Sound

Storyboard

Sound are fluctuations in the density of a gas, liquid or solid that are capable of propagating in the medium.

>Model

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Mechanisms

Definition


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Sound

Image

The sound is described as fluctuations in the densities of the particles within the medium through which it propagates. These fluctuations are characteristic of sound, whether it occurs in gases, liquids, or solids.

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Sound generation

Note

The sound is produced when a surface moves, either increasing or decreasing the volume of gas.

In the first case, the surrounding molecules will occupy the new space, creating a zone of lower air density that will be filled by other neighboring molecules.

In the second case, the surrounding molecules are compressed, resulting in a displacement towards regions of lower density.

Altoparlante

Both changes lead to the propagation of reductions or increases in density, which corresponds to a sound wave.

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Movement of molecules

Quote

The oscillation of a molecule due to a sound wave can be described in terms of its position and velocity.

If both are plotted as edges on a graph, an elliptical trajectory can be observed. At the vertical extreme points, the particle reaches maximum velocity, with one end being positive (moving from left to right) and the other end being negative (moving from right to left). The horizontal extreme points represent the amplitude, with the left point indicating a minimum value and the right point indicating a positive value.

Similarly, these oscillations can be represented as a function of the time ($t$). If we start from a point where the amplitude Oscillation Molecule ($a$) is initially negative and maximum, the velocity is described by a sine function, while the average Position of the Molecule ($x$) is described by a cosine function that initially has an amplitude negative. However, this choice is arbitrary, since the cycle can start from any other point, for example, when the amplitude is initially zero, as is the case when the sound wave arrives. In the latter case, the position is modeled with a sine function.

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Propagation of sound

Exercise

Sound is generated when a surface moves, either increasing or decreasing the volume of a gas.

Once a density/pressure variation is created, it propagates at the wave speed ($c$):

Altoparlante



This is why we are able to hear the sound produced by a speaker.

It is important to recognize:

Sound requires a medium in which density/pressure varies, whether it's gas, liquid, or solid. Therefore, sound cannot propagate in a vacuum.

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Model

Equation


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Sound

Storyboard

Sound consists of fluctuations in the density of a gas, liquid, or solid that can propagate through the medium. Sound exists in all media gas, liquid, or solid with differences in propagation speed and attenuation, although the models that describe it are generally similar.

Variables

Symbol
Text
Variable
Value
Units
Calculate
MKS Value
MKS Units
$a$
a
Amplitude Oscillation Molecule
m
$\omega$
omega
Angular frequency
rad/s
$x$
x
Average Position of the Molecule
m
$u$
u
Molecule speed
m/s
$T$
T
Period
s
$\nu$
nu
Sound frequency
Hz
$t$
t
Time
s
$c$
c
Wave speed
m/s
$\lambda$
lambda
Wavelength
m

Calculations


First, select the equation:   to ,  then, select the variable:   to 

Symbol
Equation
Solved
Translated

Calculations

Symbol
Equation
Solved
Translated

 Variable   Given   Calculate   Target :   Equation   To be used



Equations


Examples


mechanisms

The sound is described as fluctuations in the densities of the particles within the medium through which it propagates. These fluctuations are characteristic of sound, whether it occurs in gases, liquids, or solids.

The sound is produced when a surface moves, either increasing or decreasing the volume of gas.

In the first case, the surrounding molecules will occupy the new space, creating a zone of lower air density that will be filled by other neighboring molecules.

In the second case, the surrounding molecules are compressed, resulting in a displacement towards regions of lower density.

image

Both changes lead to the propagation of reductions or increases in density, which corresponds to a sound wave.

The oscillation of a molecule due to a sound wave can be described in terms of its position and velocity.

If both are plotted as edges on a graph, an elliptical trajectory can be observed. At the vertical extreme points, the particle reaches maximum velocity, with one end being positive (moving from left to right) and the other end being negative (moving from right to left). The horizontal extreme points represent the amplitude, with the left point indicating a minimum value and the right point indicating a positive value.

Similarly, these oscillations can be represented as a function of the time ($t$). If we start from a point where the amplitude Oscillation Molecule ($a$) is initially negative and maximum, the velocity is described by a sine function, while the average Position of the Molecule ($x$) is described by a cosine function that initially has an amplitude negative. However, this choice is arbitrary, since the cycle can start from any other point, for example, when the amplitude is initially zero, as is the case when the sound wave arrives. In the latter case, the position is modeled with a sine function.

image

Sound is generated when a surface moves, either increasing or decreasing the volume of a gas.

Once a density/pressure variation is created, it propagates at the wave speed ($c$):

image

This is why we are able to hear the sound produced by a speaker.

It is important to recognize:

Sound requires a medium in which density/pressure varies, whether it's gas, liquid, or solid. Therefore, sound cannot propagate in a vacuum.


model

The average motion generated by the sound wave corresponds to an oscillation around the molecule's original position.

This oscillation can be described using a trigonometric function that involves an amplitude $a$, an angular frequency $\omega$, and time $t$.

The oscillation is described as follows:

kyon

The sound frequency ($\nu$) corresponds to the number of times an oscillation occurs within one second. The period ($T$) represents the time it takes for one oscillation to occur. Therefore, the number of oscillations per second is:

kyon

Frequency is indicated in Hertz (Hz).

If we consider the velocity versus position diagram, we can interpret oscillation as circular motion in this diagram. In that case, we can estimate ERROR:5715 as the perimeter, which is the distance traveled divided by the elapsed time, which is the period ($T$). If the amplitude Oscillation Molecule ($a$) is the radius, then with the angular frequency ($\omega$):

$u=\displaystyle\frac{2\pi a}{T}=a\omega$



This means that ERROR:5715 is:

kyon

The wave speed ($c$) is a velocity, which means it is equal to a length, such as the wavelength ($\lambda$), divided by the time it takes for one oscillation to advance, i.e., the periodo del resorte ($T$). Therefore, we have:

kyon

The speed of sound ($c$) is a velocity, which means it is equal to a length, such as the wavelength of Sound ($\lambda$), divided by the time it takes for one oscillation to advance. Since the inverse of time is the sound frequency ($\nu$), we have:

kyon

Con list=12335 la frecuencia angular es

equation=12335



y con list=4427 la frecuencia

equation=4427



se puede reescribir con list la frecuencia angular es

kyon


>Model

ID:(385, 0)