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In Problems 1 through 16, a homogeneous second-order linear differential equation, two functions \(y_{1}\) and \(y_{2}\), and a pair of initial conditions are given. First verify that \(y_{1}\) and \(y_{2}\) are solutions of the differential equation. Then find a particular solution of the form \(y=c_{1} y_{1}+c_{2} y_{2}\) that satisfies the given initial conditions. Primes denote derivatives with respect to \(x\). $$ \begin{aligned} &y^{\prime \prime}+25 y=0 ; y_{1}=\cos 5 x, y_{2}=\sin 5 x ; y(0)=10 \\ &y^{\prime}(0)=-10 \end{aligned} $$

Short Answer

Expert verified
The particular solution is \(y = 10\cos 5x - 2\sin 5x\).

Step by step solution

01

Verify y鈧 as a solution

Start by substituting \(y_{1} = \cos 5x\) into the differential equation \(y'' + 25y = 0\). Calculate the first and second derivatives: \[ y_{1}' = -5 \sin 5x \] \[ y_{1}'' = -25 \cos 5x \] Substitute into the equation: \[ -25\cos 5x + 25\cos 5x = 0 \] This confirms that \(y_{1}\) is a solution.
02

Verify y鈧 as a solution

Now substitute \(y_{2} = \sin 5x\) into the differential equation. Calculate the first and second derivatives: \[ y_{2}' = 5 \cos 5x \] \[ y_{2}'' = -25 \sin 5x \] Substitute into the equation: \[ -25\sin 5x + 25\sin 5x = 0 \] This confirms that \(y_{2}\) is also a solution.
03

Form the general solution

The general solution of the differential equation is a linear combination of the two solutions: \[ y = c_{1}\cos 5x + c_{2}\sin 5x \] We will use the initial conditions to find the constants \(c_{1}\) and \(c_{2}\).
04

Apply the initial condition y(0) = 10

Substitute \(x = 0\) into the general solution: \[ y(0) = c_{1}\cos 0 + c_{2}\sin 0 = c_{1} = 10 \] Thus, \(c_{1} = 10\).
05

Derive and apply the initial condition y'(0) = -10

Calculate the derivative of the general solution: \[ y' = -5c_{1}\sin 5x + 5c_{2}\cos 5x \] Substitute \(x = 0\) and the initial condition \(y'(0) = -10\): \[ y'(0) = -5c_{1}\sin 0 + 5c_{2}\cos 0 = 5c_{2} = -10 \] Therefore, \(c_{2} = -2\).
06

Formulate the particular solution

Plug the values of \(c_{1}\) and \(c_{2}\) into the general solution: \[ y = 10\cos 5x - 2\sin 5x \] This is the particular solution that satisfies the initial conditions.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Homogeneous Differential Equations
In the realm of differential equations, a homogeneous differential equation is one where every term is a multiple of the dependent variable or its derivatives. Essentially, if you have a second-order differential equation like \( y'' + 25y = 0 \), it is called homogeneous because both terms involve \( y \) or its derivatives (like \( y'' \)).

Homogeneous equations are characterized by the fact that the right-hand side is zero. This means that any non-zero function is a solution if substituted back into the equation, results in zero. Therefore, solving such equations usually involves finding two independent solutions that, when combined, can describe the complete set of solutions.

In our exercise, we dealt with the equation \( y'' + 25y = 0 \). We verified that \( \cos 5x \) and \( \sin 5x \) are valid solutions. This is done by checking whether they satisfy the equation after derivation; both lead back to an expression that equals zero, confirming their status as solutions.
Initial Value Problems
Initial value problems (IVPs) are problems that ask us to find a particular solution of a differential equation that meets specific starting conditions. These conditions are given at only one point, usually where a physical process starts or where initial measurements are taken.

In our exercise, we had initial conditions \( y(0) = 10 \) and \( y'(0) = -10 \). These conditions mean that our solution must satisfy these specific values of \( y \) and its first derivative at the point \( x = 0 \).

The process involves first solving the differential equation to get a general solution in terms of constants \( c_1 \) and \( c_2 \). By substituting the initial conditions into this general solution and its derivative, we can solve for the constants. These results give us the particular solution that fits the given initial conditions.
Linear Combinations of Solutions
When dealing with second-order linear homogeneous differential equations, a key approach is finding a general solution. This is often done by creating linear combinations of two independent solutions. A linear combination means you'll form the general solution by combining these solutions using constants, usually denoted by \( c_1 \) and \( c_2 \).

In our case, the general solution was \( y = c_1 \cos 5x + c_2 \sin 5x \). This combination works as the general solution because any linear combination of particular solutions of a homogeneous linear differential equation is also a solution.

To find a specific solution that satisfies given initial conditions, we calculate the coefficients \( c_1 \) and \( c_2 \) from those conditions, like \( y(0) = 10 \) and \( y'(0) = -10 \). Solving for these constants lets us write the particular solution. This solution ensures that the curve of our solution fits exactly through the specified conditions, representing a unique path dictated by the specific problem scenario.

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Most popular questions from this chapter

A front-loading washing machine is mounted on a thick rubber pad that acts like a spring; the weight \(W=m g\) (with \(g=9.8 \mathrm{~m} / \mathrm{s}^{2}\) ) of the machine depresses the pad exactly \(0.5 \mathrm{~cm}\). When its rotor spins at \(\omega\) radians per second, the rotor exerts a vertical force \(F_{0} \cos \omega t\) newtons on the machine. At what speed (in revolutions per minute) will resonance vibrations occur? Neglect friction.

Find a particular solution \(y_{p}\) of the given equation. In all these problems, primes denote derivatives with respect to \(x\). $$ y^{(3)}+y^{\prime}=2-\sin x $$

Each of Problems 15 through 18 gives the parameters for a forced mass-spring- dashpot system with equation \(m x^{\prime \prime}+c x^{\prime}+\) \(k x=F_{0} \cos \omega t .\) Investigate the possibility of practical resonance of this system. In particular, find the amplitude \(C(\omega)\) of steady periodic forced oscillations with frequency \(\omega .\) Sketch the graph of \(C(\omega)\) and find the practical resonance frequency \(\omega(\) if any). $$ m=1, c=4, k=5, F_{0}=10 $$

In each of Problems, a differential equation and one solution \(y_{1}\) are given. Use the method of reduction of order as in Problem 37 to find a second linearly independent solution \(y_{2}\) $$ x^{2} y^{\prime \prime}+x y^{\prime}-9 y=0(x>0) ; y_{1}(x)=x^{3} $$

In each of Problems 11 through 14, find and plot both the steady periodic solution \(x_{\mathrm{sp}}(t)=C \cos (\omega t-\alpha)\) of the given differential equation and the transient solution \(x_{\mathrm{tr}}(t)\) that satisfies the given initial conditions. $$ \begin{aligned} &x^{\prime \prime}+8 x^{\prime}+25 x=200 \cos t+520 \sin t ; x(0)=-30, \\ &x^{\prime}(0)=-10 \end{aligned} $$

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