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The general form of the antiderivative of is , where represents an arbitrary constant. This is because multiple functions differing only by a constant share the same derivative.
Conditions: The function being integrated is .; is an arbitrary constant.
The general form of the antiderivative of is , where represents an arbitrary constant. This is because multiple functions differing only by a constant share the same derivative.
Conditions: The function being integrated is .; is an arbitrary constant.