Vector, cross product, and integral

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SUMMARY

The discussion focuses on evaluating the integral of the cross product of two vector fields, \textbf{F} and \textbf{v}, in \mathbb{R}^3. The equation presented is {\int \textbf{F} \times \texttt{d}\textbf{v}}, where \texttt{d}\textbf{v} is defined as (\nabla \otimes \textbf{v} ) \texttt{d}\textbf{r}. The solution involves calculating the cross product using the determinant method, leading to three path integrals over a specified path \textbf{r}. The correctness of this approach is confirmed within the discussion.

PREREQUISITES
  • Understanding of vector calculus, specifically cross products.
  • Familiarity with integral calculus in multiple dimensions.
  • Knowledge of vector fields in \mathbb{R}^3.
  • Proficiency in using the gradient operator (\nabla) and tensor products.
NEXT STEPS
  • Study the properties of vector fields in \mathbb{R}^3.
  • Learn about path integrals and their applications in vector calculus.
  • Explore the use of the gradient operator (\nabla) in vector calculus.
  • Investigate the implications of the cross product in physics and engineering contexts.
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Students and professionals in mathematics, physics, and engineering who are working with vector calculus, particularly those dealing with vector fields and integrals in three-dimensional space.

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[SOLVED] Vector, cross product, and integral

Homework Statement


Evaluate:

{\int \textbf{F} \times \texttt{d}\textbf{v}}.

\textbf{F} and \textbf{v} are both vector fields in \mathbb{R}^3

Homework Equations



\texttt{d}\textbf{v} = (\nabla \otimes \textbf{v} ) \texttt{d}\textbf{r}

The Attempt at a Solution


<br /> \begin{array}{ll}<br /> \textbf{F} \times \texttt{d}{\textbf{v}} &amp;= \left( {<br /> \begin{array}{c}<br /> {F_2 \texttt{d}v_3 - F_3 \texttt{d}v_2 } \\<br /> {F_1 \texttt{d}v_2 - F_2 \texttt{d}v_1 } \\<br /> {F_1 \texttt{d}v_3 - F_3 \texttt{d}v_1 } \\<br /> \end{array}<br /> \right ) \\ <br /> &amp;= \left( <br /> \begin{array}{c}<br /> {F_2 \nabla v_3 \cdot \texttt{d}{\textbf{r}} - F_3 \nabla v_3 \cdot \texttt{d}{\textbf{r}}} \\<br /> {F_1 \nabla v_2 \cdot \texttt{d}{\textbf{r}} - F_2 \nabla v_1 \cdot \texttt{d}{\textbf{r}}} \\<br /> {F_1 \nabla v_3 \cdot \texttt{d}{\textbf{r}} - F_3 \nabla v_1 \cdot \texttt{d}{\textbf{r}}} \\<br /> \end{array} \right) \\ <br /> \end{array}

This can then be solved as three path integrals over some path \textbf{r}. Is this correct?
 
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Yes, that is correct.
 

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