Prove that the functions (a)
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Numerical Analysis
- A particle's position vector is given by: F(t) = R(1+ cos(wot + q cos wot))& + R sin(wnt + q cos wot)ŷ (= What is the particle's maximum speed? If it helps, you can assume that R, wo, and q are all positive numbers, and that q is very small.arrow_forwardPlease don't provide handwritten solution....arrow_forwardConsider the wave equation: utt = uxx, −∞ < x < ∞, t > 0 with ut(x, 0) = 0 and u(x, 0) = ( 0, x < 0 and x > π) u(x, 0) = cos2 x, 0 ≤ x ≤ π a)Find a solution to this problem using the D’Alembert’s formula. Then, plot the solution at t = 0, π /4 , π /2 , π b)Find a solution to this problem using the Fourier transform and show that your solution is the same as part (a).arrow_forward
- 10. a) The function y(x,t) = x² + v?t? describes a wave. This wave can be written as a sum of two functions f, and f2 as follows: y(x,t) = fi(x – vt) + f2(x + vt). Find the two function f, and f2. b) The function y(x,t) = sin(x) cos(vt) also describes a wave. This wave can be written as a sum of two other functions f3 and fa as follows: y(x,t) = f3(x – vt) + f4(x + vt). Find the two function f3 and f4.arrow_forward(a) Solve the inhomogeneous 1st order equation UU. U(,0) 0. wwwwwww SS - cos t (b) Solve the inhomogeneous wave equation on the real line Ute - c²U #sina, rER U(x,0) = 0, U.(,0) = 0. Explain what theory you are using and show your full computations. +arrow_forwardLet R be a vector function such that T(t) Find = co cos 2t ) 1 √3 ² sin 2t) and R(0) = (1, 0. –1). 2' 2 An equation of the osculating, rectifying, and normal planes to the graph of R at t = 0.arrow_forward
- Select the wave equation by utilizing separate variables with initial conditions?arrow_forwardWhich of the following vector-valued functions represent the same graph? (Select all that apply.) r(t) = (-5 cos(t) + 4)i + (6 sin(t) + 5)j + 4k r(t) = 4i + (-5 cos(t) + 4)j + (6 sin(t) + 5)k r(t) = (5 cos(t) — 4)i + (−6 sin(t) – 5)j + 4k - ✔r(t) = (-5 cos(2t) + 4)i + (6 sin(2t) + 5)j + 4karrow_forwardQ.5 Solve the wave equation: U, =U xx-e* –6x, U (0,t) =8, Ux(l,t)= 3, 57 U(x,0) = 4 sin x+e* + x3 – ex+7 %3D .... .... ............arrow_forward
- (a) Show that the function y(x, t) = x2 + v²t is a solution to the wave equation, by calculating the following quantities and expressing each in terms of x, v, and t. dy/at = dy/dx = (a?y/ar?)/v2 = y/ax? = (b) Show that the function in part (a) can be written as f(x + vt) + g(x - vt), and determine the functional forms for f and g. f(x + vt) = g(x- vt) = (c) Repeat parts (a) and (b) for the function y(x, t) = sin (x) cos (vt). dy/at = dy/dx = %3D azy/ax? = f(x + vt) = g(x- vt) =arrow_forward4. Consider a vibrating string of length L = n that satisfies the wave equation 4- 0 0. Assume that the ends of the string are fixed, and that the string is set in motion with no initial velocity from the initial position u(x,0) = 12 sin 2x – 16 sin 5x + 24 sin 6x. Find the displacement u(r, t) of the string.arrow_forwardThe technique that we used to solve the time-dependent Schrodinger equation in class is known as separation of variables. Use the same technique to investigate solutions of the wave equation: ∂2y(x,t)∂x2=1v2∂2y(x,t)∂t2arrow_forward
- Algebra & Trigonometry with Analytic GeometryAlgebraISBN:9781133382119Author:SwokowskiPublisher:Cengage