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Consider a one dimensional, two-mass, three-spring system governed by the matrix \(A\), $$ A=\left(\begin{array}{cc} 4 & -2 \\ -2 & 7 \end{array}\right) $$ such that \(A x=\omega^{2} x\) (a) Determine the eigenfrequencies and normal coordinates. (b) Choose a set of initial conditions such that the system oscillates at its highest eigenfrequency. (c) Determine the solutions \(x_{1}(t)\) and \(x_{2}(t)\).

Short Answer

Expert verified
Eigenfrequencies are \(\sqrt{8}\) and \(\sqrt{3}\). Initial conditions for highest frequency: \(x(0) = \begin{pmatrix} 1 \\ 1 \end{pmatrix}\), solutions: \(x_1(t) = \cos(\sqrt{8}t)\), \(x_2(t) = \cos(\sqrt{8}t)\).

Step by step solution

01

Finding the Eigenvalues

To find the eigenfrequencies, we first determine the eigenvalues of the matrix \(A\). The characteristic equation for matrix \(A\) is given by \(\det(A - \lambda I) = 0\), where \(\lambda\) represents the eigenvalues. For matrix \(A = \begin{pmatrix} 4 & -2 \ -2 & 7 \end{pmatrix}\), calculate \(\det(A - \lambda I) = 0\).\[\det\left(\begin{pmatrix} 4 - \lambda & -2 \ -2 & 7 - \lambda \end{pmatrix}\right) = (4 - \lambda)(7 - \lambda) - (-2)(-2) = \lambda^2 - 11\lambda + 24 = 0.\]Solving \(\lambda^2 - 11 \lambda + 24 = 0\) gives us the eigenvalues \(\lambda_1 = 8\) and \(\lambda_2 = 3\). The eigenfrequencies are \(\omega_1 = \sqrt{\lambda_1} = \sqrt{8}\) and \(\omega_2 = \sqrt{\lambda_2} = \sqrt{3}\).
02

Finding the Eigenvectors (Normal Coordinates)

For each eigenvalue, compute the corresponding eigenvectors by solving \((A - \lambda I) x = 0\). - For \(\lambda_1 = 8\): \[\begin{pmatrix} 4 - 8 & -2 \ -2 & 7 - 8 \end{pmatrix} \begin{pmatrix} x_1 \ x_2 \end{pmatrix} = \begin{pmatrix} -4 & -2 \ -2 & -1 \end{pmatrix} \begin{pmatrix} x_1 \ x_2 \end{pmatrix} = \begin{pmatrix} 0 \ 0 \end{pmatrix}\]Simplifying, \(x_1 = x_2\). Choosing \(x_2 = 1\) gives us \(\begin{pmatrix} 1 \ 1 \end{pmatrix}\). - For \(\lambda_2 = 3\): \[\begin{pmatrix} 4 - 3 & -2 \ -2 & 7 - 3 \end{pmatrix} \begin{pmatrix} x_1 \ x_2 \end{pmatrix} = \begin{pmatrix} 1 & -2 \ -2 & 4 \end{pmatrix} \begin{pmatrix} x_1 \ x_2 \end{pmatrix} = \begin{pmatrix} 0 \ 0 \end{pmatrix}\]Simplifying, \(x_1 = 2x_2\). Choosing \(x_2 = 1\) gives us \(\begin{pmatrix} 2 \ 1 \end{pmatrix}\). These are the normal coordinates.
03

Choosing Initial Conditions for Highest Eigenfrequency

To achieve oscillation at the highest eigenfrequency, set the initial condition vector \(x(0)\) as the eigenvector corresponding to the highest eigenvalue, which is \(\lambda_1 = 8\). Therefore, the initial condition is \(x(0) = \begin{pmatrix} 1 \ 1 \end{pmatrix}\). This ensures the system will oscillate at frequency \(\omega_1 = \sqrt{8}\).
04

Solving for Solutions \(x_1(t)\) and \(x_2(t)\)

The solution for each coordinate in term of time \(t\) is derived from the normal mode corresponding to each eigenfrequency. For the initial condition \(x_0 = \begin{pmatrix} 1 \ 1 \end{pmatrix}\), corresponding to \(\omega_1 = \sqrt{8}\), the solutions are:\[x_1(t) = C_1 \cos(\sqrt{8} t + \phi) \quad \text{and} \quad x_2(t) = C_1 \cos(\sqrt{8} t + \phi),\]where \(C_1\) and \(\phi\) depend on the initial conditions. Given \(x(0) = \begin{pmatrix} 1 \ 1 \end{pmatrix}\), we find that \(C_1 = 1\) and \(\phi = 0\). Thus:\[x_1(t) = \cos(\sqrt{8} t), \quad x_2(t) = \cos(\sqrt{8} t).\]

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Key Concepts

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

Two-mass, three-spring system
In physics, a two-mass, three-spring system is a classic example used to understand oscillations and wave motion. This system comprises two masses interconnected by three springs and is studied to analyze the vibrational modes of coupled oscillators.
This kind of physical system is modeled using a matrix equation like \( A x = \omega^2 x \), where \( A \) involves spring constants and mass properties. We analyze such systems to understand how energy is transferred between masses due to springs.
This system can exhibit various types of motion like stretching and compressing internally.
  • There's displacement of both masses and study of how they interact.
  • It's pivotal to find the natural frequencies and modes to control or predict such interactions.
  • The study extends to applications like building construction and vehicle suspension systems.
Understanding these concepts helps create solutions to physical systems experiencing vibration and motion.
Eigenfrequencies
Eigenfrequencies are key natural properties of mechanical systems like our two-mass, three-spring system. They are the frequencies at which a system naturally vibrates when not subjected to external forces, directly linked to the system's eigenvalues.
In our exercise, the eigenfrequencies are determined after calculating the eigenvalues through the characteristic equation derived from the system's matrix \( A \). The formula to find them is \( \omega = \sqrt{\lambda} \), where \( \lambda \) is an eigenvalue. In our exercise, the eigenvalues \( \lambda_1 = 8 \) and \( \lambda_2 = 3 \) yield \( \omega_1 = \sqrt{8} \) and \( \omega_2 = \sqrt{3} \).
  • Understanding eigenfrequencies allows us to predict resonance and potential stability or instability in systems.
  • They are crucial in designing systems to withstand vibrations or exploits like musical instruments.
Grasping these ideas helps in engineering safe buildings and precise instruments.
Normal coordinates
Normal coordinates, also known as mode shapes, describe the pattern of motion for each eigenfrequency of a system. These coordinates simplify the description of system vibrations by separating them into independent modes.
Each normal coordinate corresponds to a specific way the entire system oscillates, moving together at the same frequency. To find these in our example, we solve for the eigenvectors of the system matrix \( A \) for each eigenvalue. In our analysis,
  • The normal coordinate for eigenvalue \( \lambda_1 = 8 \) is \( \begin{pmatrix} 1 & 1 \end{pmatrix} \).
  • For \( \lambda_2 = 3 \), it's \( \begin{pmatrix} 2 & 1 \end{pmatrix} \).
Using these normal coordinates, we can express any general motion of the system as a superposition of its normal modes. This provides a fundamental understanding of the vibrations and assists in designing coupled systems and structures effectively.
Initial conditions in physics
Initial conditions are foundational in determining the specific solution of a physical system's differential equations. They define the state of the system at the starting point, such as displacements or velocities. In our study, choosing initial conditions helps us target particular motion behaviors of the coupled system.
For our two-mass, three-spring system, selecting the initial condition vector correctly enables the system to oscillate at a desired frequency.
  • In our example, by choosing \( x(0) = \begin{pmatrix} 1 & 1 \end{pmatrix} \), we ensure oscillation occurs at the system's highest eigenfrequency.
  • This is vital because the condition directly affects the solution paths \( x_1(t) \) and \( x_2(t) \).
Initial conditions in physics are not just starting points but strategic choices to control or predict future states of complex dynamic systems.

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Most popular questions from this chapter

Four masses, all of mass \(m\), lie in the \(x-y\) plane at positions \((x, y)=(a, 0),(-a, 0),(0,+2 a),(0,-2 a)\). These are joined by massless rods to form a rigid body (a) Find the inertial tensor, using the \(x, y, z\) axes as a reference system. Exhibit the tensor as a matrix. (b) Consider a direction given by the unit vector \(\hat{n}\) that lies equally between the positive \(x, y, z\) axes; that is it makes equal angles with these three directions. Find the moment of inertia for rotation about this \(\hat{n}\) axis. (c) Given that at a certain time \(t\) the angular velocity vector lies along the above direction \(\hat{n}\), find, for that instant, the angle between the angular momentum vector and \(\hat{n}\).

Determine the principal moments of inertia of a sphere of radius \(R\) with a cavity of radius \(r\) located \(\epsilon\) from the center of the sphere.

Consider an object with the center of mass is at the origin and inertia tensor, $$ I=I\left(\begin{array}{ccc} 1 / 2 & -1 / 2 & 0 \\ -1 / 2 & 1 / 2 & 0 \\ 0 & 0 & 1 \end{array}\right) $$ (a) Determine the principal moments of inertia and the principal axes. Guess the object. (b) Determine the rotation matrix \(R\) and compute \(R^{\dagger} I R\). Do the diagonal elements match with your results from (a)? Note: columns of \(R\) are eigenvectors of \(I\). (c) Assume \(\omega=\frac{\omega}{\sqrt{2}}(\hat{x}+\hat{z})\). Determine \(L\) in the rotating coordinate system. Are \(L\) and \(\omega\) in the same direction? What does this mean? (d) Repeat (c) for \(\omega=\frac{\omega}{\sqrt{2}}(\hat{x}-\hat{y})\). What is different and why? (e) For which case will there be a non-zero torque required? (f) Determine the rotational kinetic energy for the case \(\omega=\frac{\omega}{\sqrt{2}}(\hat{x}-\hat{y}) ?\)

Calculate the moments of inertia \(I_{1}, I_{2}, I_{3}\) for a homogeneous cone of mass \(M\) whose height is \(h\) and whose base has a radius \(R\). Choose the \(x_{3}\) -axis along the symmetry axis of the cone. a) Choose the origin at the apex of the cone, and calculate the elements of the inertia tensor. b) Make a transformation such that the center of mass of the cone is the origin and find the principal moments of inertia.

Consider the two identical coupled oscillators given on the right in the figure assuming \(\kappa_{1}=\kappa_{2}=\kappa .\) Let both oscillators be linearly damped with a damping constant \(\beta .\) A force \(F=F_{0} \cos (\omega t)\) is applied to mass \(m_{1}\). Write down the pair of coupled differential equations that describe the motion. Obtain a solution by expressing the differential equations in terms of the normal coordinates. Show that the normal coordinates \(\eta_{1}\) and \(\eta_{2}\) exhibit resonance peaks at the characteristic frequencies \(\omega_{1}\) and \(\omega_{2}\) respectively.

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