Context: I am currently learning about convolution integrals as they apply to circuits (LTI specifically, if I understand it correctly.
(For the following, continue under the assumption that \$\theta(t-c)\$ is always used as the Heaviside step function.
Let's say we have a simple step input: \$x(t)=\theta(t-2)\$ (step input, delayed by two seconds.)
But I am provided the impulse response \$h(t)=\theta(t+3)-\theta(t-3)\$
The short version of this question is this: How should I work with an impulse response defined before \$t=0\$ (with regards to convolution)?
Some more details:
The only way I get the same answers is to do it in a way that seems wrong as I understand these concepts.
I understand that to find the output \$y(t)\$, I am interested in the convolution $$y(t)=x(t)*h(t)\equiv\int_{-\infty}^\infty [x(t)-h(t-\tau)]d\tau$$ $$\equiv\int_{-\infty}^\infty [x(t-\tau)-h(t)]d\tau$$
When I do this using the response as the translated function, I end up with a function that is defined on the boundaries of \$t<-1\$ (no overlap), \$-1\leq t<5\$ (some overlap), and \$5\leq t\$ (full overlap.)
This does not make sense to me, as I am showing output before an input is applied over the period t=\$[-1,1)\$
I also understand that I have the option of utilizing the Laplace transform to solve the convolution.
$$y(t)=x(t)*h(t)\equiv X(s)H(s)$$
(Where X(s) and H(s) are the Laplace transforms of x(t) and h(t), respectively)
This is where things start to confuse me as if I take the Laplace transform of the impulse response, it will include the following step:
$$\mathscr{L}[\theta(t+3)](s)=\int_0^\infty\theta(t+3)e^{-st}dt\equiv\int_0^\infty e^{-st}dt=\frac{1}{s}$$
As \$\theta(t+3)=1\$ over the interval \$[0,\infty)\$.
When you continue on with the product in this way, you get
$$y(t)=(t-2)\theta(t-2)-(t-5)\theta(t-5)$$
If you ignore the one-sided restriction, you get:
$$y(t)=(t+1)\theta(t+1)-(t-5)\theta(t-5)$$
The first appears unrelated, the second perfectly matches the response from earlier (when you ignore that the input starts at \$t=2\$
So my understanding of the 'impulse response' doesn't currently fit with something that is defined before \$t=0\$, and I think that is reflected in the results. I'm trying to figure out what I am missing to understand these cases where I am provided impulse that is provided with a definition such that \$h(t)\neq0\$ for \$t<0\$