Laplace transforms of Heavyside functions

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The discussion centers on the application of Laplace transforms to Heaviside functions, specifically regarding the function g(t) defined piecewise. The confusion arises from the transformation of the term 2tH(t-1) into the form 2(t-1)H(t-1) to facilitate the Laplace transform. This adjustment is necessary because the Laplace transform requires the function to be expressed as f(t)H(t). The explanation clarifies that H(t) indicates the function is active only for t > 0, allowing the transform to be computed from a to infinity without concern for values before a. Understanding this manipulation is key to successfully applying Laplace transforms to piecewise functions involving Heaviside functions.
iceman_ch
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Ok, I have two question that have me stuck. I understand heavyside functions and how to do a laplace transform on them but, they've thrown me a curve ball. I'm sure I'm just making it more complicated then it needs to be.

Here is problem number one.

g(t) = 2t for 0 <= t < 1;
2 for 1 <= t;

This is the same as:

g(t) = 2tH(t) - 2tH(t-1) + 2H(t-1)

The next step is were I'm confused. The book finished setting up this problem for a laplace transform by changing the equation to this:

g(t) = 2tH(t) - 2(t-1)H(t-1)

Why did they change it like this and how did they do this. I'm know I'm over looking something but, I'm not sure what. Any help would be great.
 
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to take the laplace transform of the heaviside function, you want it to be of the form f(t)H(t). Since 2tH(t-1) isn't of this form, the author uses some simple algebra to get something that is.
 
H(t)=1 if t>0 and 0 if t<0

Now H(t-a)=1 if t-a>0 and 0 if t-a<0=> H(t-a)=1 if t>a and 0 if t<a.

this means that the laplace transform from 0 to a is going to be zero, so there is nothing to worry about it. Just take the laplace transfrom from a to infty.
 

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