Solve the wave equation utt = c²(uxx + Uyy) in the square D = {0 < x,y < } with homogeneous Neumann conditions on the boundary (du/an = 0) and the initial conditions u(x, y,0) = 0, ut(x, y,0) = sin(x).
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- Q5) Solve the wave equation for vibration of organ pipe subject to the boundary condition: a- u(0,t)=0, t>=0 du(1,1) b- ax - 0,1 20 ди(х.0) -U, cons tant с- d- u(x.0) =0.0<=x<=LFind the TNB frame. r(t) = (3sint)i + (3cost)j + 4tk r(t)=(cost + tsint)i+(sint - tcost)j + 3k r(t) = (e^t × cost)i + (e^t × sint) j + 2k r(t) = (6sin 2t) i + (6cos 2t) j + 5tkLet f(x,t)=cos(12x+4t). Find the value of K so that f satisfies the wave equation ∂^2f/∂x2=K∂^2f/∂t^2
- Solve the inhomogeneous wave equation on the real lineUtt − c2Uxx = sin x, x ∈ RU(x, 0) = 0, Ut(x, 0) = 0.Explain what theory you are using and show your full computations.8) Find the position vector r(t) for a particle with acceleration a(t) = (5t, 5 sin t, cos 6t), initial velocity (0) = (3, -3, 1) and initial position (0) = (5, 0, -2).Which of the following is most suitable solution for wave equation = c2? %3D at2 ax2 .(a) y = (AeP* + Be-P*)(Ce pt + De ept) (b) y = (Acos px + Bsin px)(Ccos cpt + Dsin cpt) (c) y = (Ax + B)(Ct + D) (d) y = (Aepx + Be-px)(Cep*t + De-ep*r) O a O b O c O d
- (2) Sketch the direction field associated to the system I'=x²-y-3, y = y + x² - 5. Include the x-nullclines, y-nullclines, equilibria and ordinal directions in the remaining regions.a²u B/ Solve the wave equation: 01² 3x² Under the condition: u=0 when x = 0 and x = 1 ди = 0 when t = 0 and u(x,0) = x², at a²! a = 1 0 < x < 1.Find the solution to the wave equation on half-line: Utt=C²Uzr x > 0, t > 0, u(0, t) = 0, t> 0, u(x,0)=1/x, u₁(x,0) = e, x > 0.
- Consider the wave equation Utt Uzz; 0 < x,t < ñ, u (0, t) u (T, t) = 0,0 < t < «. (a) Show that u (x, t) = sin x sin t is a solution of the above problem. (b) Find the maximum of u (x, t) on [0, 7]² . (c) Show that the above wave equation do not necessarily satisfy the maximum principle.Consider the wave equation 0 0, with u(0,1) = 1(xt)= 0, u(x,0) = sin x and =0 at t=0. Then u isSuppose a particle, whose initial position is (1, 0, 0), moves with velocity given by v(t) = (-1, cos(t), - sin(t)). Compute the vector-valued function that represents the particle's position at any time t = [0, 2π].