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Mathematical Methods for Physics and Engineering - Matematica.NET

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NORMAL MODESunder gravity. At time t, AB <strong>and</strong> BC make angles θ(t) <strong>and</strong>φ(t), respectively, withthe downward vertical. Find quadratic expressions <strong>for</strong> the kinetic <strong>and</strong> potentialenergies of the system <strong>and</strong> hence show that the normal modes have angularfrequencies given byω 2 = g [1+α ± √ ]α(1 + α) .lFor α =1/3, show that in one of the normal modes the mid-point of BC doesnot move during the motion.9.3 Continue the worked example, modelling a linear molecule, discussed at the endofsection9.1,<strong>for</strong>thecaseinwhichµ =2.(a) Show that the eigenvectors derived there have the expected orthogonalityproperties with respect to both A <strong>and</strong> B.(b) For the situation in which the atoms are released from rest with initialdisplacements x 1 =2ɛ, x 2 = −ɛ <strong>and</strong> x 3 = 0, determine their subsequentmotions <strong>and</strong> maximum displacements.9.4 Consider the circuit consisting of three equal capacitors <strong>and</strong> two different inductorsshown in the figure. For charges Q i on the capacitors <strong>and</strong> currents I iQ 1 Q 2CCQ 3L 1 C L 2I 1 I 2through the components, write down Kirchhoff’s law <strong>for</strong> the total voltage changearound each of two complete circuit loops. Note that, to within an unimportantconstant, the conservation of current implies that Q 3 = Q 1 − Q 2 . Express the loopequations in the <strong>for</strong>m given in (9.7), namelyA¨Q + BQ = 0.Use this to show that the normal frequencies of the circuit are given byω 2 =1CL 1 L 2[L1 + L 2 ± (L 2 1 + L 2 2 − L 1 L 2 ) 1/2] .Obtain the same matrices <strong>and</strong> result by finding the total energy stored in thevarious capacitors (typically Q 2 /(2C)) <strong>and</strong> in the inductors (typically LI 2 /2).For the special case L 1 = L 2 = L determine the relevant eigenvectors <strong>and</strong> sodescribe the patterns of current flow in the circuit.9.5 It is shown in physics <strong>and</strong> engineering textbooks that circuits containing capacitors<strong>and</strong> inductors can be analysed by replacing a capacitor of capacitance C by a‘complex impedance’ 1/(iωC) <strong>and</strong> an inductor of inductance L by an impedanceiωL, whereω is the angular frequency of the currents flowing <strong>and</strong> i 2 = −1.Use this approach <strong>and</strong> Kirchhoff’s circuit laws to analyse the circuit shown in330

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