Bob44
				
				
			 
			
	
	
	
		
	
	
			
		
		
			
			
				
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Let us take the Ampere-Maxwell law
$$\nabla \times \mathbf{B} = \mu_0\,\mathbf{J}+\frac{1}{c^2}\frac{\partial \mathbf{E}}{\partial t}.\tag{1}$$
Assume we produce a spark that is so fast that the ##\partial \mathbf{E}/\partial t## term in eqn.##(1)## has not yet been produced by Faraday’s law of induction
$$\nabla \times \mathbf{E}=-\frac{\partial \mathbf{B}}{\partial t}\tag{2}$$
since the current density ##\mathbf{J}## has not yet had time to generate the magnetic field ##\mathbf{B}##.
By integrating eqn.##(1)## and using Stokes law we find
$$\oint \mathbf{B}\cdot d\mathbf{l}=\mu_0 I,\tag{3}$$
$$B=\frac{\mu_0 I}{2\pi r}.\tag{4}$$
This seems to imply that a tangential magnetic field with strength ##B## appears instantly around the spark at all distances ##r##.
Does this contradict causality?
				
			$$\nabla \times \mathbf{B} = \mu_0\,\mathbf{J}+\frac{1}{c^2}\frac{\partial \mathbf{E}}{\partial t}.\tag{1}$$
Assume we produce a spark that is so fast that the ##\partial \mathbf{E}/\partial t## term in eqn.##(1)## has not yet been produced by Faraday’s law of induction
$$\nabla \times \mathbf{E}=-\frac{\partial \mathbf{B}}{\partial t}\tag{2}$$
since the current density ##\mathbf{J}## has not yet had time to generate the magnetic field ##\mathbf{B}##.
By integrating eqn.##(1)## and using Stokes law we find
$$\oint \mathbf{B}\cdot d\mathbf{l}=\mu_0 I,\tag{3}$$
$$B=\frac{\mu_0 I}{2\pi r}.\tag{4}$$
This seems to imply that a tangential magnetic field with strength ##B## appears instantly around the spark at all distances ##r##.
Does this contradict causality?
			
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