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Use a CAS to plot graphs to convince yourself that the equation tanα=-α in Problem 38 has an infinite number of roots.

Explain why the negative roots of the equation can be ignored. Explain whyλ=0is not an eigenvalue even thoughα=0is an obvious solution of the equation tanα=-α.

Short Answer

Expert verified

yx=0

Step by step solution

01

To find the boundary conditions

We see from the graph that tanx=-x has infinitely many roots. Sinceλn=αn2, there are no new eigenvalues when αn<0. Forλ=0the differential equation y''=0 has general solutiony=c1x+c2.The boundary conditions imply c1=c2=0soyx=0

02

Final proof

yx=0

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Most popular questions from this chapter

Compare the result obtained in part (b) of Problem 43 with the solution obtained using variation of parameters when the external force is F0cosωt.

Rotating of a Shaft

Suppose the x-axis on the interval[0,L]is the geometric center of a long straight shaft, such as the propeller shaft of a ship. See Figure 5.2.12. When the shaft is rotating at a constant angular speed about this axis the deflectiony(x)of the shaft satisfies the differential equation

EId4ydx4-ρω2y=0

Where is its density per unit length. If the shaft is simplify supported, or hinged , at both ends the boundary conditions are then,

y(0)=0,yn(0)=0,y(L)=0,yn(L)=0

(a) If λ=α4=ρω2EI, then find the eigenvalues and eigenfunctions for this boundary – value problem.

(b) Use the eigenvalues λnin part (a) to find corresponding angular speeds ωn. The values ωnare called critical speeds. The value is ω1called the fundamental critical speed and analogous to example 4, at this speed the shaft changes shape from y=0to a deflection given by y1(x).

A force of 2 pounds stretches a spring 1foot. A mass weighing 3.2poundsis attached to the spring, and the system is then immersed in a medium that offers a damping force that is numerically equal to 0.4times the instantaneous velocity.

(a) Find the equation of motion if the mass is initially released from rest from a point 1 foot 1footabove the equilibrium position

(b) Express the equation of motion in the form given in (23).

(c) Find the fi­rst time at which the mass passes through the equilibrium position heading upward.

In Problems 35 and 36 determine whether it is possible to find values yand y1(Problem 35) and values ofL>0 (Problem 36 ) so that the given boundary-value problem has (a) precisely one nontrivial solution, (b) more than one solution, (c) no solution, (d) the trivial solution.

35. y''+16y=0,y(0)=y,y(π/2)=y1

Use a Maclaurin series to show that a power series solution of the initial-value problem

d2θdt2+glsinθ=0,   θ(0)=π6,   θ'(0)=0

is given by

θ(t)=π6g4lt2+3g296l2t4+

[Hint: See Example 3 in Section 4.10.]

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