Problem with integrating heaviside function.

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perpich08
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Homework Statement


I need to find the integral of the following equation..

integral from 0 to 8 of {(2H[x-0]+2H[x-4])*(x/8)}dx

The Attempt at a Solution


Im am not sure what the integral of the heaviside function is?
is it 1 or 0?

Any help would be appreciated!
Thanks
 
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Write your function as a piecewise defined function and you will see how to integrate it.

f(x) = ? if 0 < x < 4
f(x) = ? if 4 < x < 8

Remember H(x) = 0 if x < 0 and H(x) = 1 if x > 0.

Also drawing the graph might help.
 
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perpich08 said:
Im am not sure what the integral of the heaviside function is?

Use integration by parts and the fact that [itex]h'(x - x_{0}) = \delta(x - x_{0})[/itex]:

[tex] \int_{a}^{b}{h(x - x_{0}) \, dx} = \left. x \, h(x - x_{0}) \right|^{b}_{a} - \int_{a}^{b}{x \, \delta(x - x_{0}) \, dx}[/tex]

Next, the integral with the Dirac delta-function can be evaluated using its property:

[tex] \int_{a}^{b}{x \, \delta(x - x_{0}) \, dx} = x_{0} \, h(x_{0} - a) \, h(b - x_{0})[/tex]

where the product of the two Heaviside functions ensures that [itex]x_{0}[/itex] is inside the segment [itex]x_{0} \in \left[a, b \right][/itex]. The integrated-out part is:

[tex] b \, h(b - x_{0}) - a \, h(a - x_{0})[/tex]

Combining everything together gives:

[tex] \int_{a}^{b}{h(x - x_{0}) \, dx} = b \, h(b - x_{0}) - a \, h(a - x_{0}) - x_{0} \, h(x_{0} - a) \, h(b - x_{0})[/tex]
 
As a check, let us differentiate it w.r.t. [itex]b[/itex]:

[tex] \frac{\partial}{\partial b} \left( b \, h(b - x_{0}) \right) = 1 \cdot h(b - x_{0}) + b \cdot \delta(b - x_{0}) = h(b - x_{0}) + x_{0} \, \delta(b - x_{0})[/tex]

[tex] \frac{\partial}{\partial b} \left( -a \, h(a - x_{0}) \right) = 0[/tex]

[tex] \frac{\partial}{\partial b} \left( -x_{0} \, h(b - x_{0}) h(x_{0} - a) \right) = -x_{0} \, \delta(b - x_{0}) \, h(x_{0} - a) = -x_{0} \, \delta(b - x_{0}) \, h(b - a) = -x_{0} \delta(b - x_{0})[/tex]

where again we used the derivative of the Heaviside step function and a consequence of the properties of the Dirac delta-function ([itex]x \, \delta(x - x_{0}) = x_{0} \, \delta(x - x_{0})[/itex]) as well as the assumption that [itex]b > a[/itex]. Combining everything together and substituting [itex]b \rightarrow x[/itex]. we see that we get the integrand. Also, if [itex]b = a[/itex], the first two terms cancel and the last cancels because [itex]h(a - x_{0}) h(x_{0} - a)[/itex] is always zero. So, according to the fundamental theorem of calculus, we should get the correct result.
 
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Of course, you can always write:

[tex] \int_{0}^{8}{\left( 2 h(x) + 2 h(x - 4) \right) \frac{x}{8} \, dx} = \frac{1}{4} \, \left[\int_{0}^{8}{x \, h(x) \, dx} + \int_{0}^{8}{x \, h(x - 4) \, dx}\right][/tex]

[tex] \frac{1}{4} \, \left[ \int_{0}^{8}{x \, dx} + \int_{4}^{8}{x \, dx}\right][/tex]

and do the remaining elementary integrals :)
 
Thanks guys! I think I can figure it out now
 
I would consider using integration by parts for integrating the Heaviside function "overkill".

If a<0, then H(x)= 0 for all [itex]x\le 0[/itex] so [itex]\int_{-\infty}^a H(x)dx= 0[/itex]. For [itex]a\ge 0[/itex], [itex]\int_{-\infty}^a H(x)dx= \int_0^a H(x)dx[/itex][itex]= \int_0^a dx= a[/itex].

For the "indefinite integral" [itex]\int H(x)dx[/itex] is 0+ C for x< 0, x+ C for [itex]x\ge 0[/itex].