Field is rotational, if its curl does not vanish. In cylindrical coordinates, curl is:∇×F=aρ(ρ1∂φ∂Az+∂z∂Aφ)+aφ(∂z∂Aρ−∂ρ∂Az)+azρ1(∂ρ∂(ρAφ−∂φ∂Aρ)
For given field, ∇×F=azρ1(∂ρ∂(10ρ))=ρ10az.
From the last formula, curl does not vanish, hence the field is rotational.
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