/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 78 A 1 -H inductance has \(i_{L}(0)... [FREE SOLUTION] | 91Ó°ÊÓ

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A 1 -H inductance has \(i_{L}(0)=0\) and \(v_{L}(t)\) \(=t \exp (-t)\) for \(0 \leq t\). Using your calculus skills, find an expression for \(i_{L}(t)\). Then, use MATLAB to verify your answer for \(i_{L}(t)\) and to plot \(v_{L}(t)\) and \(i_{L}(t)\) for \(0 \leq t \leq 10 \mathrm{~s}\).

Short Answer

Expert verified
The expression for the current is \(i_L(t) = -t \exp(-t) - \exp(-t) + 1\). Plot in MATLAB to verify.

Step by step solution

01

Understand the Relationship between Voltage and Current in an Inductor

The voltage across an inductor is related to the current through the inductor by the formula \( v_L(t) = L \frac{di_L(t)}{dt} \), where \( L \) is the inductance. For this problem, \( L = 1H \), so the equation simplifies to \( v_L(t) = \frac{di_L(t)}{dt} \).
02

Write the Differential Equation for Current

Given that \( v_L(t) = t \exp(-t) \), substitute this into the simplified inductor equation to get \( \frac{di_L(t)}{dt} = t \exp(-t) \).
03

Integrate the Differential Equation

Integrate both sides to solve for \( i_L(t) \): \[i_L(t) = \int t \exp(-t) \, dt\]Use integration by parts to solve this integral, where you let \( u = t \) and \( dv = \exp(-t) dt \). This results in:\[i_L(t) = -t \exp(-t) - \exp(-t) + C\]
04

Apply Initial Conditions

Using the initial condition \( i_L(0) = 0 \), substitute \( t = 0 \) into the equation: \[0 = -(0) \exp(0) - \exp(0) + C\]\[C = 1\]Therefore, the expression for the current is:\[i_L(t) = -t \exp(-t) - \exp(-t) + 1\]
05

Verify the Solution Using MATLAB

To verify, write a MATLAB script to calculate and plot both \( v_L(t) = t \exp(-t) \) and \( i_L(t) = -t \exp(-t) - \exp(-t) + 1 \) over the interval \( 0 \leq t \leq 10 \). Use `fplot` to graph the functions and `hold on` to overlay the graphs for comparison.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Differential Equations
Differential equations are equations that involve functions and their derivatives. In the context of circuits, these equations are vital in describing how current and voltage change over time. For an inductor circuit, which is what we're focusing on, the relationship between voltage and current is captured by the equation\( v_L(t) = L \frac{di_L(t)}{dt} \). Here, \( L \) represents the inductance, and \( v_L(t) \) and \( i_L(t) \) are the voltage and current, respectively.
In our specific problem, because the inductance \( L = 1 \) Henry, the differential equation simplifies to \( \frac{di_L(t)}{dt} = v_L(t) \). Given that \( v_L(t) = t \exp(-t) \), we substitute this into the equation to form \( \frac{di_L(t)}{dt} = t \exp(-t) \). This establishes a first-order linear differential equation that can be solved to find \( i_L(t) \).
Solving such equations often involves integration or other techniques like Laplace transforms. Understanding how to set up and solve these differential equations is crucial for anyone delving into electronics and circuit design.
Integration by Parts
Integration by parts is a technique used to solve integrals that involve products of functions. This method is particularly useful when dealing with integrals like \( \int t \exp(-t) \, dt \). The formula for integration by parts is given as:
  • \( \int u \, dv = uv - \int v \, du \)
To use this method, we select parts of the integral to be \( u \) and \( dv \). In our calculus problem, let \( u = t \) which makes \( du = dt \), and \( dv = \exp(-t) \, dt \) which implies \( v = -\exp(-t) \).
Using integration by parts leads to the integral\( \int t \exp(-t) \, dt = -t \exp(-t) - \int -\exp(-t) \, dt \). Solving this further, we find:\( i_L(t) = -t \exp(-t) - \exp(-t) + C \), where \( C \) is the constant determined by initial conditions.
This integral process is crucial in solving for current, \( i_L(t) \), and confirms how integration by parts can transform complex calculus problems into solvable components.
MATLAB for Electrical Engineering
MATLAB is a powerful tool frequently used in engineering to solve and visualize complex problems. In electrical engineering, MATLAB can simulate circuits and solve differential equations, helping verify analytical solutions. In our exercise, MATLAB helps us graph the functions \( v_L(t) = t \exp(-t) \) and \( i_L(t) = -t \exp(-t) - \exp(-t) + 1 \).
To verify our solution using MATLAB, follow these basic steps:
  • Define the functions for \( v_L(t) \) and \( i_L(t) \).
  • Use `fplot` to plot both functions over the desired interval, \( 0 \leq t \leq 10 \).
  • Use `hold on` to ensure both plots appear on the same graph.
These steps enable us to visually compare \( v_L(t) \) and \( i_L(t) \), ensuring that the solutions obtained analytically match their graphical representation.
By integrating MATLAB into electrical engineering studies, students can enhance their understanding of circuit behavior and confirm the results they calculate by hand.

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Most popular questions from this chapter

Suppose that we are designing a cardiac pacemaker circuit. The circuit is required to deliver pulses of 1-ms duration to the heart, which can be modeled as a \(500-\Omega\) resistance. The peak amplitude of the pulses is required to be \(5 \mathrm{~V}\). However, the battery delivers only \(2.5 \mathrm{~V}\). Therefore, we decide to charge two equal-value capacitors in parallel from the \(2.5\)-V battery and then switch the capacitors in series with the heart during the 1-ms pulse. What is the minimum value of the capacitances required so the output pulse amplitude remains between \(4.9 \mathrm{~V}\) and \(5.0 \mathrm{~V}\) throughout its 1 -ms duration? If the pulses occur once every second, what is the average current drain from the battery? Use approximate calculations, assuming constant current during the output pulse. Find the ampere-hour rating of the battery so it lasts for five years.

Determine the capacitance of a parallel-plate capacitor having plates \(100 \mathrm{~mm}\) by \(0.3 \mathrm{~m}\) separated by \(0.04 \mathrm{~mm}\). The dielectric constant \(\epsilon=100 \mathrm{pF} / \mathrm{m}\).

At \(t=t_{0}\) the voltage across a certain capacitance \(C\) is zero. A pulse of current flows through the capacitance between \(t_{0}\) and \(t_{0}+\) \(\Delta t\), and the voltage across the capacitance increases to \(V_{f}\). What can you say about the peak amplitude \(I_{m}\) and area under the pulse waveform (i.e., current versus time)? What are the units and physical significance of the area under the pulse? What must happen to the peak amplitude and area under the pulse as \(\Delta t\) approaches zero, assuming that \(V_{f}\) remains the same?

The current in a \(100-\mathrm{mH}\) inductance is given by \(0.5 \sin (1000 t)\) A. Find expressions and sketch the waveforms to scale for the voltage, power, and stored energy, allowing \(t\) to range from 0 to \(3 \pi \mathrm{ms}\). The argument of the sine function is in radians.

We want to store sufficient energy in a \(0.01-\mathrm{F}\) capacitor to supply 5 horsepower (hp) for 1 hour. To what voltage must the capacitor be charged? (Note: One horsepower is equivalent to \(745.7\) watts.) Does this seem to be a practical method for storing this amount of energy? Do you think that an electric automobile design based on capacitive energy storage is feasible?

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