- #1
Amok
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I would have said it is 0, but then why is it that a twice derivable function is a function like, for example, f(x) = x. I've been studying maths for a while, but I had never asked myself this question until I came across the Heaviside function:
[tex] H(x) = 1 \ if\ x\geq 0\ and\ H(x)=0\ if\ x<0[/tex]
The derivative of this function (in the distributional sense) is the Dirac delta function:
Let [tex]\varphi \in S [/tex], the Schwartz space then:
[tex] \langle T_{H}^{(1)},\varphi \rangle = - \int_{- \infty}^{+ \infty} H(x) \varphi '(x) dx = - \int_{0}^{+ \infty} \varphi '(x) dx = -[\varphi (x)]_{0}^{\infty} = \varphi (0) = \langle \delta, \varphi \rangle = \delta [/tex]
And not,
[tex] \langle T_{H}^{(1)},\varphi \rangle = \int_{- \infty}^{+ \infty} H'(x) \varphi (x) dx = \int_{0}^{+ \infty} 0 \cdot \varphi (x) dx + \int_{- \infty}^{0} 0 \cdot \varphi (x) dx = 0 [/tex]
Which implies that H(x) is not derivable in the 'normal' sense (which implies 0 doesn't have a derivative).
EDIT: I just realized the Heaviside function is not differentiable at 0 (it is not even continuous)!
[tex] H(x) = 1 \ if\ x\geq 0\ and\ H(x)=0\ if\ x<0[/tex]
The derivative of this function (in the distributional sense) is the Dirac delta function:
Let [tex]\varphi \in S [/tex], the Schwartz space then:
[tex] \langle T_{H}^{(1)},\varphi \rangle = - \int_{- \infty}^{+ \infty} H(x) \varphi '(x) dx = - \int_{0}^{+ \infty} \varphi '(x) dx = -[\varphi (x)]_{0}^{\infty} = \varphi (0) = \langle \delta, \varphi \rangle = \delta [/tex]
And not,
[tex] \langle T_{H}^{(1)},\varphi \rangle = \int_{- \infty}^{+ \infty} H'(x) \varphi (x) dx = \int_{0}^{+ \infty} 0 \cdot \varphi (x) dx + \int_{- \infty}^{0} 0 \cdot \varphi (x) dx = 0 [/tex]
Which implies that H(x) is not derivable in the 'normal' sense (which implies 0 doesn't have a derivative).
EDIT: I just realized the Heaviside function is not differentiable at 0 (it is not even continuous)!
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