So, what did we learn from this last example. Substituting \(y(x)\) into the differential equation, we have, \[\begin{align*}a_2(x)y+a_1(x)y+a_0(x)y &=a_2(x)(c_1y_1+c_2y_2+y_p)+a_1(x)(c_1y_1+c_2y_2+y_p) \\ &\;\;\;\; +a_0(x)(c_1y_1+c_2y_2+y_p) \\[4pt] &=[a_2(x)(c_1y_1+c_2y_2)+a_1(x)(c_1y_1+c_2y_2)+a_0(x)(c_1y_1+c_2y_2)] \\ &\;\;\;\; +a_2(x)y_p+a_1(x)y_p+a_0(x)y_p \\[4pt] &=0+r(x) \\[4pt] &=r(x). Write the general solution to a nonhomogeneous differential equation. Once, again we will generally want the complementary solution in hand first, but again were working with the same homogeneous differential equation (youll eventually see why we keep working with the same homogeneous problem) so well again just refer to the first example. You appear to be on a device with a "narrow" screen width (. Complementary function Calculator | Calculate Complementary function Complementary function / particular integral. Anshika Arya has created this Calculator and 2000+ more calculators! Welcome to the third instalment of my solving differential equations series. We will justify this later. Well eventually see why it is a good habit. This fact can be used to both find particular solutions to differential equations that have sums in them and to write down guess for functions that have sums in them. Checking Irreducibility to a Polynomial with Non-constant Degree over Integer. If we simplify this equation by imposing the additional condition \(uy_1+vy_2=0\), the first two terms are zero, and this reduces to \(uy_1+vy_2=r(x)\). . Stack Exchange network consists of 181 Q&A communities including Stack Overflow, the largest, most trusted online community for developers to learn, share their knowledge, and build their careers. The exponential function, \(y=e^x\), is its own derivative and its own integral. Find the simplest correct form of the particular integral yp. While technically we dont need the complementary solution to do undetermined coefficients, you can go through a lot of work only to figure out at the end that you needed to add in a \(t\) to the guess because it appeared in the complementary solution. Conic Sections Transformation. Consider the nonhomogeneous linear differential equation, \[a_2(x)y+a_1(x)y+a_0(x)y=r(x). Integration is a way to sum up parts to find the whole. Solutions Graphing Practice . If the function \(r(x)\) is a polynomial, our guess for the particular solution should be a polynomial of the same degree, and it must include all lower-order terms, regardless of whether they are present in \(r(x)\). Accessibility StatementFor more information contact us atinfo@libretexts.org. This will greatly simplify the work required to find the coefficients. Parametric Equations and Polar Coordinates, 9.5 Surface Area with Parametric Equations, 9.11 Arc Length and Surface Area Revisited, 10.7 Comparison Test/Limit Comparison Test, 12.8 Tangent, Normal and Binormal Vectors, 13.3 Interpretations of Partial Derivatives, 14.1 Tangent Planes and Linear Approximations, 14.2 Gradient Vector, Tangent Planes and Normal Lines, 15.3 Double Integrals over General Regions, 15.4 Double Integrals in Polar Coordinates, 15.6 Triple Integrals in Cylindrical Coordinates, 15.7 Triple Integrals in Spherical Coordinates, 16.5 Fundamental Theorem for Line Integrals, 3.8 Nonhomogeneous Differential Equations, 4.5 Solving IVP's with Laplace Transforms, 7.2 Linear Homogeneous Differential Equations, 8. \end{align*}\]. From our previous work we know that the guess for the particular solution should be. Complementary Function - an overview | ScienceDirect Topics Solve a nonhomogeneous differential equation by the method of undetermined coefficients. Then, \(y_p(x)=u(x)y_1(x)+v(x)y_2(x)\) is a particular solution to the differential equation. However, because the homogeneous differential equation for this example is the same as that for the first example we wont bother with that here. Particular integral of a fifth order linear ODE? This is best shown with an example so lets jump into one. Let \(y_p(x)\) be any particular solution to the nonhomogeneous linear differential equation, Also, let \(c_1y_1(x)+c_2y_2(x)\) denote the general solution to the complementary equation. This differential equation has a sine so lets try the following guess for the particular solution. 17.2: Nonhomogeneous Linear Equations - Mathematics LibreTexts The guess here is. \end{align*}\], \[\begin{align*}6A &=12 \\[4pt] 2A3B &=0. There is not much to the guess here. In order for the cosine to drop out, as it must in order for the guess to satisfy the differential equation, we need to set \(A = 0\), but if \(A = 0\), the sine will also drop out and that cant happen. One final note before we move onto the next part. The complementary function is found to be $Ae^{2x}+Be^{3x}$. The method of undetermined coefficients involves making educated guesses about the form of the particular solution based on the form of \(r(x)\). Solve the following initial value problem using complementary function and particular integral method( D2 + 1)y = e2* + cosh x + x, where y(0) = 1 and y'(o) = 2 a) Q2. Now, lets take our experience from the first example and apply that here. A first guess for the particular solution is. Use Cramers rule to solve the following system of equations. This one can be a little tricky if you arent paying attention. Our calculator allows you to check your solutions to calculus exercises. e^{x}D(e^{-3x}y) & = x + c \\ So, we would get a cosine from each guess and a sine from each guess. Checking this new guess, we see that none of the terms in \(y_p(t)\) solve the complementary equation, so this is a valid guess (step 3 again). Since \(r(x)=2e^{3x}\), the particular solution might have the form \(y_p(x)=Ae^{3x}.\) Then, we have \(yp(x)=3Ae^{3x}\) and \(y_p(x)=9Ae^{3x}\). First, since there is no cosine on the right hand side this means that the coefficient must be zero on that side. My text book then says to let $y=\lambda xe^{2x}$ without justification. So this means that we only need to look at the term with the highest degree polynomial in front of it. Lets look at some examples to see how this works. What does 'They're at four. Site design / logo 2023 Stack Exchange Inc; user contributions licensed under CC BY-SA. First, it will only work for a fairly small class of \(g(t)\)s. When the explicit functions y = f ( x) + cg ( x) form the solution of an ODE, g is called the complementary function; f is the particular integral. Recall that the complementary solution comes from solving. 2.4 Equations With More Than One Variable, 2.9 Equations Reducible to Quadratic in Form, 4.1 Lines, Circles and Piecewise Functions, 1.5 Trig Equations with Calculators, Part I, 1.6 Trig Equations with Calculators, Part II, 3.6 Derivatives of Exponential and Logarithm Functions, 3.7 Derivatives of Inverse Trig Functions, 4.10 L'Hospital's Rule and Indeterminate Forms, 5.3 Substitution Rule for Indefinite Integrals, 5.8 Substitution Rule for Definite Integrals, 6.3 Volumes of Solids of Revolution / Method of Rings, 6.4 Volumes of Solids of Revolution/Method of Cylinders, A.2 Proof of Various Derivative Properties, A.4 Proofs of Derivative Applications Facts, 7.9 Comparison Test for Improper Integrals, 9. We can still use the method of undetermined coefficients in this case, but we have to alter our guess by multiplying it by \(x\). When this happens we look at the term that contains the largest degree polynomial, write down the guess for that and dont bother writing down the guess for the other term as that guess will be completely contained in the first guess. \\[4pt] &=2 \cos _2 x+\sin_2x \\[4pt] &= \cos _2 x+1 \end{align*}\], \[y(x)=c_1 \cos x+c_2 \sin x+1+ \cos^2 x(\text{step 5}).\nonumber \], \(y(x)=c_1 \cos x+c_2 \sin x+ \cos x \ln| \cos x|+x \sin x\). We will get one set for the sine with just a \(t\) as its argument and well get another set for the sine and cosine with the 14\(t\) as their arguments. The guess for this is. Notice however that if we were to multiply the exponential in the second term through we would end up with two terms that are essentially the same and would need to be combined. The more complicated functions arise by taking products and sums of the basic kinds of functions. and we already have both the complementary and particular solution from the first example so we dont really need to do any extra work for this problem. dy dx = sin ( 5x) Go! complementary solution is y c = C 1 e t + C 2 e 3t. The solution of the homogeneous equation is : y ( x) = c 1 e 2 x + c 2 e 3 x So the particular solution should be y p ( x) = A x e 2 x Normally the guess should be A e 2 x. When solving ordinary differential equation, why use specific formula for particular integral. The following set of examples will show you how to do this. \end{align*} \nonumber \], So, \(4A=2\) and \(A=1/2\). Effect of a "bad grade" in grad school applications, What was the purpose of laying hands on the seven in Acts 6:6. As mentioned prior to the start of this example we need to make a guess as to the form of a particular solution to this differential equation. The guess for this is then, If we dont do this and treat the function as the sum of three terms we would get. The method is quite simple. However, we see that the constant term in this guess solves the complementary equation, so we must multiply by \(t\), which gives a new guess: \(y_p(t)=At^2+Bt\) (step 3). In fact, if both a sine and a cosine had shown up we will see that the same guess will also work. Embedded hyperlinks in a thesis or research paper, Counting and finding real solutions of an equation. This final part has all three parts to it. In this case, unlike the previous ones, a \(t\) wasnt sufficient to fix the problem. First, we will ignore the exponential and write down a guess for. This problem seems almost too simple to be given this late in the section. If you recall that a constant is nothing more than a zeroth degree polynomial the guess becomes clear. Everywhere we see a product of constants we will rename it and call it a single constant. Now, without worrying about the complementary solution for a couple more seconds lets go ahead and get to work on the particular solution. (D - 2)^2(D - 3)y = 0. We use an approach called the method of variation of parameters. EDIT A good exercice is to solve the following equation : \end{align*}\], \[y(x)=c_1e^x \cos 2x+c_2e^x \sin 2x+2x^2+x1.\nonumber \], \[\begin{align*}y3y &=12t \\[4pt] 2A3(2At+B) &=12t \\[4pt] 6At+(2A3B) &=12t. This last example illustrated the general rule that we will follow when products involve an exponential. We only need to worry about terms showing up in the complementary solution if the only difference between the complementary solution term and the particular guess term is the constant in front of them. Since \(r(x)=3x\), the particular solution might have the form \(y_p(x)=Ax+B\). Here is how the Complementary function calculation can be explained with given input values -> 4.813663 = 0.01*cos (6-0.785398163397301). (D - 2)(D - 3)y & = e^{2x} \\ We need to calculate $du$, we can do that by deriving the equation above, Substituting $u$ and $dx$ in the integral and simplify, Take the constant $\frac{1}{5}$ out of the integral, Apply the integral of the sine function: $\int\sin(x)dx=-\cos(x)$, Replace $u$ with the value that we assigned to it in the beginning: $5x$, Solve the integral $\int\sin\left(5x\right)dx$ and replace the result in the differential equation, As the integral that we are solving is an indefinite integral, when we finish integrating we must add the constant of integration $C$. We have \(y_p(x)=2Ax+B\) and \(y_p(x)=2A\), so we want to find values of \(A\), \(B\), and \(C\) such that, The complementary equation is \(y3y=0\), which has the general solution \(c_1e^{3t}+c_2\) (step 1). The Integral Calculator lets you calculate integrals and antiderivatives of functions online for free! What to do when particular integral is part of complementary function? All that we need to do it go back to the appropriate examples above and get the particular solution from that example and add them all together. Add the general solution to the complementary equation and the particular solution found in step 3 to obtain the general solution to the nonhomogeneous equation. Word order in a sentence with two clauses. \nonumber \], When \(r(x)\) is a combination of polynomials, exponential functions, sines, and cosines, use the method of undetermined coefficients to find the particular solution. \end{align*}\], Substituting into the differential equation, we obtain, \[\begin{align*}y_p+py_p+qy_p &=[(uy_1+vy_2)+uy_1+uy_1+vy_2+vy_2] \\ &\;\;\;\;+p[uy_1+uy_1+vy_2+vy_2]+q[uy_1+vy_2] \\[4pt] &=u[y_1+p_y1+qy_1]+v[y_2+py_2+qy_2] \\ &\;\;\;\; +(uy_1+vy_2)+p(uy_1+vy_2)+(uy_1+vy_2). This first one weve actually already told you how to do. It only takes a minute to sign up. Then, we want to find functions \(u(x)\) and \(v(x)\) such that. Therefore, we will only add a \(t\) onto the last term. \end{align*}\], \[y(x)=c_1e^{3x}+c_2e^{3x}+\dfrac{1}{3} \cos 3x.\nonumber \], \[\begin{align*}x_p(t) &=At^2e^{t}, \text{ so} \\[4pt] x_p(t) &=2Ate^{t}At^2e^{t} \end{align*}\], and \[x_p(t)=2Ae^{t}2Ate^{t}(2Ate^{t}At^2e^{t})=2Ae^{t}4Ate^{t}+At^2e^{t}. 0.00481366327239356 Meter -->4.81366327239356 Millimeter, Static Force using Maximum Displacement or Amplitude of Forced Vibration, Maximum Displacement of Forced Vibration using Natural Frequency, Maximum Displacement of Forced Vibration at Resonance, Maximum Displacement of Forced Vibration with Negligible Damping, Total displacement of forced vibration given particular integral and complementary function, The Complementary function formula is defined as a part of the solution for the differential equation of the under-damped forced vibrations and is represented as, The Complementary function formula is defined as a part of the solution for the differential equation of the under-damped forced vibrations is calculated using. Calculating the derivatives, we get \(y_1(t)=e^t\) and \(y_2(t)=e^t+te^t\) (step 1). Here is how the Complementary function calculation can be explained with given input values -> 4.813663 = 0.01*cos(6-0.785398163397301). Something seems wrong here. How to calculate Complementary function using this online calculator? \end{align*}\]. For \(y_p\) to be a solution to the differential equation, we must find a value for \(A\) such that, \[\begin{align*} yy2y &=2e^{3x} \\[4pt] 9Ae^{3x}3Ae^{3x}2Ae^{3x} &=2e^{3x} \\[4pt] 4Ae^{3x} &=2e^{3x}. The guess for the \(t\) would be, while the guess for the exponential would be, Now, since weve got a product of two functions it seems like taking a product of the guesses for the individual pieces might work. Solve a nonhomogeneous differential equation by the method of variation of parameters. Find the general solution to \(yy2y=2e^{3x}\). If a portion of your guess does show up in the complementary solution then well need to modify that portion of the guess by adding in a \(t\) to the portion of the guess that is causing the problems. Also, in what cases can we simply add an x for the solution to work? The complementary equation is \(x''+2x+x=0,\) which has the general solution \(c_1e^{t}+c_2te^{t}\) (step 1). We promise that eventually youll see why we keep using the same homogeneous problem and why we say its a good idea to have the complementary solution in hand first. Example 17.2.5: Using the Method of Variation of Parameters. Notice in the last example that we kept saying a particular solution, not the particular solution. Then, \(y_p(x)=u(x)y_1(x)+v(x)y_2(x)\) is a particular solution to the equation. By clicking Accept all cookies, you agree Stack Exchange can store cookies on your device and disclose information in accordance with our Cookie Policy. Are there any canonical examples of the Prime Directive being broken that aren't shown on screen? This will simplify your work later on. Differential Equations - Variation of Parameters - Lamar University These types of systems are generally very difficult to solve. Since \(g(t)\) is an exponential and we know that exponentials never just appear or disappear in the differentiation process it seems that a likely form of the particular solution would be. Do not solve for the values of the coefficients. We will see that solving the complementary equation is an important step in solving a nonhomogeneous differential equation. I hope they would help you understand the matter better. Complementary function / particular integral - Mathematics Stack Exchange Also, because the point of this example is to illustrate why it is generally a good idea to have the complementary solution in hand first well lets go ahead and recall the complementary solution first. Notice that even though \(g(t)\) doesnt have a \({t^2}\) in it our guess will still need one! What was the actual cockpit layout and crew of the Mi-24A? We do need to be a little careful and make sure that we add the \(t\) in the correct place however. This will arise because we have two different arguments in them. Plugging this into our differential equation gives. Forced vibration is when an alternating force or motion is applied to a mechanical system, for example when a washing machine shakes due to an imbalance. particular solution - Symbolab Did the Golden Gate Bridge 'flatten' under the weight of 300,000 people in 1987? \(g\left( t \right) = 4\cos \left( {6t} \right) - 9\sin \left( {6t} \right)\), \(g\left( t \right) = - 2\sin t + \sin \left( {14t} \right) - 5\cos \left( {14t} \right)\), \(g\left( t \right) = {{\bf{e}}^{7t}} + 6\), \(g\left( t \right) = 6{t^2} - 7\sin \left( {3t} \right) + 9\), \(g\left( t \right) = 10{{\bf{e}}^t} - 5t{{\bf{e}}^{ - 8t}} + 2{{\bf{e}}^{ - 8t}}\), \(g\left( t \right) = {t^2}\cos t - 5t\sin t\), \(g\left( t \right) = 5{{\bf{e}}^{ - 3t}} + {{\bf{e}}^{ - 3t}}\cos \left( {6t} \right) - \sin \left( {6t} \right)\), \(y'' + 3y' - 28y = 7t + {{\bf{e}}^{ - 7t}} - 1\), \(y'' - 100y = 9{t^2}{{\bf{e}}^{10t}} + \cos t - t\sin t\), \(4y'' + y = {{\bf{e}}^{ - 2t}}\sin \left( {\frac{t}{2}} \right) + 6t\cos \left( {\frac{t}{2}} \right)\), \(4y'' + 16y' + 17y = {{\bf{e}}^{ - 2t}}\sin \left( {\frac{t}{2}} \right) + 6t\cos \left( {\frac{t}{2}} \right)\), \(y'' + 8y' + 16y = {{\bf{e}}^{ - 4t}} + \left( {{t^2} + 5} \right){{\bf{e}}^{ - 4t}}\). One of the more common mistakes in these problems is to find the complementary solution and then, because were probably in the habit of doing it, apply the initial conditions to the complementary solution to find the constants. Expert Answer. Now, all that we need to do is do a couple of derivatives, plug this into the differential equation and see if we can determine what \(A\) needs to be. Complementary function / particular integral. Find the general solution to the following differential equations. This gives. However, we should do at least one full blown IVP to make sure that we can say that weve done one. If so, multiply the guess by \(x.\) Repeat this step until there are no terms in \(y_p(x)\) that solve the complementary equation. We now examine two techniques for this: the method of undetermined coefficients and the method of variation of parameters. None of the terms in \(y_p(x)\) solve the complementary equation, so this is a valid guess (step 3). First multiply the polynomial through as follows. Also, because we arent going to give an actual differential equation we cant deal with finding the complementary solution first. A particular solution to the differential equation is then. A particular solution to the differential equation is then. But since e 2 x is already solution of the homogeneous equation, you need to multiply by x the guess. The general solution is, \[y(t)=c_1e^t+c_2te^te^t \ln |t| \tag{step 5} \], \[\begin{align*} u \cos x+v \sin x &=0 \\[4pt] u \sin x+v \cos x &=3 \sin _2 x \end{align*}. Solving this system gives \(c_{1} = 2\) and \(c_{2} = 1\). yc(t) = c1y1(t) + c2y2(t) Remember as well that this is the general solution to the homogeneous differential equation. What is scrcpy OTG mode and how does it work. Trying solutions of the form y = A e t leads to the auxiliary equation 5 2 + 6 + 5 = 0. I am considering the equation $\frac{d^2y}{dx^2}-5\frac{dy}{dx}+6y=e^{2x}$. This gives us the following general solution, \[y(x)=c_1e^{2x}+c_2e^{3x}+3xe^{2x}. Complementary function and particular integral - YouTube In this case the problem was the cosine that cropped up. Complementary function and particular integral | Physics Forums The first two terms however arent a problem and dont appear in the complementary solution. There is nothing to do with this problem. The characteristic equation for this differential equation and its roots are. Lets take a look at some more products. If you can remember these two rules you cant go wrong with products. At this point do not worry about why it is a good habit. Practice and Assignment problems are not yet written. Now, lets proceed with finding a particular solution. \nonumber \], In this case, we use the two linearly independent solutions to the complementary equation to form our particular solution. Substitute \(y_p(x)\) into the differential equation and equate like terms to find values for the unknown coefficients in \(y_p(x)\). Notice that if we multiplied the exponential term through the parenthesis the last two terms would be the complementary solution. The Complementary function formula is defined as a part of the solution for the differential equation of the under-damped forced vibrations and is represented as x1 = A*cos(d-) or Complementary function = Amplitude of vibration*cos(Circular damped frequency-Phase Constant). Differential Equations - Undetermined Coefficients - Lamar University This is not technically part the method of Undetermined Coefficients however, as well eventually see, having this in hand before we make our guess for the particular solution can save us a lot of work and/or headache. Line Equations Functions Arithmetic & Comp. How do I stop the Flickering on Mode 13h? We never gave any reason for this other that trust us. We can use particular integrals and complementary functions to help solve ODEs if we notice that: 1. General solution is complimentary function and particular integral. 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MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "zz:_Back_Matter" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()" }, [ "article:topic", "Cramer\u2019s rule", "method of undetermined coefficients", "complementary equation", "particular solution", "method of variation of parameters", "authorname:openstax", "license:ccbyncsa", "showtoc:no", "program:openstax", "licenseversion:40", "source@https://openstax.org/details/books/calculus-volume-1", "author@Gilbert Strang", "author@Edwin \u201cJed\u201d Herman" ], https://math.libretexts.org/@app/auth/3/login?returnto=https%3A%2F%2Fmath.libretexts.org%2FBookshelves%2FCalculus%2FCalculus_(OpenStax)%2F17%253A_Second-Order_Differential_Equations%2F17.02%253A_Nonhomogeneous_Linear_Equations, \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}}}\) \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{#1}}} \)\(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\) \(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\)\(\newcommand{\AA}{\unicode[.8,0]{x212B}}\), GENERAL Solution TO A NONHOMOGENEOUS EQUATION, Example \(\PageIndex{1}\): Verifying the General Solution, Example \(\PageIndex{2}\): Undetermined Coefficients When \(r(x)\) Is a Polynomial, Example \(\PageIndex{3}\): Undetermined Coefficients When \(r(x)\) Is an Exponential, PROBLEM-SOLVING STRATEGY: METHOD OF UNDETERMINED COEFFICIENTS, Example \(\PageIndex{3}\): Solving Nonhomogeneous Equations, Example \(\PageIndex{4}\): Using Cramers Rule, PROBLEM-SOLVING STRATEGY: METHOD OF VARIATION OF PARAMETERS, Example \(\PageIndex{5}\): Using the Method of Variation of Parameters, General Solution to a Nonhomogeneous Linear Equation, source@https://openstax.org/details/books/calculus-volume-1, \((a_2x^2+a_1x+a0) \cos x \\ +(b_2x^2+b_1x+b_0) \sin x\), \((A_2x^2+A_1x+A_0) \cos x \\ +(B_2x^2+B_1x+B_0) \sin x \), \((a_2x^2+a_1x+a_0)e^{x} \cos x \\ +(b_2x^2+b_1x+b_0)e^{x} \sin x \), \((A_2x^2+A_1x+A_0)e^{x} \cos x \\ +(B_2x^2+B_1x+B_0)e^{x} \sin x \).

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