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Vector definitions, identities, and theorems

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Identities<br />

1. (A × B) · C = A · (B × C)<br />

2. A × (B × C) = B (A · C) − C (A · B)<br />

3. ∇ (fg) = f∇g + g∇f<br />

4. ∇ (a/b) = (1/b)∇a − a/b 2 ∇b<br />

5. ∇ · (A · B) = (B · ∇)A + (A · ∇)B + B × (∇ × A) + A × (∇ × B)<br />

6. ∇ · (fA) = (∇f) · A + f (∇ · A)<br />

7. ∇ · (A · B) = B · (∇ × A) − A · (∇ × B)<br />

8. ∇ · ∇ × A = ∇ 2 A<br />

9. ∇ × (∇f) = 0<br />

10. ∇ · (∇ × A) = 0<br />

11. ∇ × (fA) = (∇f) × A + f (∇ × A)<br />

12. ∇ × (A × B) = (B · ∇)A − (A · ∇)B + (∇ · B)A − (∇ · A) B<br />

13. ∇ × (∇ × A) = ∇ (∇ · A) − ∇ 2 A<br />

14.<br />

References<br />

<br />

∂Bx<br />

(A · ∇)B = Ax<br />

∂x<br />

<br />

∂By<br />

+ Ax<br />

<br />

+<br />

Ax<br />

∂x<br />

∂Bz<br />

∂x<br />

∂Bx<br />

+ Ay + Az<br />

∂y<br />

∂By<br />

+ Ay + Az<br />

∂y<br />

∂Bz<br />

+ Ay + Ax<br />

∂y<br />

<br />

∂Bx<br />

∂z<br />

ˆx<br />

<br />

∂By<br />

ˆy<br />

∂z<br />

<br />

ˆz<br />

[1] P. Lorrain, D. R. Corson, F. Lorrain, Electromagnetic Fields <strong>and</strong> Waves, Includinger Electric Circuits, 3rd<br />

ed, W. H. Feeman <strong>and</strong> Company, New York, 1988<br />

2<br />

∂Bz<br />

∂z

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