Understanding the First Order Prototype Solution in Time Domain

In summary, the solution in the time domain for the first order prototype driven by a step function can be found by solving the differential equation using the integrating factor method. The solution consists of a transient and steady state component, with the steady state component simply being the value of the step function.
  • #1
Dustinsfl
2,281
5
Consider the first order prototype,
\[
\frac{dy(t)}{dt} + \frac{1}{\tau}y(t) = f(t),\]
driven by a step function,
\[
f(t) = \mathcal{U}(t) =
\begin{cases}
1, & \text{if } t \geq 0\\
0, & \text{otherwise}
\end{cases}
\]
Find the solution in the time domain. That is, find the transient and steady state solution.

What does this mean? The second part is use a Laplace transform. I can find the solution that way no problem but not sure about what I need to do for finding the solution in the time domain.
 
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  • #2
The solution in the time domain can be found by solving the differential equation. Since we have a first order differential equation, the solution can be found using the integrating factor method. We start by rewriting the differential equation as:$$\frac{dy}{dt} + \frac{1}{\tau}y=f(t)$$Now, we multiply both sides of the equation by the integrating factor $e^{\frac{t}{\tau}}$ to obtain:$$e^{\frac{t}{\tau}}\frac{dy}{dt} + e^{\frac{t}{\tau}}\frac{1}{\tau}y=e^{\frac{t}{\tau}}f(t)$$We can now integrate both sides of the equation with respect to $t$ to get:$$e^{\frac{t}{\tau}}y(t) = \int_{0}^{t}e^{\frac{x}{\tau}}f(x)dx + C_1$$where $C_1$ is an integration constant. The transient solution is given by the integral on the right hand side and the steady state solution is obtained when we let $t\rightarrow \infty$. In this case, the steady state solution is simply the value of the step function $f(t)$, that is, $f(t)=1$ for all $t\geq 0$.Therefore, the solution of the differential equation is given by:$$y(t) = e^{-\frac{t}{\tau}}\left(\int_{0}^{t}e^{\frac{x}{\tau}}dx + C_1\right)+ 1$$where $C_1$ is an integration constant.
 

FAQ: Understanding the First Order Prototype Solution in Time Domain

What is a First Order Prototype Solution in Time Domain?

A First Order Prototype Solution in Time Domain is a mathematical representation of a physical system that follows first order differential equations in the time domain. It is used in engineering and science to model and understand the behavior of various systems.

What are some examples of systems that can be modeled using a First Order Prototype Solution in Time Domain?

Some examples of systems that can be modeled using a First Order Prototype Solution in Time Domain include electrical circuits, mechanical systems, chemical reactions, and biological processes.

How is a First Order Prototype Solution in Time Domain different from other types of mathematical models?

A First Order Prototype Solution in Time Domain differs from other types of mathematical models in that it specifically focuses on modeling systems that follow first order differential equations in the time domain. This makes it particularly useful for analyzing systems that involve changes over time.

What are the steps involved in understanding a First Order Prototype Solution in Time Domain?

The first step in understanding a First Order Prototype Solution in Time Domain is to identify the system and its components. Then, the differential equations that govern the system's behavior are determined. The next step is to solve these equations using appropriate mathematical techniques. The solution is then analyzed and interpreted to gain insights into the behavior of the system.

Why is it important to understand First Order Prototype Solution in Time Domain?

Understanding First Order Prototype Solution in Time Domain is important because it allows us to predict and analyze the behavior of various physical systems. This can help in designing and optimizing systems, troubleshooting issues, and making informed decisions in various fields such as engineering, physics, and biology.

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