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Regular singular points at x=1and atx=-3

Short Answer

Expert verified

Answer

(x+3)2(x-1)2y"+(x+3)(x-1)y'+y=0

Step by step solution

01

To Find a linear second-order differential equation

Consider a linear second-order differential equation in the standard form

">y"+P(x)y'+Q(x)y=0

If the factor x-1appears at most to the first power in the denominator of Pxand at most to the second power in the denominator of Qx, then x=1is a regular singular point. Similarly for x=-3So, let

Px=1x+3x-1andQx=1x+32x-12

02

Final Answer

We see that for the above parameters, x=1and x=-3are regular singular points for a linear second-order differential equation. Hence, the equation with the given properties in the standard form is

y"+1(X+3x-1y'+1x+32(x-1)2y=0

or equivalently

x+32+x-22y"+x+3x-1y'+y=0

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Most popular questions from this chapter

Consider a pendulum that is released from rest from an initial displacement of radians. Solving the linear model (7) subject to the initial condition θ0=θ0,θ'0=0gives θt=θ0cosglt . The period of oscillations predicted by this model is given by the familiar formula T=2πgI=2πIg.

The interesting thing about this formula for Tis that it does not depend on the magnitude of the initial displacement θ0. In other words, the linear model predicts that the time it would take the pendulum to swing from an initial displacement of, say,θ0=π2=90oto-π2and back again would be exactly the same as the time it would take to cycle from, say,θ0=π360=0.5oto-π360o. This is intuitively unreasonable; the actual period must depend on θ0.

If we assume that g=32ft/s2and l=32ft, then the period of oscillation of the linear model is T=2πs. Let us compare this last number with the period predicted by the non linear model when θ0=π4. Using a numerical solver that is capable of generating hard data, approximate the solution of,

d2θdt2+sinθ=0,θ0=π4,θ'0=0

On the interval 0t2. As in the problem 25, ift1 denotes the first time the pendulum reaches the position OP in Figure 5.3.3, then the period of the non linear pendulum is 4t1. Here is another way of solving the equationθt=0 . Experiment with small step sizes and advance the time, starting at t=0and ending att=2 . From your hard data observe the timet1 whenθt changes , for the first time , from positive to negative. Use the value t1to determine the true value of the period of the non linear pendulum. Compute the percentage relative error in the period estimated by T=2π.


In Problems 9 and 10 the eigenvalues and eigenfunctions of theboundary-value problemy''+λy=0,y'(0)=0,y'(π)=0areλn=n2,n=0,1,2,...,andy=cosnx, respectively. Fill in theblanks.

A solution of the BVP whenλ=36isy=____because _____.

In Problem 37 write the equation of motion in the form x(t)=Asin(ωt+ϕ)+Be2tsin(4t+θ). What is the amplitude of vibrations after a very long time?

Use a CAS to approximate the eigenvalues λ1,λ2,λ3, andλ4defined by the equation in part (a) of Problem 32 .

(a) Show that the current i(t) in an L R C-series circuit satisfies

Ld2idt2+Rdidt+1Ci=E'(t)

whereE'(t)denotes the derivative of E(t).

(b) Two initial conditions i(0) andi'(0)can be specified for the DE in part (a). Ifi(0)=i0and, q(0)=q0what isi'(0)?

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