( det A) is dened by
jAj =
?
i, j,k,...

i jk...
A
1i
A
2 j
A
3k
. . .
where the number of the sufxes is equal to the order of the matrix.
22 matrices
If A =

a b
c d

then,
T
=

a c
b d

A
1
=
1
jAj

d b
c a

Product rules
(AB . . . N)
T
= N
T
. . . B
T
A
T
(AB . . . N)
1
= N
1
. . . B
1
A
1
(if individual inverses exist)
jAB . . . Nj =jAjjBj . . .jNj (if individual matrices are square)
Orthogonal matrices
An orthogonal matrix Q is a square matrix whose columns q
i
form a set of orthonormal vectors. For any orthogonal
matrix Q,
Q
1
= Q
T
, jQj =1, Q
T
is also orthogonal.
Matrix Algebra Solving sets of linear simultaneous equations
If A is square then Ax = b has a unique solution x = A
1
b if A
1
exists, i.e., ifjAj6= 0.
If A is square then Ax = 0 has a non-trivial solution if and only ifjAj = 0.
An over-constrained set of equations Ax = b is one in which A has m rows and n columns, where m (the number
of equations) is greater than n (the number of variables). The best solution x (in the sense that it minimizes the
errorjAx bj) is the solution of the n equations A
T
Ax = A
T
b. If the columns of A are orthonormal vectors then
x = A
T
b.
Hermitian matrices
The Hermitian conjugate of A is A
y
= (A

)
T
, where A

is a matrix each of whose components is the complex
conjugate of the corresponding components of A. If A = A
y
then A is called a Hermitian matrix.
Eigenvalues and eigenvectors
The n eigenvalues
i
and eigenvectors u
i
of an n n matrix A are the solutions of the equation Au = u. The
eigenvalues are the zeros of the polynomial of degree n, P
n
() = jAIj. If A is Hermitian then the eigenvalues

i
are real and the eigenvectors u
i
are mutually orthogonal. jAIj = 0 is called the characteristic equation of the
matrix A.
Tr A =
?
i

i
, alsojAj =
?
i

i
.
If S is a symmetric matrix, is the diagonal matrix whose diagonal elements are the eigenvalues of S, and U is the
matrix whose columns are the normalized eigenvectors of A, then
U
T
SU = and S = UU
T
.
If x is an approximation to an eigenvector of A then x
T
Ax=(x
T
x) (Rayleigh's quotient) is an approximation to the
corresponding eigenvalue.
Commutators
[A, B]  AB BA
[A, B] =[B, A]
[A, B]
y
= [B
y
, A
y
]
[A + B, C] = [A, C] + [B, C]
[AB, C] = A[B, C] + [A, C]B
[A, [B, C]] + [B, [C, A]] + [C, [A, B]] = 0
Hermitian algebra
b
y
= (b

1
, b

2
, . . .)
Matrix form Operator form Bra-ket form
Hermiticity b

 A c = (A b)

 c
Z


O =
Z
(O )

h jOji
Eigenvalues, real Au
i
=
(i)
u
i
O
i
=
(i)

i
Ojii =
i
jii
Orthogonality u
i
 u
j
= 0
Z


i

j
= 0 hij ji = 0 (i6= j)
Completeness b =
?
i
u
i
(u
i
 b)  =
?
i

i

Z


i


=
?
i
jiihiji
Rayleigh?Ritz
Lowest eigenvalue 
0

b

 A b
b

 b

0

Z


O
Z



h jOj i
h j i
Pauli spin matrices

x
=

0 1
1 0

, 
y
=

0 i
i 0

, 
z
=

1 0
0 1


x

y
= i
z
, 
y

z
= i
x
, 
z

x
= i
y
, 
x

x
=
y

y
=
z

z
= I
Notation
is a scalar function of a set of position coordinates. In Cartesian coordinates
= (x, y, z); in cylindrical polar coordinates = (,', z); in spherical
polar coordinates = (r,,'); in cases with radial symmetry = (r).
A is a vector function whose components are scalar functions of the position
coordinates: in Cartesian coordinates A = iA
x
+ jA
y
+ kA
z
, where A
x
, A
y
, A
z
are independent functions of x, y, z.
In Cartesian coordinatesr (`del')  i
?
?x
+ j
?
?y
+ k
?
?z

2
6
6
6
6
6
6
6
4
?
?x
?
?y
?
?z
3
7
7
7
7
7
7
7
5
grad =r, div A =r A, curl A =r A
Identities
1
+
2
1
2
div(A
1
+ A
2
) div A
1
+ div A
2
1

2
)
1
2
+
2
1
curl(A
1
+ A
2
) curl A
1
+ curl A
2
div(A) div A + (grad) A, curl(A) curl A + (grad) A
div(A
1
 A
2
) A
2
 curl A
1
A
1
 curl A
2
curl(A
1
 A
2
) A
1
div A
2
A
2
div A
1
+ (A
2
1
(A
1
2
div(curl A) 0, curl(grad) 0
2
A
1
 A
2
) A
1
 (curl A
2
) + (A
1
2
+ A
2
 (curl A
1
) + (A
2
1
Vector Calculus
```

## Engineering Mathematics

65 videos|121 docs|94 tests

## FAQs on Engineering Mathematics Formulas for GATE Exam - Engineering Mathematics - Civil Engineering (CE)

 1. What are some important engineering mathematics formulas for the GATE exam?
Ans. Some important engineering mathematics formulas for the GATE exam include: - Quadratic equation formula: x = (-b ± √(b^2 - 4ac))/(2a) - Trigonometric identities: sin^2θ + cos^2θ = 1, sin(θ ± φ) = sinθcosφ ± cosθsinφ - Differential calculus formulas: d/dx(a) = 0, d/dx(x^n) = nx^(n-1), d/dx(e^x) = e^x - Integral calculus formulas: ∫(k*f(x))dx = k∫f(x)dx, ∫(f(x) + g(x))dx = ∫f(x)dx + ∫g(x)dx - Probability formulas: P(A ∪ B) = P(A) + P(B) - P(A ∩ B), P(A|B) = P(A ∩ B)/P(B)
 2. How can I effectively prepare for the engineering mathematics section of the GATE exam?
Ans. To effectively prepare for the engineering mathematics section of the GATE exam, you can follow these tips: - Understand the syllabus and exam pattern thoroughly. - Make a study plan and allocate sufficient time for each topic. - Practice solving a variety of problems from previous year question papers and sample papers. - Focus on understanding the concepts and derivations of important formulas. - Seek help from textbooks, online resources, and video tutorials for clarification on difficult topics. - Regularly revise the topics to strengthen your understanding and retention. - Take mock tests to assess your preparation level and improve your time management skills.
 3. What are the common mistakes to avoid while solving engineering mathematics problems in the GATE exam?
Ans. Common mistakes to avoid while solving engineering mathematics problems in the GATE exam include: - Misinterpreting the question or not understanding the problem statement clearly. - Failing to apply the correct formula or concept to solve the problem. - Making calculation errors due to lack of attention or rushing through the solution. - Not showing proper steps or working in a systematic manner, leading to confusion or mistakes. - Neglecting to double-check the final answer for accuracy and correctness. - Ignoring units or not converting them properly in calculations. - Overlooking special cases or exceptions mentioned in the question.
 4. Are there any shortcuts or tricks to solve engineering mathematics problems faster in the GATE exam?
Ans. Yes, there are some shortcuts or tricks that can help you solve engineering mathematics problems faster in the GATE exam. Some of them include: - Memorizing important formulas and identities to save time on derivations or derivations during the exam. - Using approximation techniques to simplify complex calculations, especially when the answer options are far apart. - Applying mental math strategies like multiplying or dividing by powers of 10 to simplify calculations. - Using symmetry properties or properties of special functions to simplify expressions or equations. - Using smart substitutions or transformations to convert the problem into a simpler form. - Identifying patterns or relationships between variables to solve problems more efficiently.
 5. How can I improve my speed and accuracy in solving engineering mathematics problems for the GATE exam?
Ans. To improve your speed and accuracy in solving engineering mathematics problems for the GATE exam, you can follow these tips: - Practice regularly to build fluency and familiarity with different types of problems. - Solve timed mock tests to simulate the exam environment and improve your speed. - Focus on understanding the underlying concepts and principles rather than rote memorization. - Develop a systematic approach to problem-solving, breaking down complex problems into smaller steps. - Identify and work on your weak areas to minimize errors and improve accuracy. - Learn and apply shortcut techniques or tricks to save time on calculations. - Analyze your mistakes and learn from them to avoid repeating them in the actual exam.

## Engineering Mathematics

65 videos|121 docs|94 tests

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