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By the end of this section, you will be able to:
  • Explain how mechanical waves are reflected and transmitted at the boundaries of a medium
  • Define the terms interference and superposition
  • Find the resultant wave of two identical sinusoidal waves that differ only by a phase shift

Up to now, we have been studying mechanical waves that propagate continuously through a medium, but we have not discussed what happens when waves encounter the boundary of the medium or what happens when a wave encounters another wave propagating through the same medium. Waves do interact with boundaries of the medium, and all or part of the wave can be reflected. For example, when you stand some distance from a rigid cliff face and yell, you can hear the sound waves reflect off the rigid surface as an echo. Waves can also interact with other waves propagating in the same medium. If you throw two rocks into a pond some distance from one another, the circular ripples that result from the two stones seem to pass through one another as they propagate out from where the stones entered the water. This phenomenon is known as interference. In this section, we examine what happens to waves encountering a boundary of a medium or another wave propagating in the same medium. We will see that their behavior is quite different from the behavior of particles and rigid bodies. Later, when we study modern physics, we will see that only at the scale of atoms do we see similarities in the properties of waves and particles.

Reflection and transmission

When a wave propagates through a medium, it reflects when it encounters the boundary of the medium. The wave before hitting the boundary is known as the incident wave. The wave after encountering the boundary is known as the reflected wave. How the wave is reflected at the boundary of the medium depends on the boundary conditions; waves will react differently if the boundary of the medium is fixed in place or free to move ( [link] ). A fixed boundary condition    exists when the medium at a boundary is fixed in place so it cannot move. A free boundary condition    exists when the medium at the boundary is free to move.

Figure a shows two figures of a string attached to a rigid support at the right. The top string is labeled before reflection. A pulse formed at the top of the string propagates towards the right with velocity v subscript i. The bottom string is labeled after reflection. A pulse formed at the bottom of the string propagates towards the left with velocity v subscript R. Figure b shows two figures of a string attached to a ring that is passed through a pole on the right. The top string is labeled before reflection. A pulse formed at the top of the string propagates towards the right with velocity v subscript i. The bottom string is labeled after reflection. A pulse formed at the top of the string propagates towards the left with velocity v subscript R.
(a) One end of a string is fixed so that it cannot move. A wave propagating on the string, encountering this fixed boundary condition , is reflected 180 ° ( π rad ) out of phase with respect to the incident wave. (b) One end of a string is tied to a solid ring of negligible mass on a frictionless lab pole, where the ring is free to move. A wave propagating on the string, encountering this free boundary condition , is reflected in phase 0 ° ( 0 rad ) with respect to the wave.

Part (a) of the [link] shows a fixed boundary condition. Here, one end of the string is fixed to a wall so the end of the string is fixed in place and the medium (the string) at the boundary cannot move. When the wave is reflected, the amplitude of the reflected way is exactly the same as the amplitude of the incident wave, but the reflected wave is reflected 180 ° ( π rad ) out of phase with respect to the incident wave. The phase change can be explained using Newton’s third law: Recall that Newton’s third law states that when object A exerts a force on object B , then object B exerts an equal and opposite force on object A . As the incident wave encounters the wall, the string exerts an upward force on the wall and the wall reacts by exerting an equal and opposite force on the string. The reflection at a fixed boundary is inverted. Note that the figure shows a crest of the incident wave reflected as a trough. If the incident wave were a trough, the reflected wave would be a crest.

Practice Key Terms 6

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Source:  OpenStax, University physics volume 1. OpenStax CNX. Sep 19, 2016 Download for free at http://cnx.org/content/col12031/1.5
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