(a) Show that $\mathit{x}\frac{\mathbf{d}}{\mathbf{d}\mathbf{x}}\left(\delta \left(x\right)\right)\mathbf{=}\mathbf{-}\mathit{\delta }\left(x\right)$

[Hint:Use integration by parts.]

(b) Let $\mathit{\theta }\left(x\right)$be the step function:

$\mathit{\theta }\left(x\right)\mathbf{=}\{\begin{array}{ll}1& \mathrm{if}\mathit{}\mathit{x}>0\\ 0,& \mathrm{if}\mathit{}\mathit{x}\le 0\end{array}$

Show that $\frac{\mathbf{d\theta }}{\mathbf{dx}}\mathbf{=}\mathit{\delta }\mathbf{\left(}\mathbf{x}\mathbf{\right)}$

The Dirac Delta function which is represented as $\mathit{\delta }\mathbf{\left(}\mathbf{x}\mathbf{\right)}$, is defined as $\mathit{\theta }\mathbf{\left(}\mathbf{x}\mathbf{\right)}\mathbf{=}\mathbf{\{}\begin{array}{ll}\mathbf{1}& \mathbf{}\mathbf{x}\mathbf{\ne }\mathbf{0}\\ \mathbf{0}\mathbf{,}& \mathbf{}\mathbf{x}\mathbf{=}\mathbf{0}\end{array}$, .the Dirac delta function has the property ${\mathbf{\int }}_{\mathbf{-}\mathbf{\infty }}^{\mathbf{\infty }}\mathit{f}\mathbf{\left(}\mathbf{x}\mathbf{\right)}\mathit{\delta }\mathbf{\left(}\mathbf{x}\mathbf{\right)}\mathit{d}\mathit{x}\mathbf{=}\mathit{f}\mathbf{\left(}\mathbf{0}\mathbf{\right)}$, where $\mathit{f}\mathbf{\left(}\mathbf{x}\mathbf{\right)}$is a continuous containing$\mathit{x}\mathbf{=}\mathbf{0}$.

(a)

Let function $u\left(x\right)=\delta \left(x\right)$and $v\left(x\right)=x$. Differentiate $u\left(x\right)=\delta \left(x\right)$and $v\left(x\right)=x$with respect to $x$.

$\begin{array}{l}u\text{'}\left(x\right)=\frac{d}{dx}\delta \left(x\right)\\ v^{\text{'}}\left(x\right)=1\end{array}$

Substitute $\delta \left(x\right)$for $u$, $x$for $v\left(x\right)$into $\int udv=uv-\int vdu$as,

localid="1657365897288" $$\begin{gathered} {\int }_{-\infty }^{\infty }\delta \left(x\right)dx={\int }_{-\infty }^{\infty }c\left(x\right)\times 1dx \\ ={\overline{)x\delta \left(x\right)}}_{-\infty }^{\infty }-{\int }_{-\infty }^{\infty }x\frac{d}{dx}\left(\delta \left(x\right)\right)dx \end{gathered}$$ ….. (1)

Define $x\delta \left(x\right)$as,

$x\delta \left(\mathrm{x}\right)=\{\begin{array}{ll}0\times \infty & \mathrm{x}=0\\ x=0& \mathrm{x}\ne 0\end{array}$

Thus the value of $x\delta \left(x\right)$is 0 for all x.

Hence, $x\delta {\overline{)\left(x\right)}}_{-\infty }^{\infty }=0$.

Now equation (1) can be rewritten as,

$$\begin{gathered} {\int }_{-\infty }^{\infty }\delta \left(x\right)dx={\int }_{-\infty }^{\infty }\times \frac{d}{dx}\left(\delta \left(x\right)\right)dx \\ ={\int }_{-\infty }^{\infty }x\frac{d}{dx}\left(\delta \left(x\right)\right)dx \end{gathered}$$ ……. (2)

Equation (2) can be rewritten as $x\frac{\mathrm{d}}{\mathrm{dx}}\left(\mathrm{\delta }\left(\mathrm{x}\right)\right)=-\delta \left(\mathrm{x}\right)$

(b)

According to equation (1), ${\int }_{-\infty }^{\infty }\delta \left(x\right)dx={\overline{)x\delta \left(x\right)}}_{-\infty }^{\infty }-{\int }_{-\infty }^{\infty }\times \frac{d}{dx}\left(\delta \left(x\right)\right)dx$. The second property of Dirac Delta function can be written as follows

$$\begin{gathered} {\int }_{-\infty }^{\infty }f\left(x\right)\left(\frac{d\theta }{dx}\right)dx=f\left(x\right)\theta {\overline{)\left(x\right)}}_{-\infty }^{\infty }-{\int }_{-\infty }^{\infty }\frac{df}{dx}\left(\theta \left(x\right)\right)dx \\ =f\left(x\right)\theta {\overline{)\left(x\right)}}_{-\infty }^{\infty }-\left[{\int }_{-\infty }^0\frac{df}{dx}\left(\theta \left(x\right)\right)dx+{\int }_0^{\infty }\frac{df}{dx}\left(\theta \left(x\right)\right)dx\right] \\ =f\left(x\right)\theta {\overline{)\left(x\right)}}_{-\infty }^{\infty }-\left[0+{\int }_0^{\infty }\frac{df}{dx}dx\right] \\ =f\left(x\right)(\infty )-{\int }_0^{\infty }\frac{df}{dx}dx \end{gathered}$$

Solve further as,

$$\begin{gathered} {\int }_{-\infty }^{\infty }f\left(x\right)\left(\frac{d\theta }{dx}\right)dx=(f\left(\infty \right)-f\left(0\right)) \\ =f\left(0\right) \\ ={\int }_{-\infty }^{\infty }f\left(x\right)\delta \left(x\right)dx \end{gathered}$$

Thus, it can be written as $\left(\frac{d\theta }{dx}\right)=\delta x$.