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Curl and Divergence
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Curl Let π
= π,π,π
be a vector field on π 3 and assume the partial derivatives of π, π and π
all exist. Let π»= π ππ₯ , π ππ¦ , π ππ§ (the βdelβ operator) The curl of the vector field π
is Example 1: Let Find curl F. P Q R
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Curl Example 2: Let F π₯,π¦,π§ = π₯,π¦,π§ . Evaluate curl π
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A field with π»Γπ
=π is called curl free or irrotational. Theorem 1: A conservative vector field with continuous derivatives is irrotational. Proof: Suppose π
is a conservative vector field and let π be its potential function: π
=π»π= π π₯ , π π¦ , π π§ Clairautβs Theorem
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Curl The converse of Theorem 1 is also true if we assume the domain of the vector field is simply connected (in particular, the whole πΉ 3 ) Theorem 2: If π
is a vector field on all of πΉ 3 with continuous partial derivatives and π»Γπ
=π, then π
is a conservative vector field. REMARKS: Theorem 2 provides a quick and easy way to check whether a 3D vector field is conservative. The 2D vector field π
π₯,π¦ = π π₯,π¦ ,π(π₯,π¦) can be written as a 3D vector field π
π₯,π¦ = π π₯,π¦ ,π π₯,π¦ ,0 . Then π»Γπ
= 0,0, π π₯ β π π¦ . Therefore, in 2D, π»Γπ
=0 is equivalent to π π₯ = π π¦ The Fundamental Theorem of Line Integrals holds also in 3D for conservative vector fields.
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Curl β Example 3 Show that π
= π¦,π₯+π§,π¦+6π§ is conservative and find a potential function. π
is irrotational, therefore there exists a potential function π such that π
=π»π π π₯ =π¦ π π¦ =π₯+π§ π π§ =π¦+6π§ Integrate w.r.t π₯ π π₯,π¦,π§ =π₯π¦+π(π¦,π§) differentiate w.r.t π¦ π π¦ =π₯+ π π¦ (π¦,π§) =π₯+π§ π π¦ π¦,π§ =π§ g π¦,π§ =π§π¦+β(π§) π π₯,π¦,π§ =π₯π¦+π§π¦+β(π§) differentiate w.r.t π§ π π§ =π¦+ββ²(π§) =π¦+6π§ β β² π§ =6π§ β π§ =3 π§ 2 +πΎ π π₯,π¦,π§ =π₯π¦+π§π¦+3 π§ 2 +πΎ
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Curl - Example 3 continued
Evaluate the line integral of π
along the curve comprised of the line segment from (0,0,0) to (1,1,2) and the line segment from (1,1,2) to (3,1,4) Initial point: (0,0,0) Terminal point: (3,1,4) Potential Function: π π₯,π¦,π§ =π₯π¦+π§π¦+3 π§ 2 Fundamental Theorem for Line Integrals:
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Curl Interpreting the curl: If we think of the vector field as a velocity vector field of a fluid in motion, the curl measures rotation. At a given point, the curl is a vector parallel to the axis of rotation of flow lines near the point, with direction determined by the Right Hand Rule. Example 4: Determine whether the curl of each vector field at the origin is the zero vector or points in the same direction as Β± i, Β± j, Β± k. (a) Based on the direction of the rotation and the Right Hand Rule, the curl will point in the βπ€= 0,0,β1 direction.
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Curl β Example 4 continued
(b) The vector field is clearly irrotational, thus the curl is the zero vector: 0,0,0 . (c) Based on the direction of the rotation and the Right Hand Rule, the curl points in the direction of +π£= 0,1,0
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Divergence Let be a differentiable vector field on a region in π 3 .
Let π»= π ππ₯ , π ππ¦ , π ππ§ (the βdelβ operator) The divergence of the vector field π
is (a scalar) Example 5: Let π
= π π₯π¦π§ ,π¦π§ sin π₯ , π₯ 2 + π¦ 2 + π§ Find div F. Example 6: Let π
= π₯,π¦,π§ . Find div F.
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Divergence Interpreting the Divergence: The divergence at a given point measures the net flow out of a small box around the point, that is, it measures what is produced (source) or consumed (sink) at a given point in space. Example 7: Determine whether the divergence of each vector field at the indicated point P is positive, negative or zero (a) Draw a box around the point P. We can clearly see from the magnitude of the vectors that the net flow out of the box is negative (more βstuffβ coming in than out). Thus the divergence is negative and we say the point P is a sink.
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Divergence β Example 7 continued
Draw a box around the point. We can see that the net flow out of the box is zero (same amount of βstuffβ is coming in than coming out). (b) Thus the divergence is zero and we say that the vector field is incompressible at the point. Draw a box around the point. The net flow is positive (less βstuffβ coming in than out). (c) Thus the divergence is positive and we say that the point is a source.
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