Problem 2
Question
For an object in damped harmonic motion with initial amplitude \(k\) , period \(2 \pi / \omega,\) and damping constant \(c\) , find an equation that models the displacement \(y\) at time \(t\) if (a) \(y=0\) at time \(t=0 : y=\)________ (b) \(y=a\) at time \(t=0 : y=\) _______
Step-by-Step Solution
Verified Answer
(a) \(y(t) = k e^{-ct/2} \sin(\omega t)\); (b) \(y(t) = k e^{-ct/2} \left( \cos(\omega t) \frac{a}{k} - \sin(\omega t) \sqrt{1 - \left(\frac{a}{k}\right)^2} \right) \)."
1Step 1: Understanding Damped Harmonic Motion
Damped harmonic motion can be described with an equation of the form \( y(t) = Ae^{-ct/2} \cos(\omega t + \phi) \), where \( A \) is the initial amplitude, \( c \) is the damping constant, and \( \omega \) is the angular frequency related to the period by \( \omega = \frac{2\pi}{T} \). The term \( \phi \) represents the phase angle.
2Step 2: Case (a): Initial Displacement is Zero
For case (a), where the initial displacement \( y=0 \) at \( t=0 \), we need to determine the conditions that lead to this result. Solving \( y(0) = A e^{0} \cos(\phi) = 0 \) gives us \( \cos(\phi) = 0 \). Thus, \( \phi = \frac{\pi}{2} + n\pi \) for any integer \( n \). A suitable choice is \( \phi = \frac{\pi}{2} \). We assume \( A=k \), so the equation becomes: \[ y(t) = k e^{-ct/2} \sin(\omega t) \].
3Step 3: Case (b): Initial Displacement is a
For case (b), where the initial displacement \( y=a \) at \( t=0 \), solve \( y(0) = A e^{0} \cos(\phi) = a \). This leads to \( A \cos(\phi) = a \). Assume \( A = k \) and so \( \cos(\phi) = \frac{a}{k} \). The equation is then given as \[ y(t) = k e^{-ct/2} \left( \cos(\omega t) \frac{a}{k} - \sin(\omega t) \sqrt{1 - \left(\frac{a}{k}\right)^2} \right) \].
Key Concepts
Displacement Equation in Damped Harmonic MotionUnderstanding Harmonic MotionRole of Damping ConstantSignificance of Initial Amplitude
Displacement Equation in Damped Harmonic Motion
In the context of damped harmonic motion, the displacement equation is a mathematical expression that describes how the position of a moving object changes over time. This type of motion combines oscillation with a gradual reduction in amplitude due to a damping effect. The general form of the displacement equation is written as:
\[ y(t) = A e^{-ct/2} \cos(\omega t + \phi) \]
Here, \( y(t) \) is the displacement at time \( t \), \( A \) is the initial amplitude, \( c \) is the damping constant, \( \omega \) is the angular frequency, and \( \phi \) is the phase angle.
\[ y(t) = A e^{-ct/2} \cos(\omega t + \phi) \]
Here, \( y(t) \) is the displacement at time \( t \), \( A \) is the initial amplitude, \( c \) is the damping constant, \( \omega \) is the angular frequency, and \( \phi \) is the phase angle.
- The term \( e^{-ct/2} \) represents the damping effect, leading to a decreasing amplitude over time.
- \( \cos(\omega t + \phi) \) captures the cyclical nature of the motion.
Understanding Harmonic Motion
Harmonic motion refers to a type of periodic oscillation where an object moves back and forth around a central position. It's commonly observed in systems where the force acting on the object is proportional to the displacement from its equilibrium position, such as springs or pendulums.
In the context of damped harmonic motion:
In the context of damped harmonic motion:
- The periodic motion gradually decreases over time due to external forces like friction or air resistance.
- This results in an oscillation that becomes less severe, eventually coming to rest.
Role of Damping Constant
The damping constant, denoted \( c \), is a critical parameter in the displacement equation. It quantifies the rate at which energy is lost in the system due to damping forces. This could be due to friction, air resistance, or another dissipating force.
- A larger \( c \) value implies a stronger damping effect, which means the oscillations die out more quickly.
- A smaller \( c \) results in slower energy loss, allowing the motion to persist longer.
Significance of Initial Amplitude
The initial amplitude, represented by \( A \), is the maximum extent of displacement from the rest position when time \( t = 0 \). It provides a baseline for how far the object initially moves during its oscillation.
In practice, solving specific scenarios requires integrating the initial amplitude with other variables like the damping constant to model the real-life motion accurately.
- If \( A = k \), then the motion begins with this amplitude, which subsequently decreases due to damping.
- The larger the initial amplitude, the more energy the system initially possesses.
In practice, solving specific scenarios requires integrating the initial amplitude with other variables like the damping constant to model the real-life motion accurately.
Other exercises in this chapter
Problem 1
The trigonometric function \(y=\tan x\) has period __________ and asymptotes \(x=\) __________ Sketch a graph of this function on the interval \((-\pi / 2, \pi
View solution Problem 1
The trigonometric functions \(y=\sin x\) and \(y=\cos x\) have amplitude _____ and period _____ Sketch a graph of each function on the interval \([0,2 \pi]\)
View solution Problem 2
The cancellation property \(\sin ^{-1}(\sin x)=x\) is valid for \(x\) in the interval ___________ Which of the following is not true? (a) \(\sin ^{-1}\left(\sin
View solution Problem 2
The trigonometric function \(y=3 \sin 2 x\) has amplitude _____ and period _____.
View solution