Second-Order Differential Equation Solver Calculator is a free online tool that displays classifications of given ordinary differential equation. CoolGyan’S online second-order differential equation solver calculator tool makes the calculation faster, and it displays the ODEs classification in a fraction of seconds. Show
How to Use the Second Order Differential Equation Solver Calculator?The procedure to use the second-order differential equation solver calculator is as follows: What is Meant by Second Order Differential Equation?In Calculus, a second-order differential equation is an ordinary differential equation whose derivative of the function is not greater than 2. It means that the highest derivative of the given function should be 2. In other words, if the equation has the highest of a second-order derivative is called the second-order differential equation. It is represented by d2y/dx2 = f”(x) = y” Here we learn how to solve equations of this type: d2ydx2 + pdydx + qy = 0 Differential EquationA Differential Equation is an equation with a function and one or more of its derivatives:
OrderThe Order is the highest derivative (is it a first derivative? a second derivative? etc): Example:dydx + y2 = 5x It has only the first derivative dy dx , so is "First Order" Example:d2ydx2 + xy = sin(x) This has a second derivative d2y dx2 , so is "Second Order" or "Order 2" Example:d3ydx3 + xdydx + y = ex This has a third derivative d3y dx3 which outranks the dy dx , so is "Third Order" or "Order 3" Before tackling second order differential equations, make sure you are familiar with the various methods for solving first order differential equations.Second Order Differential EquationsWe can solve a second order differential equation of the type: d2ydx2 + P(x)dydx + Q(x)y = f(x) where P(x), Q(x) and f(x) are functions of x, by using: Undetermined Coefficients which only works when f(x) is a polynomial, exponential, sine, cosine or a linear combination of those. Variation of Parameters which is a little messier but works on a wider range of functions. But here we begin by learning the case where f(x) = 0 (this makes it "homogeneous"): d2ydx2 + P(x)dydx + Q(x)y = 0 and also where the functions P(X) and Q(x) are constants p and q: d2ydx2 + pdydx + qy = 0 Let's learn to solve them! e to the rescueWe are going to use a special property of the derivative of the exponential function: At any point the slope (derivative) of ex equals the value of ex : And when we introduce a value "r" like this: f(x) = erx We find:
In other words, the first and second derivatives of f(x) are both multiples of f(x) This is going to help us a lot! Example 1: Solved2ydx2 + dydx − 6y = 0 Let y = erx so we get:
Substitute these into the equation above: r2erx + rerx − 6erx = 0 Simplify: erx(r2 + r − 6) = 0 r2 + r − 6 = 0 We have reduced the differential equation to an ordinary quadratic equation! This quadratic equation is given the special name of characteristic equation. We can factor this one to: (r − 2)(r + 3) = 0 So r = 2 or −3 And so we have two solutions: y = e2x y = e−3x But that’s not the final answer because we can combine different multiples of these two answers to get a more general solution: y = Ae2x + Be−3x CheckLet us check that answer. First take derivatives: y = Ae2x + Be−3x dydx = 2Ae2x − 3Be−3x d2ydx2 = 4Ae2x + 9Be−3x Now substitute into the original equation: d2ydx2 + dydx − 6y = 0 (4Ae2x + 9Be−3x) + (2Ae2x − 3Be−3x) − 6(Ae2x + Be−3x) = 0 4Ae2x + 9Be−3x + 2Ae2x − 3Be−3x − 6Ae2x − 6Be−3x = 0 4Ae2x + 2Ae2x − 6Ae2x+ 9Be−3x− 3Be−3x − 6Be−3x = 0 0 = 0 It worked! So, does this method work generally?Well, yes and no. The answer to this question depends on the constants p and q. With y = erx as a solution of the differential equation: d2ydx2 + pdydx + qy = 0 we get: r2erx + prerx + qerx = 0 erx(r2 + pr + q) = 0 r2 + pr + q = 0 This is a quadratic equation, and there can be three types of answer:
How we solve it depends which type! We can easily find which type by calculating the discriminant p2 − 4q. When it is
Two Real RootsWhen the discriminant p2 − 4q is positive we can go straight from the differential equation d2ydx2 + pdydx + qy = 0 through the "characteristic equation": r2 + pr + q = 0 to the general solution with two real roots r1 and r2: y = Aer1x + Ber2x Example 2: Solved2ydx2 − 9dydx + 20y = 0 The characteristic equation is: r2 − 9r+ 20 = 0 Factor: (r − 4)(r − 5) = 0 r = 4 or 5 So the general solution of our differential equation is: y = Ae4x + Be5x And here are some sample values:
Example 3: Solve6d2ydx2 + 5dydx − 6y = 0 The characteristic equation is: 6r2 + 5r− 6 = 0 Factor: (3r − 2)(2r + 3) = 0 r = 23 or −32 So the general solution of our differential equation is: y = Ae(23x) + Be(−32x) Example 4: Solve9d2ydx2 − 6dydx − y = 0 The characteristic equation is: 9r2 − 6r− 1 = 0 This does not factor easily, so we use the quadratic equation formula: x = −b ± √(b2 − 4ac) 2a with a = 9, b = −6 and c = −1 x = −(−6) ± √((−6)2 − 4×9×(−1)) 2×9 x = 6 ± √(36+ 36) 18 x = 6 ± 6√2 18 x = 1 ± √2 3 So the general solution of the differential equation is y = Ae(1 + √2 3)x + Be(1 − √2 3)x One Real RootWhen the discriminant p2 − 4q is zero we get one real root (i.e. both real roots are equal). Here are some examples: Example 5: Solved2ydx2 − 10dydx + 25y = 0 The characteristic equation is: r2 − 10r+ 25 = 0 Factor: (r − 5)(r − 5) = 0 r = 5 So we have one solution: y = e5x BUT when e5x is a solution, then xe5x is also a solution! Why? I can show you: y = xe5x dydx = e5x + 5xe5x d2ydx2 = 5e5x + 5e5x + 25xe5x So d2ydx2 − 10dydx + 25y = 5e5x + 5e5x + 25xe5x − 10(e5x + 5xe5x) + 25xe5x = (5e5x + 5e5x − 10e5x) + (25xe5x − 50xe5x + 25xe5x) = 0 So, in this case our solution is: y = Ae5x + Bxe5x How does this work in the general case?With y = xerx we get the derivatives:
So d2ydx2 + p dydx + qy = (rerx + rerx + r2xerx) + p( erx + rxerx ) + q( xerx ) = erx(r + r + r2x + p + prx + qx) = erx(2r + p + x(r2 + pr + q)) = erx(2r + p) because we already know that r2 + pr + q = 0 And when r2 + pr + q has a repeated root, then r = −p2 and 2r + p = 0 So if r is a repeated root of the characteristic equation, then the general solution is y = Aerx + Bxerx Let's try another example to see how quickly we can get a solution: Example 6: Solve4d2ydx2 + 4dydx + y = 0 The characteristic equation is: 4r2 + 4r+ 1 = 0 Then: (2r + 1)2 = 0 r = −12 So the solution of the differential equation is: y = Ae(−½)x + Bxe(−½)x Complex rootsWhen the discriminant p2 − 4q is negative we get complex roots. Let’s try an example to help us work out how to do this type: Example 7: Solved2ydx2 − 4dydx + 13y = 0 The characteristic equation is: r2 − 4r+ 13 = 0 This does not factor, so we use the quadratic equation formula: x = −b ± √(b2 − 4ac) 2a with a = 1, b = −4 and c = 13 x = −(−4) ± √((−4)2 − 4×1×13) 2×1 x = 4 ± √(16− 52) 2 x = 4 ± √(−36) 2 x = 4 ± 6i 2 x = 2 ± 3i If we follow the method used for two real roots, then we can try the solution: y = Ae(2+3i)x + Be(2−3i)x We can simplify this since e2x is a common factor: y = e2x( Ae3ix + Be−3ix ) But we haven't finished yet ... ! Euler's formula tells us that: eix = cos(x) + i sin(x) So now we can follow a whole new avenue to (eventually) make things simpler. Looking just at the "A plus B" part: Ae3ix + Be−3ix A(cos(3x) + i sin(3x)) + B(cos(−3x) + i sin(−3x)) Acos(3x) + Bcos(−3x) + i(Asin(3x) + Bsin(−3x)) Now apply the Trigonometric Identities: cos(−θ)=cos(θ) and sin(−θ)=−sin(θ): Acos(3x) + Bcos(3x) + i(Asin(3x) − Bsin(3x) (A+B)cos(3x) + i(A−B)sin(3x) Replace A+B by C, and A−B by D: Ccos(3x) + iDsin(3x) And we get the solution: y = e2x( Ccos(3x) + iDsin(3x) ) CheckWe have our answer, but maybe we should check that it does indeed satisfy the original equation: y = e2x( Ccos(3x) + iDsin(3x) ) dydx = e2x( −3Csin(3x)+3iDcos(3x) ) + 2e2x( Ccos(3x)+iDsin(3x) ) d2ydx2 = e2x( −(6C+9iD)sin(3x) + (−9C+6iD)cos(3x)) + 2e2x(2C+3iD)cos(3x) + (−3C+2iD)sin(3x) ) Substitute: d2ydx2
− 4dydx + 13y = e2x( −(6C+9iD)sin(3x) + (−9C+6iD)cos(3x)) + 2e2x(2C+3iD)cos(3x) + (−3C+2iD)sin(3x) ) − 4( e2x( −3Csin(3x)+3iDcos(3x) ) + 2e2x( Ccos(3x)+iDsin(3x) ) ) + 13( e2x(Ccos(3x) + iDsin(3x)) ) ... hey, why don't YOU try adding up all the terms to see if they equal zero ... if not please let me know, OK? How do we generalize this?Generally, when we solve the characteristic equation with complex roots, we will get two solutions r1 = v + wi and r2 = v − wi So the general solution of the differential equation is y = evx ( Ccos(wx) + iDsin(wx) ) Example 8: Solved2ydx2 − 6dydx + 25y = 0 The characteristic
equation is: r2 − 6r+ 25 = 0 Use the quadratic equation formula: x = −b ± √(b2 − 4ac) 2a with a = 1, b = −6 and c = 25 x = −(−6) ± √((−6)2 − 4×1×25) 2×1 x = 6 ± √(36− 100) 2 x = 6 ± √(−64) 2 x = 6 ± 8i 2 x = 3 ± 4i And we get the solution: y = e3x(Ccos(4x) + iDsin(4x)) Example 9: Solve9d2ydx2 + 12dydx + 29y = 0 The characteristic equation is: 9r2 + 12r+ 29 = 0 Use the quadratic equation formula: x = −b ± √(b2 − 4ac) 2a with a = 9, b = 12 and c = 29 x = −12 ± √(122 − 4×9×29) 2×9 x = −12 ± √(144− 1044) 18 x = −12 ± √(−900) 18 x = −12 ± 30i 18 x = −23 ± 53i And we get the solution: y = e(−23)x(Ccos(53x) + iDsin(53x)) SummaryTo solve a linear second order differential equation of the form d2ydx2 + pdydx + qy = 0 where p and q are constants, we must find the roots of the characteristic equation r2 + pr + q = 0 There are three cases, depending on the discriminant p2 - 4q. When it is positive we get two real roots, and the solution is y = Aer1x + Ber2x zero we get one real root, and the solution is y = Aerx + Bxerx negative we get two complex roots r1 = v + wi and r2 = v − wi, and the solution is y = evx ( Ccos(wx) + iDsin(wx) ) 9479, 9480, 9481, 9482, 9483, 9484, 9485, 9486, 9487, 9488 How do you solve a 2nd degree differential equation?Solving Second Order Differential Equation. If r1 and r2 are real and distinct roots, then the general solution is y = Aer1x + Ber2x.. If r1 = r2 = r, then the general solution is y = Aerx + Bxerx. If r1 = a + bi and r2 = a - bi are complex roots, then the general solution is y = eax(A sin bx + B cos bx). How Do You Solve second order differential equations with variable coefficients?The solution of the second-order linear differential equation with variable coefficients can be determined using the Laplace transform. In particular, when the equations have terms of the form tmy(n)(t), its Laplace transform is (– 1)m dm/ds[L{y(n)(t)}].
How Do You Solve second order differential equations with boundary conditions?A second-order boundary-value problem consists of a second-order differential equation along with constraints on the solution y = y(x) at two values of x . For example, y′′ + y = 0 with y(0) = 0 and y (π/6) = 4 is a fairly simple boundary value problem. So is y′′ + y = 0 with y′(0) = 0 and y′ (π/6) = 4 .
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