Can a Vector Field Have Curl without Satisfying Clairaut's Theorem?

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A vector field can exhibit curl when the mixed partial derivatives do not satisfy Clairaut's theorem, specifically when the condition fx ≠ fy is met. The curl is defined as the difference between the partial derivatives of the vector field components, leading to a non-zero quantity. The discussion raises the question of how a vector field can have curl while still adhering to the conditions for zero divergence as dictated by Clairaut's theorem. The theorem states that if a function has continuous second derivatives, the mixed partials should be equal. The conversation highlights the complexities of vector calculus and the implications of these mathematical principles.
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Divergenceofthecurl.jpg


For there to be curl is some vector field fxy cannot equal fyx.
Where fx= P, and fy=Q. Since the (partial of Q with respect to x)-(Partial of P with respect to y) is a non zero quantity giving curl.

I understand that the terms will cancel due to the right-handedness of the definition but we are assuming the these second order partials of P,Q,R follow Clairaut's theroem?

How can clairauts theorem be unsatisfied in order for the vector field to have curl and the clairauts theorem to be satisfied in order for their to be zero divergence?

I hope that makes sense. Thanks
 
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MotoPayton said:
Divergenceofthecurl.jpg


For there to be curl is some scaler field fxy cannot equal fyx.
I have no clue what you mean by this. What "scaler field" are you talking about?
If F is a any vector valued function with differentiable components, then "curl F" is defined.

Where fx= P, and fy=Q. Since the (partial of Q with respect to x)-(Partial of P with respect to y) is a non zero quantity giving curl.

I understand that the terms will cancel due to the right-handedness of the definition but we are assuming the these second order partials of P,Q,R follow Clairaut's theroem?

How can clairauts theorem be unsatisfied in order for the vector field to have curl and the clairauts theorem to be satisfied in order for their to be zero divergence?

I hope that makes sense. Thanks
Clairaut's theorem simply says that if F(x,y) is any function of two variables, with continuous second derivatives, then
\frac{\partial^2F}{\partial x\partial y}= \frac{\partial^2F}{\partial y\partial x}
 
Vector field... my mistake
 

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