In parts (a) - (h), prove the property for vector fields F and G and scalar function f . (Assume that the required partial derivatives are continuous.) a) curl( F + G = curlF + curlG b) c u r l ( ∇ f ) = ∇ x ( ∇ f ) = 0 c) div( ∇ f ) = ∇ x ( ∇ f ) = 0 d) div(FxG ) = ( curl G − F ( curlG ) e) ∇ x [ ∇ f + ( ∇ x F ) ] = ∇ x ( ∇ x F ) f) ∇ x ( f F ) = f ( ∇ x F ) + ( ∇ f ) x F g) d i v ( f F ) = f ( d i v F ) + ( ∇ f ) . F h) d i v ( c u r l F ) = 0
In parts (a) - (h), prove the property for vector fields F and G and scalar function f . (Assume that the required partial derivatives are continuous.) a) curl( F + G = curlF + curlG b) c u r l ( ∇ f ) = ∇ x ( ∇ f ) = 0 c) div( ∇ f ) = ∇ x ( ∇ f ) = 0 d) div(FxG ) = ( curl G − F ( curlG ) e) ∇ x [ ∇ f + ( ∇ x F ) ] = ∇ x ( ∇ x F ) f) ∇ x ( f F ) = f ( ∇ x F ) + ( ∇ f ) x F g) d i v ( f F ) = f ( d i v F ) + ( ∇ f ) . F h) d i v ( c u r l F ) = 0
In parts (a) - (h), prove the property for vector fields F and G and scalar function f. (Assume that the required partial derivatives are continuous.)
a)
curl(
F
+
G
=
curlF
+
curlG
b)
c
u
r
l
(
∇
f
)
=
∇
x
(
∇
f
)
=
0
c)
div(
∇
f
)
=
∇
x
(
∇
f
)
=
0
d)
div(FxG
)
=
(
curl
G
−
F
(
curlG
)
e)
∇
x
[
∇
f
+
(
∇
x
F
)
]
=
∇
x
(
∇
x
F
)
f)
∇
x
(
f
F
)
=
f
(
∇
x
F
)
+
(
∇
f
)
x
F
g)
d
i
v
(
f
F
)
=
f
(
d
i
v
F
)
+
(
∇
f
)
.
F
h)
d
i
v
(
c
u
r
l
F
)
=
0
Quantities that have magnitude and direction but not position. Some examples of vectors are velocity, displacement, acceleration, and force. They are sometimes called Euclidean or spatial vectors.
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