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Mathematical Methods for Physics and Engineering: A Comprehensive Guide

K. F. Riley, M. P. Hobson, S. J. Bence

Chapter 9

Normal modes - all with Video Answers

Educators


Chapter Questions

01:59

Problem 1

Three coupled pendulums swing perpendicularly to the horizontal line containing their points of suspension, and the following equations of motion are satisfied:
$$
\begin{aligned}
-m \ddot{x}_{1} &=c m x_{1}+d\left(x_{1}-x_{2}\right) \\
-M \ddot{x}_{2} &=c M x_{2}+d\left(x_{2}-x_{1}\right)+d\left(x_{2}-x_{3}\right) \\
-m \ddot{x}_{3} &=c m x_{3}+d\left(x_{3}-x_{2}\right)
\end{aligned}
$$
where $x_{1}, x_{2}$ and $x_{3}$ are measured from the equilibrium points, $m, M$ and $m$ are the masses of the pendulum bobs and $c$ and $d$ are positive constants. Find the normal frequencies of the system and sketch the corresponding patterns of oscillation. What happens as $d \rightarrow 0$ or $d \rightarrow \infty$ ?

Penny Riley
Penny Riley
Numerade Educator
01:59

Problem 2

A double pendulum, smoothly pivoted at $A$, consists of two light rigid rods, $A B$ and $B C$, each of length $l$, which are smoothly jointed at $B$ and carry masses $m$ and $\alpha m$ at $B$ and $C$ respectively. The pendulum makes small oscillations in one plane under gravity; at time $t, A B$ and $B C$ make angles $\theta(t)$ and $\phi(t)$ respectively with the downward vertical. Find quadratic expressions for the kinetic and potential energies of the system and hence show that the normal modes have angular frequencies given by
$$
\omega^{2}=\frac{g}{l}[1+\alpha \pm \sqrt{\alpha(1+\alpha)}]
$$
For $\alpha=1 / 3$, show that in one of the normal modes the mid-point of $B C$ does not move during the motion.

Penny Riley
Penny Riley
Numerade Educator
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Problem 3

Continue the worked example modelling a linear molecule discussed at the end of section 9.1, for the case in which $\mu=2$.
(a) Show that the eigenvectors derived there have the expected orthogonality properties with respect to both $\mathrm{A}$ and $\mathrm{B}$.
(b) For the situation in which the atoms are released from rest with initial displacements $x_{1}=2 \epsilon, x_{2}=-\epsilon$ and $x_{3}=0$, determine their subsequent motions and maximum displacements.

Nick Johnson
Nick Johnson
Numerade Educator
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Problem 4

Consider the circuit consisting of three equal capacitors and two different inductors shown in the figure. For charges $Q_{i}$ on the capacitors and currents $I_{i}$ through the components, write down Kirchhoff's law for the total voltage change around each of two complete circuit loops. Note that, to within an unimportant constant, the conservation of current implies that $Q_{3}=Q_{1}-Q_{2}$ and hence express the loop equations in the form given in (9.7), namely
$$
A \ddot{Q}+B Q=0
$$
Use this to show that the normal frequencies of the circuit are given by
$$
\omega^{2}=\frac{1}{C L_{1} L_{2}}\left[L_{1}+L_{2} \pm\left(L_{1}^{2}+L_{2}^{2}-L_{1} L_{2}\right)^{1 / 2}\right]
$$
Obtain the same matrices and result by finding the total energy stored in the various capacitors (typically $\left.Q^{2} /(2 C)\right)$ and in the inductors (typically $\left.L I^{2} / 2\right)$.
For the special case $L_{1}=L_{2}=L$ determine the relevant eigenvectors and so describe the patterns of current flow in the circuit.

Lainey Roebuck
Lainey Roebuck
Numerade Educator
14:22

Problem 5

It is shown in physics and engineering textbooks that circuits containing capacitors and inductors can be analysed by replacing a capacitor of capacitance $C$ by a 'complex impedance' $1 /(i \omega C)$ and an inductor of inductance $L$ by an impedance $i \omega L$, where $\omega$ is the angular frequency of the currents flowing and $i^{2}=-1$ Use this approach and Kirchhoff's circuit laws to analyse the circuit shown in the figure and obtain three linear equations governing the currents $I_{1}, I_{2}$ and $I_{3}$. Show that the only possible frequencies of self-sustaining currents satisfy either (a) $\omega^{2} L C=1$ or (b) $3 \omega^{2} L C=1 .$ Find the corresponding current patterns and, in each case, by identifying parts of the circuit in which no current flows, draw an equivalent circuit that contains only one capacitor and one inductor.

Shareef Jackson
Shareef Jackson
Numerade Educator
14:21

Problem 6

The simultaneous reduction to diagonal form of two real symmetric quadratic forms. Consider the two real symmetric quadratic forms $u^{T} A u$ and $u^{T} B u$, where $u^{T}$ stands for the row matrix $(x \quad y \quad z)$, and denote by $\mathrm{u}^{n}$ those column matrices that satisfy
$$
\mathrm{Bu}^{n}=\lambda_{n} \mathrm{Au}^{n}
$$
in which $n$ is a label and the $\lambda_{n}$ are real, non-zero and all different.
(a) By multiplying (E9.1) on the left by $\left(\mathrm{u}^{m}\right)^{\mathrm{T}}$ and the transpose of the corresponding equation for $\mathrm{u}^{m}$ on the right by $\mathrm{u}^{n}$, show that $\left(\mathrm{u}^{m}\right)^{\mathrm{T}} \mathrm{Au}^{n}=0$ for $n \neq m$
(b) By noting that $A u^{n}=\left(\lambda_{n}\right)^{-1} B u^{n}$, deduce that $\left(\mathrm{u}^{m}\right)^{\mathrm{T}} \mathrm{Bu}^{n}=0$ for $m \neq n$. It can be shown that the $u^{n}$ are linearly independent; the next step is to construct a matrix $\mathrm{P}$ whose columns are the vectors $\mathrm{u}^{n}$.
(c) Make a change of variables $u=P v$ such that $u^{\mathrm{T}}$ Au becomes $v^{\mathrm{T}} C v$, and $u^{\mathrm{T}} B u$ becomes $v^{\mathrm{T}} D v$. Show that $C$ and $D$ are diagonal by showing that $c_{i j}=0$ if $i \neq j$ and similarly for $d_{i j}$
Thus $\mathrm{u}=\mathrm{Pv}$ or $\mathrm{v}=\mathrm{P}^{-1} \mathrm{u}$ reduces both quadratics to diagonal form.
To summarise, the method is as follows:
(a) find the $\lambda_{n}$ that allow (E9.1) a non-zero solution, by solving $|\mathrm{B}-\lambda \mathrm{A}|=0$;
(b) for each $\lambda_{n}$ construct $\mathrm{u}^{n}$;
(c) construct the non-singular matrix $\mathrm{P}$ whose columns are the vectors $\mathrm{u}^{n}$;
(d) make the change of variable $\mathrm{u}=\mathrm{Pv}$.

Matthew Allcock
Matthew Allcock
Numerade Educator
02:08

Problem 7

(It is recommended that the reader does not attempt this question until exercise $9.6$ has been studied.)

If, in the pendulum system studied in section $9.1$, the string is replaced by a second rod identical to the first then the expressions for the kinetic energy $T$ and the potential energy $V$ become (to second order in the $\theta_{i}$ )
$$
\begin{aligned}
&T \approx M l^{2}\left(\frac{8}{3} \dot{\theta}_{1}^{2}+2 \dot{\theta}_{1} \dot{\theta}_{2}+\frac{2}{3} \dot{\theta}_{2}^{2}\right) \\
&V \approx M g l\left(\frac{3}{2} \theta_{1}^{2}+\frac{1}{2} \theta_{2}^{2}\right)
\end{aligned}
$$
Determine the normal frequencies of the system and find new variables $\xi$ and $\eta$ that will reduce these two expressions to diagonal form, i.e. to
$$
a_{1} \dot{\xi}^{2}+a_{2} \dot{\eta}^{2} \quad \text { and } \quad b_{1} \xi^{2}+b_{2} \eta^{2}
$$

Narayan Hari
Narayan Hari
Numerade Educator
06:13

Problem 8

(It is recommended that the reader does not attempt this question until exercise $9.6$ has been studied.)

Find a real linear transformation that simultaneously reduces the quadratic forms
$$
\begin{gathered}
3 x^{2}+5 y^{2}+5 z^{2}+2 y z+6 z x-2 x y \\
5 x^{2}+12 y^{2}+8 y z+4 z x
\end{gathered}
$$
to diagonal form.

Victor Salazar
Victor Salazar
Numerade Educator
02:29

Problem 9

Three particles of mass $m$ are attached to a light horizontal string having fixed ends, the string being thus divided into four equal portions of length $a$ each under a tension $T$. Show that for small transverse vibrations the amplitudes $\mathrm{x}^{i}$ of the normal modes satisfy $\mathrm{Bx}=\left(\operatorname{ma\omega}^{2} / T\right) \mathrm{x}$, where $\mathrm{B}$ is the matrix
$$
\left(\begin{array}{ccc}
2 & -1 & 0 \\
-1 & 2 & -1 \\
0 & -1 & 2
\end{array}\right)
$$
Estimate the lowest and highest eigenfrequencies using trial vectors $\left(\begin{array}{lll}3 & 4 & 3\end{array}\right)^{\mathrm{T}}$ and $\left.\begin{array}{lll}3 & -4 & 3\end{array}\right)^{\mathrm{T}}$. Use also the exact vectors $\left(\begin{array}{lll}1 & \sqrt{2} & 1\end{array}\right)^{\mathrm{T}}$ and $\left(\begin{array}{llll}1 & -\sqrt{2} & 1\end{array}\right)^{\mathrm{T}}$, and compare the results.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:25

Problem 10

Use the Rayleigh-Ritz method to estimate the lowest oscillation frequency of a heavy chain of $N$ links, each of length $a(=L / N)$, which hangs freely from one end. (Try simple calculable configurations such as all links but one vertical, or all links collinear, etc.)

Farnaz Mohseni
Farnaz Mohseni
Numerade Educator