Suppose that F x , y , = f x , y i + g x , y j is a vector field on the x y -plane and that f and g have continuous first partial derivatives with f y = g x everywhere. Use Green’s Theorem to explain why ∫ C 1 F ⋅ d r = ∫ C 2 F ⋅ d r where C 1 and C 2 are the oriented curves in the accompanying figure. [ Note : Compare this result with Theorems 15.3.2 and 15.3.3.]
Suppose that F x , y , = f x , y i + g x , y j is a vector field on the x y -plane and that f and g have continuous first partial derivatives with f y = g x everywhere. Use Green’s Theorem to explain why ∫ C 1 F ⋅ d r = ∫ C 2 F ⋅ d r where C 1 and C 2 are the oriented curves in the accompanying figure. [ Note : Compare this result with Theorems 15.3.2 and 15.3.3.]
Suppose that
F
x
,
y
,
=
f
x
,
y
i
+
g
x
,
y
j
is a vector field on the
x
y
-plane
and that f and g have continuous first partial derivatives with
f
y
=
g
x
everywhere. Use Green’s Theorem to explain why
∫
C
1
F
⋅
d
r
=
∫
C
2
F
⋅
d
r
where
C
1
and
C
2
are the oriented curves in the accompanying figure. [Note: Compare this result with Theorems 15.3.2 and 15.3.3.]
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.
The gradient vector field of f(x,y)=y(2x2 -y3 ) is given by:
O1. (2xy)i +(x2 -3y² )i
O II. (4xy)i -(2x2 -3y? )i
O II (4xy)i +(4x2 -3y² )i
OV. (4xy)i +(2x2 -3y² )i
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