On each interval , , the function is on and on . Its ordinary derivative exists off and is the locally integrable function
Assign arbitrary values at the endpoints. For a test function , split at these corners and apply integration by parts on each piece. The adjacent boundary terms cancel because is continuous, and only finitely many pieces meet the compact support of . Hence
The distributional derivative is exactly the regular distribution of the ordinary derivative defined almost everywhere. There are no Dirac delta distributions in this first distributional derivative: corners change slope, while a jump of the function itself would create a point mass.

Articles by others on the same topic (0)

There are currently no matching articles.