For , a function is its weak derivative when
for every test function . Equivalently, the distributional derivative of is represented by the locally integrable function .
For , the ordinary derivative away from zero is
This bounded function is locally integrable. For a test function , integration by parts on and produces boundary terms at zero which cancel because is continuous there and . Hence
Therefore has the weak derivative
The jump in the ordinary derivative creates no Dirac delta function; such a term would arise from a jump in the function itself.

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