Expanding Vector Identity: ∆ x [(u.∆)u]

In summary, the conversation is discussing how to expand the expression ∆ x [(u.∆)u], with the initial confusion about the notation and variables used. The conversation then progresses to finding the expression (u.∆)u and transforming it to subscript notation to perform the dot product.
  • #1
Fairy111
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0

Homework Statement



Could someone please tell me how to expand:

∆ x [(u.∆)u]

Homework Equations





3. The Attempt at a Solution
thankyou
 
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  • #2
do you mean nabla again, and i assume u is a vector? so
[tex] \nabla \times ((u \bullet \nabla) u) [/tex]

start first with finding the expression
[tex] (u \bullet \nabla) u [/tex]

i think for teh expression in the brackets, you consider it as an operator, so transforming to the subscript notation, where x_i is the ith coordinate, and we sum over repeated indicies to perform the dot product
[tex] u \bullet \nabla = u_i \frac{\partial}{\partial x_i} = u_x \frac{\partial}{\partial x} + u_y \frac{\partial}{\partial y} + u_z \frac{\partial}{\partial z} [/tex]
 
Last edited:

FAQ: Expanding Vector Identity: ∆ x [(u.∆)u]

What is "Expanding Vector Identity: ∆ x [(u.∆)u]"?

Expanding Vector Identity: ∆ x [(u.∆)u] is a mathematical formula used to expand the vector identity of a vector function u.

How is "Expanding Vector Identity: ∆ x [(u.∆)u]" derived?

The formula is derived using vector calculus and the product rule for differentiation.

What is the significance of "Expanding Vector Identity: ∆ x [(u.∆)u]"?

The formula has many applications in physics and engineering, particularly in the study of fluid dynamics and electromagnetism.

Can "Expanding Vector Identity: ∆ x [(u.∆)u]" be used for any type of vector function?

Yes, the formula is applicable to any vector function, as long as the function is differentiable.

Are there any limitations to using "Expanding Vector Identity: ∆ x [(u.∆)u]"?

The formula may not be applicable in cases where the vector function is not differentiable or when dealing with non-Euclidean spaces.

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