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This example shows how to use functional derivatives in the Symbolic Math Toolbox™ using the example of the wave equation. This example performs calculations symbolically to obtain analytic results. The wave equation for a string fixed at its ends is solved using functional derivatives. A functional derivative is the derivative of a functional with respect to the function that the functional depends on. The Symbolic Math Toolbox™ implements functional derivatives using the `functionalDerivative`

function.

Solving the wave equation is one application of functional derivatives. It describes the motion of waves, from the motion of a string to the propagation of an electromagnetic wave, and is an important equation in physics. You can apply the techniques illustrate in this example to applications in the calculus of variations from solving the Brachistochrone problem to finding minimal surfaces of soap bubbles.

Consider a string of length `L`

suspended between the two points `x = 0`

and `x = L`

. The string has a characteristic density per unit length and a characteristic tension. Define the length, density, and tension as constants for later use. For simplicity, set these constants to `1`

.

Length = 1; Density = 1; Tension = 1;

If the string is in motion, the string's kinetic and potential energies are a function of its displacement from rest `S(x,t)`

, which varies with position `x`

and time `t`

. If `d`

is the density per unit length, the kinetic energy is

$$T={\int}_{0}^{L}\frac{d}{2}{(\frac{d}{dt}S(x,t))}^{2}dx.$$

The potential energy is

$$V={\int}_{0}^{L}\frac{r}{2}{(\frac{d}{dx}S(x,t))}^{2}dx,$$

where *r* is the tension.

Enter these equations in MATLAB®. Since length must be positive, set this assumption. This assumption allows `simplify`

to simplify the resulting equations into the expected form.

syms S(x,t) d r v L assume(L>0) T(x,t) = int(d/2*diff(S,t)^2,x,0,L); V(x,t) = int(r/2*diff(S,x)^2,x,0,L);

The action `A`

is `T-V`

. The Principle of Least Action states that action is always minimized. Determine the condition for minimum action, by finding the functional derivative of `A`

with respect to `S`

using `functionalDerivative`

and equate it to zero.

A = T-V; eqn = functionalDerivative(A,S) == 0

eqn(x, t) =$$L\hspace{0.17em}r\hspace{0.17em}\frac{{\partial}^{2}}{\partial {x}^{2}}\mathrm{}S\left(x,t\right)-L\hspace{0.17em}d\hspace{0.17em}\frac{{\partial}^{2}}{\partial {t}^{2}}\mathrm{}S\left(x,t\right)=0$$

Simplify the equation using `simplify`

. Convert the equation into its expected form by substituting for `r/d`

with the square of the wave velocity `v`

.

eqn = simplify(eqn)/r; eqn = subs(eqn,r/d,v^2)

eqn(x, t) =$$\frac{\frac{{\partial}^{2}}{\partial {t}^{2}}\mathrm{}S\left(x,t\right)}{{v}^{2}}=\frac{{\partial}^{2}}{\partial {x}^{2}}\mathrm{}S\left(x,t\right)$$

Solve the equation using the method of separation of variables. Set `S(x,t) = U(x)*V(t)`

to separate the dependence on position `x`

and time `t`

. Separate both sides of the resulting equation using `children`

.

syms U(x) V(t) eqn2 = subs(eqn,S(x,t),U(x)*V(t)); eqn2 = eqn2/(U(x)*V(t))

eqn2(x, t) =$$\frac{\frac{{\partial}^{2}}{\partial {t}^{2}}\mathrm{}V\left(t\right)}{{v}^{2}\hspace{0.17em}V\left(t\right)}=\frac{\frac{{\partial}^{2}}{\partial {x}^{2}}\mathrm{}U\left(x\right)}{U\left(x\right)}$$

tmp = children(eqn2);

Both sides of the equation depend on different variables, yet are equal. This is only possible if each side is a constant. Equate each side to an arbitrary constant `C`

to get two differential equations.

```
syms C
eqn3 = tmp(1) == C
```

eqn3 =$$\frac{\frac{{\partial}^{2}}{\partial {t}^{2}}\mathrm{}V\left(t\right)}{{v}^{2}\hspace{0.17em}V\left(t\right)}=C$$

eqn4 = tmp(2) == C

eqn4 =$$\frac{\frac{{\partial}^{2}}{\partial {x}^{2}}\mathrm{}U\left(x\right)}{U\left(x\right)}=C$$

Solve the differential equations using `dsolve`

with the condition that displacement is `0`

at `x = 0`

and `t = 0`

. Simplify the equations to their expected form using `simplify`

with the `Steps`

option set to `50`

.

```
V(t) = dsolve(eqn3,V(0)==0,t);
U(x) = dsolve(eqn4,U(0)==0,x);
V(t) = simplify(V(t),'Steps',50)
```

`V(t) = $$-2\hspace{0.17em}{C}_{1}\hspace{0.17em}\mathrm{sinh}\left(\sqrt{C}\hspace{0.17em}t\hspace{0.17em}v\right)$$`

`U(x) = simplify(U(x),'Steps',50)`

`U(x) = $$2\hspace{0.17em}{C}_{1}\hspace{0.17em}\mathrm{sinh}\left(\sqrt{C}\hspace{0.17em}x\right)$$`

Obtain the constants in the equations.

p1 = setdiff(symvar(U(x)),sym([C,x]))

`p1 = $${C}_{1}$$`

p2 = setdiff(symvar(V(t)),sym([C,v,t]))

`p2 = $${C}_{1}$$`

The string is fixed at the positions `x = 0`

and `x = L`

. The condition `U(0) = 0`

already exists. Apply the boundary condition that `U(L) = 0`

and solve for `C`

.

```
eqn_bc = U(L) == 0;
[solC,param,cond] = solve(eqn_bc,C,'ReturnConditions',true)
```

solC =$$-\frac{{k}^{2}\hspace{0.17em}{\pi}^{2}}{{L}^{2}}$$

`param = $$k$$`

`cond = $$k\in \mathbb{Z}\wedge {C}_{1}\ne 0\wedge 1\le k$$`

assume(cond)

The solution `S(x,t)`

is the product of `U(x)`

and `V(t)`

. Find the solution, and substitute the characteristic values of the string into the solution to obtain the final form of the solution.

S(x,t) = U(x)*V(t); S = subs(S,C,solC); S = subs(S,[L v],[Length sqrt(Tension/Density)]);

The parameters `p1`

and `p2`

determine the amplitude of the vibrations. Set `p1`

and `p2`

to `1`

for simplicity.

```
S = subs(S,[p1 p2],[1 1]);
S = simplify(S,'Steps',50)
```

`S(x, t) = $$4\hspace{0.17em}\mathrm{sin}\left(\pi \hspace{0.17em}k\hspace{0.17em}t\right)\hspace{0.17em}\mathrm{sin}\left(\pi \hspace{0.17em}k\hspace{0.17em}x\right)$$`

The string has different modes of vibration for different values of `k`

. Plot the first four modes for an arbitrary value of time `t`

. Use the `param`

argument returned by `solve`

to address parameter `k`

.

Splot(x) = S(x,0.3); figure(1) hold on grid on ymin = double(coeffs(Splot)); for i = 1:4 yplot = subs(Splot,param,i); fplot(yplot,[0 Length]) end ylim([-ymin ymin]) legend('k = 1','k = 2','k = 3','k = 4','Location','best') xlabel('Position (x)') ylabel('Displacement (S)') title('Modes of a string')

The wave equation is linear. This means that any linear combination of the allowed modes is a valid solution to the wave equation. Hence, the full solution to the wave equation with the given boundary conditions and initial values is a sum over allowed modes

$$F(x,t)=\sum _{k=n}^{m}{A}_{k}\mathrm{sin}(\pi kt)\mathrm{sin}(\pi kx),$$

where $${A}_{k}$$ denotes arbitrary constants.

Use `symsum`

to sum the first five modes of the string. On a new figure, display the resulting waveform at the same instant of time as the previous waveforms for comparison.

figure(2) S5(x) = 1/5*symsum(S,param,1,5); fplot(subs(S5,t,0.3),[0 Length]) ylim([-ymin ymin]) grid on xlabel('Position (x)') ylabel('Displacement (S)') title('Summation of first 5 modes')

The figure shows that summing modes allows you to model a qualitatively different waveform. Here, we specified the initial condition is $$S(x,t=0)=0$$ for all $$x$$.

You can calculate the values $${A}_{k}$$ in the equation $$F(x,t)=\sum _{k=n}^{m}{A}_{k}\mathrm{sin}(\pi kt)\mathrm{sin}(\pi kx)$$ by specifying a condition for initial velocity

$${u}_{t}(x,t=0)={F}_{t}(x,0).$$

The appropriate summation of modes can represent any waveform, which is the same as using the Fourier series to represent the string's motion.