blog
Blog
## Intro

## Deriving impedance

#### Side note: recall from Waves I

## Relating to Power

## Closing remarks

### Related

In this brief part of the waves series, we will be defining the concept of impedance of a string. *Impedance* is an important concept in many physical systems, as it will usually impact how much energy you are able to transmit across certain boundaries. Quite often in physics (and other fields), we're trying to solve problems where we need to do some sort of impedance matching. We will tackle this type of problem in a later post.

You may already be familiar with a type of impedance if you've studied electrical circuits. Indeed, you can find analogues (no pun intended) in electrical systems for most of the concepts involved here. We will also investigate this later, when we derive the wave equation for an electrical transmission line.

While I won't be continuing on from where we left off in Waves IV, I will assume that you know about everything we covered in the previous parts. You can find part 1 here.

Imagine again a stretched string along which a wave needs to be propagated. In order to create a sinusoidal waves of the form $y(x,t) = y(x\pm ct)$ (as investigated in part 2), we presumably had to apply some harmonic time-varying force, which we'll call $F_y$.

At any given moment in time, the applied force, $F_y$, must be whatever is required to balance the transverse component of the tension, $T$, on the string. This is shown here:

Forces at a point $x=x_0$ on a string.

We can balance the forces in this system at the point $x=x_0$ to get:

$$F_y = - T\sin \theta \approx - T\tan \theta = - T\frac{\partial y}{\partial x}|_{x=x_0}$$

Recall from Waves I, that for a small angle $\theta$, we can apply the small angle approximation $\sin \theta \approx \tan \theta$. Also recall that the slope at a point, $x_0$, on the string is $\frac{\partial y}{\partial x}|_{x=x_0}=\tan \theta$, where $\theta$ is the angle with the horizontal at that point on the string.

Now, remember from Waves II, that for a constant-shape travelling wave *moving in the positive x-direction* with a solution of the form $y(x,t) = y(x - ct)$, we have the important relation:

$$\frac{\partial y}{\partial t} = - c\frac{\partial y}{\partial x}$$ $$\Rightarrow \frac{\partial y}{\partial x} = - \frac{1}{c} \frac{\partial y}{\partial t}$$

Substituting this into the expression for $F_y$:

$$F_y = \frac{T}{c} \frac{\partial y}{\partial t}|_{x=x_0}$$

Now, it's important to note that the expression $\frac{\partial y}{\partial t}|_{x=x_0}$ is exactly the transverse (vertical) velocity of the string at the point $x_0$, which we'll call $v_y$. So we can write:

$$\Rightarrow F_y = \frac{T}{c} v_y$$

Recall again that $c$, the speed of the waves on the string, is given by $c = \sqrt{\frac{T}{\rho}}$, so we can rewrite this as:

$$\Rightarrow F_y = \sqrt{T\rho} v_y$$

This quantity, $\sqrt{T\rho}$, is defined as the *characteristic impedance of the string*:

$$Z = \sqrt{T\rho}$$

This is because the definition of the *mechanical impedance of a physical system* is the ratio of the force applied at a point to the resulting velocity of that point. This is exactly our case. A force $F_y$ acts to balance the vertical component of tension on the string and results in a velocity $v_y$, such that:

$$\frac{F_y}{v_y} = \sqrt{T\rho} = Z$$

$$\Rightarrow F_y = Z v_y$$

In analogy to electrical circuits, this is the *"Ohm's law"* ($V = IR$) of the string on the wave! This is such that $F_y$ represents the voltage, $V$, $v_y$ represents the current in the circuit $I$, and Z, the impedance, naturally represents the resistance of a circuit element, $R$.

Remember the final result from our consideration of power in Waves IV, which was:

$$P = \frac{1}{2} A^2\omega^2\sqrt{T\rho}$$

We can now rewrite this in terms of the impedance, $Z$:

$$P = \frac{1}{2} A^2\omega^2 Z$$

While we're here, and since we considered the transverse velocity of the string in this post, we can also consider a different definition of power to the one we took in Waves IV.

Consider the definition $P = Fv$ of power. In our case, $F$ is the transverse force acting on the string: $F = F_y$ and $v$, naturally, is the transverse velocity resulting from the force: $v = v_y$. From the equations derived above for $F_y$ and $v_y$:

$$F_y = - T\frac{\partial y}{\partial x}|_{x=x_0}, v_y = \frac{\partial y}{\partial t}|_{x=x_0},$$

we can write (omitting $x=x_0$):

$$P = - T\frac{\partial y}{\partial x}\frac{\partial y}{\partial t}$$

Applying again the relation $\frac{\partial y}{\partial x} = - \frac{1}{c} \frac{\partial y}{\partial t}$:

$$P = \frac{T}{c}(\frac{\partial y}{\partial t})^2 = Zv_y^2$$

This is again analogous to electrical circuits: $P = I^2R$!

Thanks for reading! As always, I hope you found this post informative.

Feel free to message me with any questions you have about this topic either through the website or by leaving a comment below!

*Happy Physics-ing!*

*Update (06/06/2018)*: *Waves VI* is now up, here.

You may also be interested in:

Waves IV: Power transported by a Wave on a String

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