Proof of Vector Identity Using Standard Identities | C^2 Scalar Functions

Hi madachi! :smile:(just got up :zzz: …)… Then we use identity 8 to show that the vector field on the first term equal to 0 right? Not sure how you get it from 8 :redface: …how about 13? :smile:Sorry, I meant identity 9. Since that is the only identity that involves the curl of a vector field, and it says that the divergence of the curl is 0.Using that, we can rewrite \nabla \cdot (\nabla g \times \nabla h ) as - \nabla \times (\nabla \times (\nabla g \
  • #1
madachi
29
0

Homework Statement



Let [itex] f(x,y,z), g(x,y,z), h(x,y,z) [/itex] be any [itex] C^2 [/itex] scalar functions. Using the standard identities of vector analysis (provided in section 2 below), prove that

[itex] \nabla \cdot ( f \nabla g \times \nabla h ) = \nabla f \cdot ( \nabla g \times \nabla h) [/itex]


Homework Equations



Note: The identities below require [itex] f,g,F,G [/itex] to be suitable differentiable, either order [itex] C^1 [/itex] or [itex] C^2 [/itex].

[itex] 1. \nabla (f+g) = \nabla f + \nabla g [/itex]
[itex] 2. \nabla (\lambda f) = \lambda \nabla f [/itex], where [itex] \lambda [/itex] is a constant
[itex] 3. \nabla (fg) = f \nabla g + g \nabla f [/itex]
[itex] 4. \nabla (\frac{f}{g}) = \frac{g \nabla f - f \nabla g}{g^2} [/itex]
[itex] 5. \nabla \cdot (F+G) = \nabla \cdot F + \nabla \cdot G [/itex]
[itex] 6. \nabla \times (F+G) = \nabla \times F + \nabla \times G [/itex]
[itex] 7. \nabla \cdot (fF) = f \nabla \cdot F + F \cdot \nabla f [/itex]
[itex] 8. \nabla \cdot (F \times G) = G \cdot (\nabla \times F ) - F \cdot (\nabla \times G) [/itex]
[itex] 9. \nabla \cdot (\nabla \times F) = 0 [/itex]
[itex] 10. \nabla \times (fF) = f \nabla \times F + \nabla f \times F [/itex]
[itex] 11. \nabla \times (\nabla f) = 0 [/itex]
[itex] 12. {\nabla}^2 (fg) = f{\nabla}^2 g + g{\nabla}^2 f + 2 \nabla f \cdot \nabla g [/itex]
[itex] 13. \nabla \cdot (\nabla f \times \nabla g) = 0 [/itex]
[itex] 14. \nabla (f \nabla g - g \nabla f) = f {\nabla}^2 g - g {\nabla}^2 f [/itex]


The Attempt at a Solution



Using identity 8,

[itex] \nabla \cdot ( f \nabla g \times \nabla h ) = \nabla h \cdot (\nabla \times (f \nabla g)) - (f \nabla g) \cdot (\nabla \times (\nabla h)) [/itex]

One of the terms on RHS, [itex] \nabla \times (\nabla h) = 0 [/itex] by identity 11.

So the equation reduces to

[itex] \nabla \cdot ( f \nabla g \times \nabla h ) = \nabla h \cdot (\nabla \times (f \nabla g)) [/itex]

I'm stuck here. There is no identity that I can use to further simplify this to the one required. (from what I can see, or am I wrong?) How do we proceed?

Thanks!
 
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  • #2
Welcome to PF!

Hi madachi! Welcome to PF! :wink:

Looking at the RHS of the answer, you need to separate the f from the g and h, and 8. won't do that.

But 7. will, so try 7. :smile:
 
  • #3
Might be a naive question, but is there an f missing on the left side in this equation?
[tex] \nabla \cdot ( f \nabla g \times \nabla h ) = \nabla f \cdot ( \nabla g \times \nabla h) [/tex]

If so, here's the corrected version.
[tex] \nabla \cdot ( f \nabla g \times \bold{f} \nabla h ) = \nabla f \cdot ( \nabla g \times \nabla h) [/tex]
 
  • #4
tiny-tim said:
Hi madachi! Welcome to PF! :wink:

Looking at the RHS of the answer, you need to separate the f from the g and h, and 8. won't do that.

But 7. will, so try 7. :smile:

How do we use 7 ? Because the original equation doesn't look like "the form" of identity 7. Could you show me the first step?

Thanks!

Mark44 said:
Might be a naive question, but is there an f missing on the left side in this equation?
[tex] \nabla \cdot ( f \nabla g \times \nabla h ) = \nabla f \cdot ( \nabla g \times \nabla h) [/tex]

If so, here's the corrected version.
[tex] \nabla \cdot ( f \nabla g \times \bold{f} \nabla h ) = \nabla f \cdot ( \nabla g \times \nabla h) [/tex]

No there isn't an f missing on the left side in the equation.

Thanks.
 
  • #5
Hi madachi! :smile:

(have a nabla: ∇ :wink:)

f is f, and F is ∇g x ∇h :smile:
 
  • #6
tiny-tim said:
Hi madachi! :smile:

(have a nabla: ∇ :wink:)

f is f, and F is ∇g x ∇h :smile:

Thanks! Using what you suggest,

So

[itex] \nabla \cdot ( f \nabla g \times \nabla h) [/itex]
= [itex] f \nabla \cdot (\nabla g \times \nabla h ) + ( \nabla g \times \nabla h ) \cdot \nabla f [/itex]

Then we use identity 8 to show that the vector field on the first term equal to 0 right? And the second term on RHS is just the identity that we are required to show?

Thanks!
 
  • #7
Hi madachi! :smile:

(just got up :zzz: …)
madachi said:
… Then we use identity 8 to show that the vector field on the first term equal to 0 right?

Not sure how you get it from 8 :redface:

how about 13? :smile:
 

Related to Proof of Vector Identity Using Standard Identities | C^2 Scalar Functions

1. What is a vector identity?

A vector identity is a mathematical equation that expresses a relationship between different vector quantities. It is used to simplify and manipulate vector equations and can be derived using various mathematical techniques such as the dot product, cross product, and vector calculus.

2. Why is vector identity important in science?

Vector identities are crucial in science because they allow us to solve complex problems involving vector quantities in a more efficient and elegant manner. They also help us understand the underlying principles and relationships between different vector quantities in various physical phenomena.

3. How can vector identities be proven?

Vector identities can be proven using mathematical techniques such as algebraic manipulation, vector calculus, and geometric reasoning. These techniques involve breaking down the vector equations into simpler forms and then showing that both sides of the equation are equal through logical steps.

4. Are there different types of vector identities?

Yes, there are various types of vector identities, including trigonometric identities, product identities, and differential identities. These identities are used in different areas of science, such as mechanics, electromagnetism, and quantum mechanics, to solve specific problems involving vector quantities.

5. How can vector identities be applied in real-world situations?

Vector identities have numerous applications in real-world situations, such as in engineering, physics, and computer graphics. They are used to calculate forces, velocities, and accelerations in mechanical systems, to model and simulate electromagnetic fields, and to create realistic 3D graphics in computer games and animations.

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