Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Use a CAS to approximate the eigenvalues λ1,λ2,λ3, and λ4 of the boundary-value problem:

y''+λy=0,y(0)=0,y(1)-12y'(1)=0.Give the corresponding approximate eigenfunctions y1x,y2x, y3(x) , and y4x.

Short Answer

Expert verified

λ1=-3.667,y1(x)=sinh(1.915x)λ2=18.2738,y2(x)=sin(4.27487x)λ3=57.7075,y3(x)=sin(7.59655xx)λ4=116.9139,y4(x)=sin(10.8127x)

Step by step solution

01

To Find the solution of the differential equation

In the case when λ=-α2<0, the solution of the differential equation is y=c1coshαx+c2sinhαx. The condition y(0)=0 gives c1=0. The condition y(1)-12y'(1)=0applied to y=c2sinhαx gives c2sinhα-12αcoshα=0 or tanhα=12α. As can be seen from the figure, the graphs of y=tanhx and y=12xintersect at a single point with approximate x- coordinate α1=1.915. Thus, there is a single negative eigenvalue λ1=-α12-3.667and the corresponding eigenfunction is y1(x)=sinh1.915x. For λ=0 the only solution of the boundary-value problem is y=0.

For λ=α2>0 the solution of the differential equation is y=c1cosαx+c2sinαx. The condition y(0)=0 gives c1=0, so y=c2sinαx.The condition y(1)-12y'(1)=0 gives c2sinα-12cosα=0 , so the eigenvalues are λn=αn2 when an,n=2,3,4,.... are the positive roots of tanα=12α.

Using a CAS we find that the first three values of α are α2=4.27487,α3=7.59655 and α4=10.8127 The first three eigenvalues are then λ2=α22=18.2738,λ3=α23=57.7075 and λ4=α24=116.9139with corresponding eigenfunctions ,y2=sin4.27487x,y3=sin7.59655x, and y4=sin10.8127x.

02

Final proof

λ1=-3.667,y1x=sinh1.915xλ2=18.2738,y2x=sin4.27487xλ3=57.7075,y3x=sin7.59655xxλ4=116.9139,y4x=sin10.8127x

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Consider the boundary – value problem introduced in the construction of the mathematical model for the shape of a rotating string

Td2ydx2+ρω2y=0,y(0)=0,y(L)=0

For constant c2and , define the Critical speeds of angular rotation ωnas the values of ωfor which the boundary – value problem has nontrivial solutions. Find the critical speeds ωnand the corresponding deflectionsyn(x).

Relief supplies As shown in figurea plane flying horizontally at a constant speed drops V0 relief supply pack to a person on the ground. Assume the origin is the point where the supply pack is released and that the positive x-axis points forward and that positive y-axis points downward. under the assumption that the horizontal and vertical components of the air resistance are proportional to(dx/dt)2and=(dy/dt)2,respectively, and if the position of the supply pack is given by r(t)=x(i)+y(t)j, then its velocity is v(t)=(dx/dt)i+(dy/dt)j Equating components in the vector form of Newton’s second law of motion.

mdydt=mg-dxdt2i+dydt2jmd2xdt2=mg-kdxdt2,x0=0,x'0='v0md2ydt2=mg-kdydt2y0=0,y'0='0

a)solve both of the foregoing initial-value problems by means of the substitutionsu=dxdy,w=dydt and separation of variable.[Hint: see the Remarks at the end of

section .]

b)suppose the plane files at an altitude of 1000ftft and that its constant speed 300is mi/h. assume that the constant of proportionality for air resistance is k=0.0053 and that the supply pack weighs256 Ib. use a root-finding application of a CAC or a graphic calculator to determine the horizontal distance the pack travels, measured from its point of release to the point where it hits the ground.

A mass weighing24poundsstretches a spring4feet. The subsequent motion takes place in medium that offers a damping force numerically equal to localid="1664048610111" β(β>0)times the instantaneous velocity. If the mass is initially released from the equilibrium position with an upward velocity of 2fts, show that β>32 the equation of motion is

localid="1664048854781" style="max-width: none; vertical-align: -15px;" x(t)=3β218e2βt/3sinh23β218t
.

Spring Pendulum The rotational form of Newton’s secondlaw of motion is:The time rate of change of angular momentum about a point isequal to the moment of the resultant force (torque).In the absence of damping or other external forces, an analogueof (14) in Section 5.3 for the pendulum shown in Figure 5.3.3is then

(a) When m and l are constant show that (1) reduces to (6) ofSection 5.3.

(b) Now suppose the rod in Figure 5.3.3 is replaced with aspring of negligible mass. When a mass m is attached toits free end the spring hangs in the vertical equilibriumposition shown in Figure 5.R.4 and has length l0. When the spring pendulum is set in motion we assume that themotion takes place in a vertical plane and the spring is stiffenough not to bend. For t . 0 the length of the spring isthen lstd 5 l0 1 xstd, whereis the displacement from theequilibrium position. Find the differential equation for thedisplacement angledefined by (1).

In parts (a) and (b) of Problem 27 determine whether the mass passes through the equilibrium position. In each case ­and the time at which the mass attains its extreme displacement from the equilibrium position. What is the position of the mass at this instant?

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free