Find a general solution to the givenhomogeneous equation.(D+1)2(D6)3(D+5)(D2+1)(D2+4)2[y]=0

Short Answer

Expert verified

The general solution to the homogeneous equation is:

y=C1ex+C2xex+C3e6x+C4xe6x+C5x2e6x+C6e5x+C7cosx+C8sinx+C9cos2x+C10sin2x

Step by step solution

01

Homogenous Equation

A homogeneous system of linear equations is one in which all of the constant terms are zero. A homogeneous system always has at least one solution, namely the zero vector. When a row operation is applied to a homogeneous system, the new system is still homogeneous.

02

Solving of Homogenous Equation:

The given differential equation is (D1)2(D6)(D+5)(D2+1)(D2+4)[y]=0. To solve this equation we look at its auxillary equation which is .(m+1)2(m6)3(m+5)(m2+1)(m2+4)=0

03

 Step 3: Solving for general equation:

The complete set of solution of auxillary equation is {1,1,6,66,5,i,i,2i,2i}

To conclude that the general solution of the given differential equation is y=C1ex+C2xex+C3e6x+C4xe6x+C5x2e6x+C6e5x+C7cosx+C8sinx+C9cos2x+C10sin2xy=C1ex+C2xex+C3e6x+C4xe6x+C5x2e6x+C6e5x+C7cosx+C8sinx+C9cos2x+C10sin2x, where Ci(1i10) are arbitrary constants.

The general solution of the given differential equation isy=C1ex+C2xex+C3e6x+C4xe6x+C5x2e6x+C6e5x+C7cosx+C8sinx+C9cos2x+C10sin2x, where Ci(1i7) are arbitrary constant.

Hence, the final answer is:

y=C1ex+C2xex+C3e6x+C4xe6x+C5x2e6x+C6e5x+C7cosx+C8sinx+C9cos2x+C10sin2x

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Most popular questions from this chapter

Higher-Order Cauchy–Euler Equations. A differential equation that can be expressed in the form

anxny(n)(x)+an1xn1y(n1)(x)+...+a0y(x)=0

wherean,an1,....,a0 are constants, is called a homogeneous Cauchy–Euler equation. (The second-order case is discussed in Section 4.7.) Use the substitution y=xyto help determine a fundamental solution set for the following Cauchy–Euler equations:

(a) x3y'''+x2y''2xy'+2y=0,x>0

(b) x4y(4)+6x3y'''+2x2y''4xy+4y=0,x>0

(c) x3y'''2x2y''+13xy'13y=0,x>0

[Hint: xα+βi=e(α+βi)lnx=xa{cos(βlnx)+isin(βlnx)}]

On a smooth horizontal surface, a mass of m1 kg isattached to a fixed wall by a spring with spring constantk1 N/m. Another mass of m2 kg is attached to thefirst object by a spring with spring constant k2 N/m. Theobjects are aligned horizontally so that the springs aretheir natural lengths. As we showed in Section 5.6, thiscoupled mass–spring system is governed by the systemof differential equations

m1d2xdt2+(k1+k2)xk2y=0

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Let’s assume that m1 = m2 = 1, k1 = 3, and k2 = 2.If both objects are displaced 1 m to the right of theirequilibrium positions (compare Figure 5.26, page 283)and then released, determine the equations of motion forthe objects as follows:

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(b) Find a general solution x(2) to (36).

(c) Substitute x(2) back into (34) to obtain a generalsolution for y(2)

(d) Use the initial conditions to determine the solutions,x(2) and y(2), which are the equations of motion.

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y'''-3y''+3y'-y=ex

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