{[ promptMessage ]}

Bookmark it

{[ promptMessage ]}


mechanical_waves_travel - MECHANICAL WAVES(TRAVELLING We...

Info iconThis preview shows pages 1–2. Sign up to view the full content.

View Full Document Right Arrow Icon
Background image of page 1

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full Document Right Arrow Icon
Background image of page 2
This is the end of the preview. Sign up to access the rest of the document.

Unformatted text preview: MECHANICAL WAVES (TRAVELLING) We begin our discussion of the wave phenomenon by considering waves in matter. The simplest definition of a wave is to call it a traveling disturbance (or equivalently, deviation from equilibrium). For instance, if you drop a stone on the surface of an undisturbed body of water you can watch the “disturbance” traveling radially out of the “point” of contact. Formally, we can “construct” a wave in several steps. For simplicity, we take a wave traveling along x—axis. Step 1. We need a disturbance D. Step 2. D must be a function of x. Step 3. D must also be a function of t. Step 4. If x and t appear in the function in the combinations (x Trvt) the disturbance D cannot be stationary. It must travel along x with speed v. Further, (x—vt) implies v = vfltravel in+ ivex — direction] —) (x+vt) implies v = —v£[travel in— we): — direction] ._) EXERCIZE: Put D = A(x — If)2 and show that “parabola” travels. Periodic Waves The simplest wave is when (x-vt) appears in a sin or cos function. D = sin (x—vt) But this equation is not justified. First, since D is a disturbance it must have dimensions so we need D: A Sin(x— vt) Where A has the dimensions of D. Next, argument of Sin cannot have dimensions, so we need (x— vt) /l D=A Sin v Where 1 is alength. Since A has dimension of (l/Time), put is: % 275x 2m Next, introduce a phase angle Q and we get D = A Sin(7— 7+ Q) as the most general periodic wave. Note that 27: has been put in, as we know repeat angle for Sin. If you put Q = 7? you recover the Equation in some books. . 2m 27m) D— ASm[ T — A As shown in class xt = Repeat Distance= wavelength . 1 T = perlod, E = f (frequency) And v = ftf 27$ Next, define k = 7 (wave vector) 0) = 27tf (angular frequency) a) = vk And we can write D = A Sin (kx — wt + Q) for any periodic wave traveling a long +z've x—axis A x H a) with velocity v I 4, Similarly, D = A Sin (be + wt + Q) is any periodic wave along —ive x-axis with ...
View Full Document

{[ snackBarMessage ]}

Page1 / 2

mechanical_waves_travel - MECHANICAL WAVES(TRAVELLING We...

This preview shows document pages 1 - 2. Sign up to view the full document.

View Full Document Right Arrow Icon bookmark
Ask a homework question - tutors are online