Mathematical Methods - Lecture 9
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1 Mathematical Methods - Lecture 9 Yuliya Tarabalka Inria Sophia-Antipolis Méditerranée, Titane team, Tel.: +33 (0) yuliya.tarabalka@inria.fr Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 1 / 33
2 Outline 1 Partial Differentiation 2 Partial Differential Equations Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 2 / 33
3 Partial Differentiation Functions of several variables f (x) is a function of one variable x We may consider functions that depend on more than one variable Example: f (x, y) = x 2 + 3xy depends on 2 variables x and y For any pair of values x, y, f (x, y) has a well-defined value Function f (x 1, x 2,..., x n ) depends on the variables x 1, x 2,..., x n Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 3 / 33
4 Partial derivatives Partial Differentiation A function f (x, y) will have a gradient in ALL directions in the xy-plane Gradient = rate of change of a function Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 4 / 33
5 Partial derivatives Partial Differentiation A function f (x, y) will have a gradient in ALL directions in the xy-plane Gradient = rate of change of a function The rates of change of f (x, y) in the positive x- and y- directions are called partial derivatives wrt x and y, respectively Partial derivatives are extremely important in a wide range of applications! Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 4 / 33
6 Partial Differentiation Partial derivatives Partial derivative of f (x, y) with respect to x is denoted by f / x: to signify that a derivative is wrt x, but to recognize that a derivative wrt y also exists f x = lim x 0 provided that the limit exists f (x + x, y) f (x, y), x Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 5 / 33
7 Partial Differentiation Partial derivatives Partial derivative of f (x, y) with respect to x is denoted by f / x: to signify that a derivative is wrt x, but to recognize that a derivative wrt y also exists f x = lim x 0 provided that the limit exists f (x + x, y) f (x, y), x The partial derivative of f with respect to y: f y = lim y 0 provided that the limit exists f (x, y + y) f (x, y), y Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 5 / 33
8 Partial Differentiation Partial derivatives - Notations Partial derivative of f (x, y) with respect to x: f x = ( f x ) = f x y Partial derivative of f with respect to y: f y = ( f y ) = f y x It is important when using partial derivatives to remember which variables are being held constant! Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 6 / 33
9 Partial derivatives Partial Differentiation The extension to the general n-variable case is straightforward: f (x 1,..., x n ) x i provided that the limit exists f (x 1,..., x i + x i,..., x n ) f (x 1,..., x i,..., x n ) = lim, x i 0 x i Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 7 / 33
10 Partial derivatives Partial Differentiation Second (and higher) partial derivatives may be defined in a similar way: x ( f x ) = 2 f x 2 = f xx x ( f y ) = 2 f x y = f xy y ( f y ) = 2 f y 2 = f yy Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 8 / 33
11 Partial Differentiation Properties of partial derivatives Provided that the second partial derivatives are continuous at the point in question: 2 f x y = 2 f y x 2 f x i x j = 2 f x j x i Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 9 / 33
12 Partial Differentiation Partial derivatives - Example Exercise: Find the first and second partial derivatives of the function f (x, y) = 2x 3 y 2 + y 3 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 10 / 33
13 Partial Differentiation Partial derivatives - Example Exercise: Find the first and second partial derivatives of the function f (x, y) = 2x 3 y 2 + y 3 The first partial derivatives: f x = 6x 2 y 2, f y = 4x 3 y + 3y 2 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 10 / 33
14 Partial Differentiation Partial derivatives - Example Exercise: Find the first and second partial derivatives of the function f (x, y) = 2x 3 y 2 + y 3 The first partial derivatives: f x = 6x 2 y 2, f y = 4x 3 y + 3y 2 The second partial derivatives: 2 f x 2 = 12xy 2, 2 f y 2 = 4x 3 + 6y, Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 10 / 33
15 Partial Differentiation Partial derivatives - Example Exercise: Find the first and second partial derivatives of the function f (x, y) = 2x 3 y 2 + y 3 The first partial derivatives: f x = 6x 2 y 2, f y = 4x 3 y + 3y 2 The second partial derivatives: 2 f x 2 = 12xy 2, 2 f y 2 = 4x 3 + 6y, 2 f x y = 2 f y x = 12x 2 y Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 10 / 33
16 The chain rule Partial Differentiation The total derivative of f (x, y) with respect to x: df dx = f dx x dx + f dy y dx The total differential of the function f (x, y): The chain rule: df = f f dx + x y dy df du = f dx x du + f dy y du Particularly useful when an equation is expressed in a parametric form Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 11 / 33
17 The chain rule Partial Differentiation Exercise: Given that x(u) = 1 + au and y(u) = bu 3, find the rate of change of f (x, y) = xe y with respect to u Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 12 / 33
18 The chain rule Partial Differentiation Exercise: Given that x(u) = 1 + au and y(u) = bu 3, find the rate of change of f (x, y) = xe y with respect to u Using the chain rule: Substituting for x and y: df du = (e y )a + ( xe y )3bu 2 df du = e bu3 (a 3bu 2 3bau 3 ) Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 12 / 33
19 What is a partial differential equation? Partial differential equation (PDE) is a differential equation that contains unknown multivariable functions and their partial derivatives PDEs are used to describe a wide variety of phenomena: sound, heat, electrodynamics, quantum mechanics... Examples: 1 transport: u x + u y = 0 2 shock wave: u x + uu y = 0 3 vibrating bar: u tt + u xxxx = 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 13 / 33
20 Partial differential equation The most general second-order PDE in two independent variables is: F (x, y, u, u x, u y, u xx, u xy, u yy ) = 0 A solution of a PDE is a function y(x, y,...) that satisfies the equation identically, at least in some region of the x, y,... variables Most of the important PDEs of physics are second-order and linear For linear homogeneous PDEs, the superposition principle applies Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 14 / 33
21 Partial differential equation - Example Exercise: Find all u(x, y) satisfying the equation u xx = 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 15 / 33
22 Partial differential equation - Example Exercise: Find all u(x, y) satisfying the equation u xx = 0 We could integrate once to get u x = constant? Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 15 / 33
23 Partial differential equation - Example Exercise: Find all u(x, y) satisfying the equation u xx = 0 We could integrate once to get u x = constant? Since there is another variable y, that s not really right. We get: u x (x, y) = f (y), where f (y) is arbitrary Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 15 / 33
24 Partial differential equation - Example Exercise: Find all u(x, y) satisfying the equation u xx = 0 We could integrate once to get u x = constant? Since there is another variable y, that s not really right. We get: where f (y) is arbitrary u x (x, y) = f (y), We integrate again to get u(x, y) = f (y)x + g(y). This is the general solution. Note that there are two arbitrary functions in the solution Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 15 / 33
25 Partial differential equation - Example 2 Exercise: Solve the PDE u xx + u = 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 16 / 33
26 Partial differential equation - Example 2 Exercise: Solve the PDE u xx + u = 0 Again, it s an ODE with an extra variable y Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 16 / 33
27 Partial differential equation - Example 2 Exercise: Solve the PDE u xx + u = 0 Again, it s an ODE with an extra variable y The solution is u = f (y) cos x + g(y) sin x, where f (y) and g(y) are two arbitrary functions of y Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 16 / 33
28 Partial differential equation - Example 2 Exercise: Solve the PDE u xx + u = 0 Again, it s an ODE with an extra variable y The solution is u = f (y) cos x + g(y) sin x, where f (y) and g(y) are two arbitrary functions of y Moral: A PDE has arbitrary functions in its solution Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 16 / 33
29 Important PDEs Partial Differential Equations Transport equation: u t + cu x = 0 Wave equation: u tt = c 2 u xx Diffusion equation: u t = ku xx Laplace equation: u xx + u yy = 0. It is often written as: 2 u = 0 or u = 0, where = 2 is the Laplace operator Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 17 / 33
30 Numerical methods to solve PDEs The three most widely used numerical methods: 1 Finite difference method The simplest method to learn and use Functions are represented by their values at certain grid points, and derivatives are approximated through differences in these values 2 Finite element method 3 Finite volume method Other methods exist: method of lines, spectral methods, multigrid methods,... Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 18 / 33
31 Partial Differential Equations Transport equation: intuition and derivation Yuliya Tarabalka Differential Equations 19 / 33
32 Transport equation: general solution Solve the transport equation u t + cu x = 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 20 / 33
33 Transport equation: general solution Solve the transport equation u t + cu x = 0 You see a wave with speed c: u t + cu x = 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 20 / 33
34 Transport equation: general solution Solve the transport equation u t + cu x = 0 You see a wave with speed c: u t + cu x = 0 I see a stationary wave Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 20 / 33
35 Transport equation: general solution Solve the transport equation u t + cu x = 0 You see a wave with speed c: u t + cu x = 0 I see a stationary wave moving coordinate ξ = x ct Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 20 / 33
36 Transport equation: general solution Solve the transport equation u t + cu x = 0 You see a wave with speed c: u t + cu x = 0 I see a stationary wave moving coordinate ξ = x ct u(x, t) = v(ξ, t) Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 20 / 33
37 Transport equation: general solution Solve the transport equation u t + cu x = 0 You see a wave with speed c: u t + cu x = 0 I see a stationary wave moving coordinate ξ = x ct u(x, t) = v(ξ, t) Derivatives using the chain rule: u t = v ξ ξ t + v t t t v = c ξ + v t Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 20 / 33
38 Transport equation: general solution Solve the transport equation u t + cu x = 0 You see a wave with speed c: u t + cu x = 0 I see a stationary wave moving coordinate ξ = x ct u(x, t) = v(ξ, t) Derivatives using the chain rule: u t = v ξ ξ t + v t t t v = c ξ + v t u x = v ξ ξ x + v t t x = v ξ Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 20 / 33
39 Transport equation: general solution Solve the transport equation u t + cu x = 0 You see a wave with speed c: u t + cu x = 0 I see a stationary wave moving coordinate ξ = x ct u(x, t) = v(ξ, t) Derivatives using the chain rule: u t = v ξ ξ t + v t t t v = c ξ + v t u x = v ξ ξ x + v t t x = v ξ u t + cu x = cv ξ + v t + cv ξ = v t = 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 20 / 33
40 Transport equation: general solution Solve the transport equation u t + cu x = 0 You see a wave with speed c: u t + cu x = 0 I see a stationary wave: v t = 0 moving coordinate ξ = x ct u(x, t) = v(ξ, t) Derivatives using the chain rule: u t = v ξ ξ t + v t t t v = c ξ + v t u x = v ξ ξ x + v t t x = v ξ u t + cu x = cv ξ + v t + cv ξ = v t = 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 20 / 33
41 Transport equation: general solution Usual coordinates (x, t): u(x, t) u t + cu x = 0 Moving coordinates (ξ, t) v(ξ, t) v t = 0 ξ = x ct Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 21 / 33
42 Transport equation: general solution Usual coordinates (x, t): u(x, t) u t + cu x = 0 Moving coordinates (ξ, t) v(ξ, t) v t = 0 ξ = x ct Procedure: solve v t = 0, use to find u(x, t) Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 21 / 33
43 Transport equation: general solution Usual coordinates (x, t): u(x, t) u t + cu x = 0 Moving coordinates (ξ, t) v(ξ, t) v t = 0 ξ = x ct Procedure: solve v t = 0, use to find u(x, t) v t = 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 21 / 33
44 Transport equation: general solution Usual coordinates (x, t): u(x, t) u t + cu x = 0 Moving coordinates (ξ, t) v(ξ, t) v t = 0 ξ = x ct Procedure: solve v t = 0, use to find u(x, t) v t = 0 v = F (ξ) Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 21 / 33
45 Transport equation: general solution Usual coordinates (x, t): u(x, t) u t + cu x = 0 Moving coordinates (ξ, t) v(ξ, t) v t = 0 ξ = x ct Procedure: solve v t = 0, use to find u(x, t) v t = 0 v = F (ξ) v(ξ, t) = u(x, t) Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 21 / 33
46 Transport equation: general solution Usual coordinates (x, t): u(x, t) u t + cu x = 0 Moving coordinates (ξ, t) v(ξ, t) v t = 0 ξ = x ct Procedure: solve v t = 0, use to find u(x, t) v t = 0 v = F (ξ) v(ξ, t) = u(x, t) u(x, t) = F (ξ) = F (x ct) Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 21 / 33
47 Transport equation: general solution Usual coordinates (x, t): u(x, t) u t + cu x = 0 Moving coordinates (ξ, t) v(ξ, t) v t = 0 ξ = x ct Procedure: solve v t = 0, use to find u(x, t) v t = 0 v = F (ξ) v(ξ, t) = u(x, t) u(x, t) = F (ξ) = F (x ct) Conclusion: General solution of u t + cu x = 0 is F (x ct), where F is a once differentiable function Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 21 / 33
48 Initial and boundary conditions Because PDEs typically have so many solutions, we single out one solution by imposing auxiliary conditions These conditions are motivated by the considered problem (ex.: physics) They come in two varieties: initial conditions and boundary conditions Yuliya Tarabalka Differential Equations 22 / 33
49 Initial and boundary conditions An initial condition specifies the physical state at a particular time t 0. We can have one or several initial conditions: u(x, t 0 ) = φ(x) = φ(x, y, z) u u(x, t 0 ) = φ(x) and t (x, t 0) = ψ(x), Examples: φ(x) is the initial position, or the initial temperature,... Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 23 / 33
50 Initial and boundary conditions In each physical domain there is a domain D in which the PDE is valid. Example: For the vibrating string, D is the interval 0 < x < l, where l is the length of the string. The boundary of D consists only of the two points x = 0 and x = l To determine the solution, it is necessary to specify some boundary conditions Three most important kinds of boundary conditions: 1 Dirichlet condition: u is specified 2 Neumann condition: the normal derivative u/ n is specified Example: u/ n = g(x, t) 3 Robin condition: u/ n + au is specified, a = a(x, y, z, t) Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 24 / 33
51 Initial and boundary conditions Three most important kinds of boundary conditions: 1 Dirichlet condition: u is specified 2 Neumann condition: the normal derivative u/ n is specified Example: u/ n = g(x, t) 3 Robin condition: u/ n + au is specified, a = a(x, y, z, t) In one-dimensional problems the boundary consists of two endpoints boundary conditions take the simple form (D) u(0, t) = g(t) and u(l, t) = h(t) (N) u x u (0, t) = g(t) and (l, t) = h(t) x Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 25 / 33
52 Well-posed problems Partial Differential Equations Well-posed problems consist of: a PDE in a domain a set of initial and/or boundary conditions or other auxiliary conditions that enjoy the following fundamental properties 1 Existence: There exists at least one solution u(x, t) satisfying all conditions 2 Uniqueness: There is at most one solution 3 Stability: If the data are changed a little, the solution changes only a little Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 26 / 33
53 Transport equation: method of characteristics Technique for solving PDE by reducing to ODE Yuliya Tarabalka Differential Equations 27 / 33
54 Transport equation: method of characteristics Technique for solving PDE by reducing to ODE x(t) = position of the moving observer Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 27 / 33
55 Transport equation: method of characteristics Technique for solving PDE by reducing to ODE x(t) = position of the moving observer How does u(x, t) change from observer s perspective? Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 27 / 33
56 Transport equation: method of characteristics Technique for solving PDE by reducing to ODE x(t) = position of the moving observer How does u(x, t) change from observer s perspective? d du u(x(t), t) = dt dt = u dx x dt + u t Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 27 / 33
57 Transport equation: method of characteristics Technique for solving PDE by reducing to ODE x(t) = position of the moving observer How does u(x, t) change from observer s perspective? d du u(x(t), t) = dt dt = u dx x dt + u t 0 = cu x + u t Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 27 / 33
58 Transport equation: method of characteristics Technique for solving PDE by reducing to ODE x(t) = position of the moving observer How does u(x, t) change from observer s perspective? d du u(x(t), t) = dt dt = u dx x dt + u t 0 = cu x + u t dx/dt = c - moving with speed c du/dt = 0 - u not changing Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 27 / 33
59 Transport equation: method of characteristics du dt u t + cu x = 0 = 0 along curves given by dx dt = c dx dt = c x = ct + x 0 Need initial condition u(x, 0) = f (x) Along x ct = x 0, u(x, t) = f (x 0 ) = f (x ct) Solution: u(x, t) = f (x ct) Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 28 / 33
60 Transport equation: Exercise Solve the initial value problem (PDE + initial condition): u t + cu x = 1 u(x, 0) = sin x Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 29 / 33
61 Transport equation: Exercise Solve the initial value problem (PDE + initial condition): du dt = u dx x dt + u t u t + cu x = 1 u(x, 0) = sin x Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 29 / 33
62 Transport equation: Exercise Solve the initial value problem (PDE + initial condition): du dt = u dx x dt + u t u t + cu x = 1 u(x, 0) = sin x 1 = u x c + u t Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 29 / 33
63 Transport equation: Exercise Solve the initial value problem (PDE + initial condition): du dt = u dx x dt + u t u t + cu x = 1 u(x, 0) = sin x 1 = u x c + u t dx/dt = c du/dt = 1 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 29 / 33
64 Transport equation: Exercise Solve the initial value problem (PDE + initial condition): du dt = u dx x dt + u t u t + cu x = 1 u(x, 0) = sin x 1 = u x c + u t dx/dt = c du/dt = 1 du dt = 1 u = t + A along characteristic lines Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 29 / 33
65 Transport equation: Exercise Solve the initial value problem (PDE + initial condition): du dt = u dx x dt + u t u t + cu x = 1 u(x, 0) = sin x 1 = u x c + u t dx/dt = c du/dt = 1 du dt = 1 u = t + A along characteristic lines Using an initial condition: u(x, 0) = 0 + sin x A = sin x Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 29 / 33
66 Transport equation: Exercise Solve the initial value problem (PDE + initial condition): du dt = u dx x dt + u t u t + cu x = 1 u(x, 0) = sin x 1 = u x c + u t dx/dt = c du/dt = 1 du dt = 1 u = t + A along characteristic lines Using an initial condition: u(x, 0) = 0 + sin x A = sin x Solution: u(x, t) = t + sin(x ct) Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 29 / 33
67 Solving PDE using Laplace transforms Laplace transforms are well suited to solve linear PDE with constant coefficients If we have a function of two variables w(x, t): L{w(x, t)} = W (x, s) = 0 e st w(x, t)dt Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 30 / 33
68 Solving PDE using Laplace transforms Laplace transforms are well suited to solve linear PDE with constant coefficients If we have a function of two variables w(x, t): L{w(x, t)} = W (x, s) = Transform of partial derivatives: 0 e st w(x, t)dt L{w t (x, t)} = sl{w(x, t)} w(x, 0) = sw (x, s) w(x, 0) L{w tt (x, t)} = s 2 L{w(x, t)} sw(x, 0) w t (x, 0) L{w x (x, t)} = L{w(x, t)} x L{w xx (x, t)} = 2 L{w(x, t)} x 2 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 30 / 33
69 Solving PDE using Laplace transforms: Example Exercise: Solve, via Laplace transforms: w x + 2xw t = 0, w(x, 0) = 0, w(0, t) = t, t 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 31 / 33
70 Solving PDE using Laplace transforms: Example Exercise: Solve, via Laplace transforms: w x + 2xw t = 0, w(x, 0) = 0, w(0, t) = t, t 0 We have: L{w x } + 2xL{w t } = 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 31 / 33
71 Solving PDE using Laplace transforms: Example Exercise: Solve, via Laplace transforms: w x + 2xw t = 0, w(x, 0) = 0, w(0, t) = t, t 0 We have: L{w x } + 2xL{w t } = 0 Apply TOD to obtain: W x + 2x[sW (x, s) w(x, 0)] = 0 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 31 / 33
72 Solving PDE using Laplace transforms: Example Exercise: Solve, via Laplace transforms: w x + 2xw t = 0, w(x, 0) = 0, w(0, t) = t, t 0 We have: L{w x } + 2xL{w t } = 0 Apply TOD to obtain: W x + 2x[sW (x, s) w(x, 0)] = 0 Apply initial conditions: W x + 2xsW = 0 (ODE, 1st-order, linear) Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 31 / 33
73 Solving PDE using Laplace transforms: Example Exercise: Solve, via Laplace transforms: w x + 2xw t = 0, w(x, 0) = 0, w(0, t) = t, t 0 We have: L{w x } + 2xL{w t } = 0 Apply TOD to obtain: W x + 2x[sW (x, s) w(x, 0)] = 0 Apply initial conditions: W x + 2xsW = 0 (ODE, 1st-order, linear) General solution of the separable equation: W (x, s) = A(s)e sx2 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 31 / 33
74 Solving PDE using Laplace transforms: Example Exercise: Solve, via Laplace transforms: w x + 2xw t = 0, w(x, 0) = 0, w(0, t) = t, t 0 We have: L{w x } + 2xL{w t } = 0 Apply TOD to obtain: W x + 2x[sW (x, s) w(x, 0)] = 0 Apply initial conditions: W x + 2xsW = 0 (ODE, 1st-order, linear) General solution of the separable equation: W (x, s) = A(s)e sx2 Obtain A(s): W (0, s) = L{w(0, t)} = L{t} = 1/s 2 A(s) = 1/s 2 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 31 / 33
75 Solving PDE using Laplace transforms: Example Exercise: Solve, via Laplace transforms: w x + 2xw t = 0, w(x, 0) = 0, w(0, t) = t, t 0 We have: L{w x } + 2xL{w t } = 0 Apply TOD to obtain: W x + 2x[sW (x, s) w(x, 0)] = 0 Apply initial conditions: W x + 2xsW = 0 (ODE, 1st-order, linear) General solution of the separable equation: W (x, s) = A(s)e sx2 Obtain A(s): W (0, s) = L{w(0, t)} = L{t} = 1/s 2 A(s) = 1/s 2 W (x, s) = 1 s 2 e sx2 Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 31 / 33
76 Solving PDE using Laplace transforms: Example Exercise: Solve, via Laplace transforms: w x + 2xw t = 0, w(x, 0) = 0, w(0, t) = t, t 0 W (x, s) = 1 s 2 e sx2 Second shifting theorem: L 1 {e cs F (s)} = u c (t)f (t c), where the Heaviside (unit step) function: 0, t < c; u c (t) = 1, t c F (s) = 1 s 2 f (t) = t w(x, t) = L 1 { 1 s 2 e sx2 } = u x 2(t)[t x 2 ] Yuliya Tarabalka (yuliya.tarabalka@inria.fr) Differential Equations 32 / 33
77 Partial differential equations Other analytical methods exist: Separation of variables Change of variables Fundamental solution You can read more here: W. A. Strauss, Partial Differential Equations: An Introduction, John Wiley & Sons Ltd, 2008 Yuliya Tarabalka Differential Equations 33 / 33
Mathematical Methods - Lecture 7
Mathematical Methods - Lecture 7 Yuliya Tarabalka Inria Sophia-Antipolis Méditerranée, Titane team, http://www-sop.inria.fr/members/yuliya.tarabalka/ Tel.: +33 (0)4 92 38 77 09 email: yuliya.tarabalka@inria.fr
First order wave equations. Transport equation is conservation law with J = cu, u t + cu x = 0, < x <.
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