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Vectors, Gradient, Divergence and Curl.
1 Introduction
A vector is determined by its length and direction. They are usually denoted
with letters with arrows on the top aor in bold letter a. We will use arrows.
a
Two vectors are equal if they have the same length and the same direction:
vw
v= w
If we are given two points in the space (p1
, p2
, p3) and (q
1, q
2, q
3) then we can
compute the vector that goes from p to q as follows:
pq= [q1 p1, q2 p2, q3 p3]
For example if you are given the point p = (1, 0, 1) and q = (3, 2, 4) then the
vector joining p and q is:
pq= [3 1, 2 0, 4 1] = [2, 2, 3].
The three principal directions (unitary vectors, vectors of length one) in the space
are
i= [1, 0, 0],
j = [0, 1, 0]
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and
k= [0, 0, 1]
i j
k
The length of a vector with coordinates [a1, a2, a3] is
|a| =
a21+a22+a
23
The sum of two vectors a = [a1, a2, a3] andb= [b1, b2, b3] is obtained by adding
the corresponding componentsa+ b= [a1+b1, a2+b2, a3+b3].
We have some properties:
1. Commutative: a+ b= b+ a
2. Associative: a+ (b+ c) = (a+ b) + c
3. There exists0 such that:
a+ 0 = 0 + a=a
and
a a= 0
We can multiply a vector by a real number, often called scalar R:
a= [a1, a2, a3] = [a1, a2a3]
And we have some properties:
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1. Distributive 1: (a+ b) =a+b
2. Distributive 2: (+ )a= a+a
3. 1a=a, (1)a= a, and 0a= 0.
Example 1 Ifa= [1, 2, 3] andb= [0, 1, 0], then compute|3a b|:
3a b = 3[1, 2, 3] [0, 1, 0]= [3, 6, 9 [0, 1, 0]= [3, 5, 9]
Then:
|3a b| =
32 + 52 + 92 =
115.
1.1 Inner product (dot product)
The inner product of the vectors a and b is a scalar (real number) defined as
follows:
a b= |a||b| cos ,
where is the angle between a andb. Ifa= [a1, a2, a3] andb = [b1, b2, b3], then
the inner product is:
a b= a1b1+a2b2+a3b3.
Observe that
|a|
=
a
a= a21+a22+a
23,
and then we can compute the angle between aandbwith the formula:
cos = ab
|a||b|=
a1b1+a2b2+a3b3a21+a
22+a
23
b21+b
22+b
23
.
Two vectors are orthogonalif and only if its inner product is 0:
ais orthogonal tob a b= 0
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The inner product has some properties:
1. Commutative: a b= b a
2. Distributive: (a+b) c= a c+b c
3. a aanda a= 0 if and only ifa= 0.
Recall that there are two important inequalities with vectors:
Cauchy-Schwarz:|a b| |a||b|
Triangle Inequality:|a+ b| |a| + |b|
1.2 Vector product (cross-product)
It is denoted by v= a b and it is a vector with length
|v| = |a b| = |a||b| sin ,
where is the angle betweena andb,and the direction ofv is perpendicular to
both a and b and such a,b, v, in this order, form a right-handed triple. (This
means that the determinant ofa,b, v is positive).
Geometrically speaking|a b| is the area of the parallelogram with sides aandb.
a
b
|a b|
And we have some properties:
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1. If R then (a b) = (a) b=a (b)
2. Distributives: a (b+ c) =a b+ a c and (a+ b) c=a c+ b c
3. Anticommutative: a b= b a
Remark: The vector product is NOT associative. Thus, in general:
a (b c) = (a b) c
Let us see this with an example:
a= [1, 0, 0],b= [1, 0, 0], c= [0, 1, 0]
Then
b c= [0, 0, 1] a (b c) = [0, 1, 0],
but
a b= [1, 0, 0] [1, 0, 0] = [0, 0, 0] (a b) c= [0, 0, 0]
1.3 Scalar triple product
It is a scalar (real number) defined as follows:
(ab c) =a (b c)
(Notice that there are no commas in (ab c)). We have:
(ab c) =a (
b c) =
a1 a2 a3
b1 b2 b3
c1 c2 c3
It is an immediate consequence of the properties of the determinants that:
a (b c) = (a b) c.
Geometric interpretation: The absolute value of (ab c) is the volume of the
parallelepiped (oblique box) witha,b andc as edges.
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Example 2 Find the area of the parallelogram with vertices (2, 2, 0), (9, 2, 0),(10, 3, 0),(3, 3, 0).
First, we need to find the vectors joining the vertices (2, 2, 0), (9, 2, 0) and
(2, 2, 0), (3, 3, 0) ((10, 3, 0) is not needed!). We will denote bya the vector from
(2, 2, 0) to (9, 2, 0) andbthe vector from (2, 2, 0) to (3, 3, 0). Then:
a= [9 2, 2 2, 0 0] = [7, 0, 0]
b= [3 2, 3 2, 0] = [1, 1, 0].
We know that the area of the parallelogram with edges aandbis the module of
its vector product:
a b=
i j k
7 0 0
1 1 0
= 7k= [0, 0, 7],
And therefore:
|a b| = 7.
Example 3 Find the area of the triangle with vertices (1, 0, 0), (0, 1, 0) and
(0, 0, 1).
To do this, we first compute the area of the the parallelogram that has as
edges the vector joining (1, 0, 0), (0, 1, 0) and the vector joining (1, 0, 0), (0, 0, 1)
and then we divide by 2.
a= [0 1, 1 0, 0 0] = [1, 1, 0] and b= [0 1, 0 0, 1 0] = [1, 0, 1].
Then:
a b=
i j k
1 1 01 0 1
= i+ j+ k= [1, 1, 1],
so the area of the parallelogram is:
|a b| =
12 + 12 + 12 =
3.
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Hence the area of the triangle is
3
2 .
Example 4 Find the volume of the parallelepiped determined by the vertices
(1, 1, 1),(4, 7, 2),(3, 2, 1) and (5, 4, 3)
The volume of the parallelepiped is the absolute value ofa (b c), wherea,bandcare the vectors joining the points (1, 1, 1) and (4, 7, 2), (1, 1, 1) and (3, 2, 1),
and (1, 1, 1) and (5, 4, 3) respectively:
a= [4
1, 7
1, 2
1] = [3, 6, 1]
b= [3 1, 2 1, 3 1] = [2, 1, 0]
c= [5 1, 4 1, 3 1] = [4, 3, 2].
Then:
a (b c) =
3 6 1
2 1 0
4 3 2
= 16.
Hence the volume is|a (b c)| = 16.
2 Gradient of a Scalar Field
A vector field Fis a function that takes any point in space and assign a vector
to it:
F: From points in the space To vectors in the space(x,y,z ) [F1(x,y,z ), F2(x,y,z ), F3(x,y,z )]
Ascalar field fis a function that takes a point in space and assigns a number to
it:
f: From points in the space To real numbers(x,y,z ) f(x,y,z )
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Example 5 The function
f(x,y,z ) =xyz
is a scalar field that assigns to the point in the space (x,y,z ) the real number
xyzbut the function
F(x,y,z ) = [ x
x2 +y2 +z2,
yx2 +y2 +z2
, z
x2 +y2 +z2]
is a vector field that assigns to the point in the space ( x,y,z ) the unit position
vector [ xx2 +y2 +z2
, y
x2 +y2 +z2, z
x2 +y2 +z2] .
Definition 1 The gradient of a given scalar fieldf(x,y,z ) is a vector field de-
noted by grad f or fand it is defined as follows:
f=
f
x, f
y, f
z
=
f
xi+
f
yj+
f
zk
This notation means that if we have a point in the space (x0, y0, z0) then
f(x0, y0, z0) = fx
|(x0,y0,z0)i+ fy |(x0,y0,z0)j+ fz|(x0,y0,z0)k
We can think as a linear operator that acts on scalar fields giving vectors fields:
: Smooth Scalar Fields Vector fieldsf f=
fx
,fy
,fz
From Vector Calculus we know that the partial derivatives fx
,fy
,fz
give the
rates of change of f(x,y,z ) in the directions ofi,j, k respectively. It seems
natural to ask what is the rate of change in any other direction. This is what the
directional derivatives represent.
Suppose thatb= [b1, b2, b3] is a unit vector, thus it has length 1:
|b| =
b21+b22+b
23= 1
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Then the directional derivative off(x,y,z ) in the direction ofa unit vector bis:
Dbf= b f, (1)
where is the scalar product.Ifa = (a1, a2, a3) is a vector which is not unit then a unit vector with the
same direction thanais a|a| :
a
|a|
= 1
|a|
a21+a22+a
23 =
1
|a| |a| = 1.
We define the directional derivative off(x,y,z ) in the direction ofaas
Daf= a
|a|f. (2)
Please note that equation (??) is equivalent to equation (??) when a is a unit
vector. (The two definitions of directional derivative are the same.)
Example 6 Given f(x,y,z ) = 2x2 + 3y2 +z2 and a = [1, 0,
2], evaluate the
directional derivative off in the direction ofaat the point (2, 1, 3).
First we compute the gradient of f:
f= [4x, 6y, 2z]
Sinceais not a unit vector the directional derivative is:
Daf= [1, 0, 2]12 + 02 + (2)2
4x
6y
2z
=[1, 0, 2]5
4x
6y
2z
= 15(4x 4z)
And evaluating at the point (2, 1, 3) we get:
Daf(2, 1, 3) =8 12
5=
45
,
the minus sign indicates that the function fdecreases in the direction ofa.
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Remark: If the gradient offat a point P is not zero f(P) = grad f(P) = 0,then it is a vector in the direction of maximum increase off at P.
Definition 2 A surface is all points in(x,y,z ) R3 that verifiesf(x,y,z ) =c,for some smooth scalar fieldf and constantc.
Consider the unit sphere in R3, S2:
S2 = {(x,y,z ) R3 :x2 +y2 +z2 = 1}.
In this case f(x,y,z ) =x2 +y2 +z2 and c= 1.
The cone with center at (0, 0, 0) is another surface withf(x,y,z ) =x2+y2z2
and c= 0:
C= {(x,y,z ) R3 :x2 +y2 z2 = 0}.
Theorem 1 Let f be differentiable and S ={(x,y,z ) : f(x,y,z ) = c} be asurface. Then the gradient of f, f at a point P of the surface S is a normal
vector to S atP. (Provided f(P) = 0).
Example 7 Find a unit normal vector of the cone of the revolution z2 = 4(x2 +
y2) at the point P = (1, 0, 2).
In this case:
f(x,y,z ) = 4(x2 +y2) z2
The theorem ensures that the gradient offat the point (1, 0, 2) is normal to the
cone:
f= [8x, 8y, 2z],
and evaluating it at P
f(1, 0, 2) = [8, 0, 4].
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But we observe that f(1, 0, 2) is not unit vector, so we calculate the unit vectorin the direction of
f(1, 0, 2):
f(1, 0, 2)|f(1, 0, 2)| =
[8, 0, 4]82 + (2)2
=[8, 0, 4]
80=
[2, 0, 1]5
And more examples (FOR YOU TO TRY):
1. Find the directional derivative offatP in the direction ofain the following
cases:
f(x,y,z ) =x2 +y2 z, P = (1, 1, 2), a= [1, 1, 2]
f(x,y,z ) =x2 +y2 +z2, P = (2, 2, 1), a= [1, 1, 0]
f(x,y,z ) =xyz, P = (1, 1, 3), a= [1, 2, 2]
2. Compute the normal to the surface:
S= {(x,y,z ) R3 :ax+by+cz=d} for any P.
S= {(x,y,z ) R3 :x2 + 3y2 +z2 = 28} and P = (4, 1, 3)
S= {(x,y,z ) R3 :x2 +y2 = 25} and P = (4, 3, 8)
Proposition 1 For allf, g smooth scalar fields, the operator verifies:
1. (f g) =g f+fg,
2.
fn =nfn1
f, for anyn
N,
3. ( fg ) = 1g2 (gf fg),
4. 2(f g) =g 2f+ 2 fg+f2g.
Proof:
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1. By definition of the gradient:
(f g) = [(f g)
x ,(f g)
y ,(f g)
z ]
= [ fx
g+fgx
,fy
g+fgy
,fz
g+fgz
]
using the product rule for partial derivatives
= [ fx
,fy
,fz
]g+f[ gx
,gy
, gz
]
using linearity of vectors
= g f+fg,
2. It is a consequence of the chain rule for partial derivatives:
fn = [ (fn)
x ,
(fn)y
,(fn)
z ]
= [nfn1fx
, nfn1fy
, nfn1fz
] =nfn1 f, for any n N,
3. For (fg ) = 1g2 (gf fg), use part 1 with f and 1g and recall that
x
1g =
1g2
gx
. (Similarly with the partial derivatives with respect to to y
and z).
4. Notice that
2(f g) = (f g) = 2(f g)
x2 +
2(f g)
y2 +
2(f g)
z2
Furthermore:
2(f g)
x2 =
x(f g)
x=
xf
x
g+fg
x=
2f
x2g+ 2
f
x
g
x
+fg
x
Similarly:
2(f g)
y2 =
2f
y2g+ 2
f
y
g
y+f
g
y
and
2(f g)
z2 =
2f
z2g+ 2
f
z
g
z+f
g
z
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The result follows on adding these three equations together and observing
that
2 = 2
x2+
2
y2+
2
z2
and
f g= fx
g
x+
f
y
g
y+
f
z
g
z
(Important) Remark: Some vector fields are gradients of scalar fields. This
means that for a vector field Fwe can find a scalar field f called potential of F
such thatF= f= [f
x,f
y,f
z].
In this case we say that F is a gradient field.
In the exercises you will be given a vector field and you will be asked to find
a potential for it:
Example 8 Is F(x,y,z ) = [yz,xz,xy] a gradient field?
If we find a scalar field f(x,y,z ) such that:
F1(x,y,z ) =yz=f
x (3)
F2(x,y,z ) =xz=f
y (4)
and
F3(x,y,z ) =xy = f
z (5)
then F is a gradient field.
If we considery and zas constants and we integrate with respect to to x equation
(??), we obtain: yzdx=
f
xdx (6)
xyz+C(y, z) =f(x,y,z ) (7)
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This means that if the potential function for F exists then it has the shape
of xyz+ C(y, z) where C(y, z) is the constant of integration that we have to
determine using equations (??) and (??). (The constant of integration must
depend on y and zbecause to integrate with respect to x (??) we thought y and
zas constants).
We use now equation (??) to equate with the differential of equation (??)
with respect to y:
f
y =
y(xyz+C(y, z)) =xz
or
xz+
yC(y, z) =xz,
and we conclude that for this equality to hold we need
yC(y, z) = 0
That is, C(y, z) does not depend on yor C(y, z) could be written as C(z). Now
we use equation (??) and we equate to the derivative with respect tozof equation
(??):f
z =
y(xyz+C(z)) =xy
or
xy+
zC(z) =xy,
which implies that the constantC(z) does not depend onzso it is just a constant,
Csay. We conclude that the potential for F is
f(x,y,z ) =xyz+C,
Cany constant in R.
You can double check that f(x,y,z ) =xyz+Cverifies that F = f.
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Example 9 Find a potential for F=
x
x2 +y2 +z2,
yx2 +y2 +z2
, zx2 +y2 +z2
We need to find a scalar field f(x,y,z ) such that:
F1(x,y,z ) = x
x2 +y2 +z2 =
f
x (8)
F2(x,y,z ) = y
x2 +y2 +z2 =
f
y (9)
and
F3(x,y,z ) = z
x2 +y2 +z2 =
f
z (10)
Integrating with respect to x equation (??) we get that if the potential exists
must it be as follows:
f(x,y,z ) =1
2ln(x2 +y2 +z2) +C(y, z). (11)
Differentiating equation (??) with respect to y and equating to equation (??):
y
x
2
+y
2
+z
2 +
y
C(y, z) = y
x
2
+y
2
+z
2
which implies that the constant C(y, z) does not depend on y. Similarly dif-
ferentiating equation (??) with respect to z and equating it to equation (??)
we conclude that the constant does not depend on z either and therefore the
potential is:
f(x,y,z ) =1
2ln(x2 +y2 +z2) +C, C R.
Give a try to find a potential for:
1. [3x, 5y, 4z]
2. [4x3, 3y2, 6z]
(The solutions are 32
x2 + 52
y2 2z2 +Cand x4 +y3 3z2 +C respectively).
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The differential operator
2f= f= 2
fx2 +
2
fy2 +
2
fz2
is called Laplace Operator.
Notice
: Smooth Scalar Fields Scalar Fieldsf f
Example 10 Iff(x,y,z ) =x3 +y2 + 3xz5 then:
fx
= 3x2 + 3z5 2fx2
= 6x
f
y = 2y
2f
y2 = 2
f
z = 15xz4
2f
z2 = 60xz3
Hence:
f= 6x+ 2 + 60xz3,
for example:
f(1, 1, 1) = 6 + 2 + 60 = 68.
3 Divergence of a Vector Field
The divergence of a vector field F = [F1, F2, F3] is a scalar field div Fdefined as
follows:
div F =F1
x +
F2
y +
F3
z .
We can understand the divergence as a differential operator acting on smooth
vector fields that produces scalar fields:
div: Smooth Vector Fields Scalar Vector FieldsF F1
x + F2
y + F3
z
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Sometimes div F is denoted by
F= div F ,
the dot is the scalar product dot because can be considered as the vector
= [ x
,
y,
z],
so we have:
F= [
x,
y,
z]
[F1
, F2
, F3] =
xF
1+
yF
2+
zF
3,
and the products x
F1, y
F2 and z
F3 mean that we have to differentiate F1
with respect to x, F2 with respect to y and F3 with respect to z:
xF1 =
F1
x
yF2 =
F2
y
z
F3=F3
z
Remark: Iff is a scalar field then we have:
div (gradf) = f
or equivalently
f= f
Example 11 Compute the divergence of the following vector field:
F(x,y,z ) = [x3 +y3, 3x2, 3zy2].
By definition:
F = (x3 +y3)
x +
(3x2)
y +
(3zy2)
z = 3x2 + 3y2
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4 The Curl of a Vector Field
The Curl of a vector field Fis another vector defined as the following determinant:
curl F=
i j k
x
y
z
F1 F2 F3
=
F3
y F2
z
i+
F1
z F3
x
j+
F2
x F1
y
k
Suppose that Frepresents the velocity of a rotating body then curl F has the
direction of the axis of rotation and its module is twice the angular speed of the
rotation.
Definition 3 If the curl of a vector field is zero we say that the vector field is
irrotational.
Remark: The definition of irrotationalvector field F= [F1, F2, F3] is equivalent
to have the following three conditions in the partial derivatives ofF1, F2 and F3:
F2
x =F1
y
F1
z =
F3
x
F3
y =
F2
z
These three equations can be a short way to prove that something is not irrota-
tional without computing the whole determinant:
Example 12 Consider F= [y,x, 0], with >0 since F2x = and F1y = then F is not irrotational.
However if we compute the determinant we obtain curl F = [0, 0, 2] which
means that the body rotates around the zaxis with angular speed .
Lemma 1 Gradient fields are irrotationals. That is, if F = f for some smoothscalar fieldf thencurl F = 0.
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Proof: Using the denition of curl:
curl f = curl
[ fx
, fy
, fz
]
=
i
j
k
x
y
z
fx
fy
fz
=
y
fz
z
fy
i+
z
fx
x
fz
j+
x
fy
y
fx
k
= 2f
yz 2f
zyi+
2f
zx 2f
xzj+
2f
xy 2f
yxk,
The result follows since the mixed partial derivatives of a smooth scalar field are
equal.
Example 13 The gravitational field p is the force of attraction between two
particles at points P0 = (x0, y0, z0) and P = (x,y,z ). It is defined by
p= cr3
r= cr3
[x x0, y y0, z z0]
where r =
(x x0)2 + (y y0)2 + (z z0)2 and it is an irrotational field be-cause the scalar field f(x,y,z ) = cr is a potential for it. (Check it!)
Lemma 2 Let Fbe a smooth vector field then
div (curl F) = 0
Proof:
div ( curl F) = x
F3y
F2z
+
y
F1z
F3x
+
z
F2x
F1y
= 2F3
xy
2F2xz
+ 2F1
yz
2F3yx
+ 2F2
zx
2F1zy
= 0
Because if F is smooth then F1, F2, F3 are smooth (scalar fields) and the mixed
second partial derivatives ofF1, F2, F3 are equal.
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Example 14 Compute the curl of the following vector field F(x,y,z ) = [ex cos y, ex sin y, 0]
curl F =
i j k
x
y
z
ex cos y ex sin y 0
= (ex sin y)
xk+
(ex cos y)z
j (ex cos y)y
k (ex sin y)z
i
= (ex sin y ex( sin y))k= [0, 0, 2ex sin y]
20