Undergrad How is rotation related to the curl of a vector field?

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The curl of a vector field indicates the presence of rotation, with a zero curl signifying that the field is irrotational. This relationship is illustrated through Stokes' theorem, which connects curl to line integrals around a point; a non-zero integral indicates rotation. A practical analogy involves a paddlewheel placed at a point in the field—if it spins, rotation is present. It is important to note that a single vector cannot possess a curl; the concept applies exclusively to vector fields. Understanding these principles is crucial for grasping the dynamics of vector calculus.
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If the curl of a vector is 0 e,g ##\vec \nabla×\vec A=0## the vector A is said to be irrotational,can anyone please tell how rotation is involved with ##curl## of a vector??
 
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Point of order: A vector by itself cannot have a curl. The concept makes no sense. All differential operators you will encounter in vector analysis involve fields. In the case of the curl, a vector field.
 
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Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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