Are Both Conditions Necessary to Confirm a Conservative Electric Field?

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To confirm if an electric field is conservative, it is sufficient to check either the condition that the curl of the electric field is zero (∇ x E = 0) or that the line integral around a closed loop is zero (∮ E·dl = 0). While both conditions are equivalent, testing the curl is often simpler and more straightforward. Understanding that a conservative field can be expressed as the gradient of a scalar potential aids in calculations. Therefore, it is not necessary to test both conditions; testing one is adequate to confirm the field's conservativeness.
Spoony
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I'm being taught electromagnetism at university, but there's one definition that has been left slightly ambiguous for an electric field to be conservative I've been taught that
1) \nablaxE = 0
But I've also been taught that
2) \oint E.dl = 0

But I am not sure if 1) & 2) have to be true for it to be conservitive.
OR that if 1) is true then 2) is true (and visa versa) ie, 1) \Leftrightarrow 2)

So do i have to test for both to check the field is conservitive, or just one and say it implies the other.
 
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2. is a definition, which is equivalent to saying a vector field E is conservative if is can be written as the gradient of some scalar field.
1. can be shown to be equivalent to 2. by writing \mathbf{E}=\nabla\phi and taking the curl.

So, in short, no you don't need to test both. Most of the time it's a lot easier to calculate 1. to check whether the vector field is conservative.
 
Thanks dude :)
 
In addition to what cristo said, knowing that (2) is true for a conservative field can make later calculations easier, but as cristo said, (1) is usually easier to calculate. So if you're asked to prove whether a vector field is conservative it is usually best to use (1), but it is also useful to know (2) as well.
 
It may be shown from the equations of electromagnetism, by James Clerk Maxwell in the 1860’s, that the speed of light in the vacuum of free space is related to electric permittivity (ϵ) and magnetic permeability (μ) by the equation: c=1/√( μ ϵ ) . This value is a constant for the vacuum of free space and is independent of the motion of the observer. It was this fact, in part, that led Albert Einstein to Special Relativity.
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