Sound Waves and the Acoustic Spectrum | Ultrasound Physics | Radiology Physics Course #1 — Transcript
Full transcript
- 0:00Hello and welcome to the ultrasound
- 0:01physics module. My name is Dr. Michael
- 0:03Now. Now in the next series of talks
- 0:05we're going to be diving into the world
- 0:07of ultrasound physics and before we get
- 0:08started in today's talk, I want to make
- 0:10sure we have a clear concept of what
- 0:12exactly a sound wave is and what it
- 0:15isn't and we'll start by having a look
- 0:16at the definition. Now sound is
- 0:18mechanical energy that propagates
- 0:20through a continuous elastic medium by
- 0:23the compression and rarefaction of the
- 0:25units in that medium. So let's break
- 0:27down this definition a little bit more.
- 0:29It's mechanical energy. It's not
- 0:31self-propagating energy like in our
- 0:33electromagnetic radiation. It requires a
- 0:35mechanical force. When we are creating
- 0:37sound, we are mechanically moving our
- 0:40voice box. When we create ultrasound
- 0:42waves, we are moving an element within
- 0:44that ultrasound. And that energy
- 0:46propagates through a medium that needs
- 0:48to be continuous. Sound needs a medium
- 0:51to propagate. When we looked at
- 0:52electromagnetic radiation, it could
- 0:54travel through a vacuum because it's
- 0:56self-propagating. Here sound is
- 0:58dependent on a medium. And if that
- 1:00medium's not continuous, there are
- 1:02regions of vacuum within that plane, the
- 1:05sound will not propagate. Secondly, the
- 1:08medium needs to be elastic. Now, what
- 1:10does that mean? Well, the molecules or
- 1:12the units within that medium need to be
- 1:14able to move, transfer energy, and
- 1:17return back to where they started. If I
- 1:20had my hand in some water and I push the
- 1:22water, the molecules that I initially
- 1:24pushed will then return back to where
- 1:26they were and a wave will propagate
- 1:28through that water. If I had a pile of
- 1:31sand in front of me and I push the sand
- 1:33like that, a wave wouldn't propagate
- 1:35through that sand. The sand that I
- 1:37pushed wouldn't return back to its
- 1:39resting place and we wouldn't get that
- 1:40transfer of energy. The sand has no
- 1:42elasticity. And we'll look in later
- 1:45talks at the elastic and inertial
- 1:47properties of a medium and how that
- 1:48affects the speed of the wave traveling
- 1:50through that medium.
- 1:52So when we look at a wave, we can see
- 1:54its regions of compression and
- 1:56rarefaction. Now these regions of
- 1:58compression and rarefaction represent
- 2:01localized pressure changes within that
- 2:03medium, and we can plot those pressure
- 2:05changes on a graph, and we get a sine
- 2:07wave here. The regions of compression
- 2:10have high localized pressures, and the
- 2:12regions of rarefaction have low
- 2:14localized pressures, and we can plot
- 2:16these with the x-axis being the normal
- 2:19pressure within the tissue. Now, in
- 2:21practice, the amplitude of compression
- 2:24is actually higher than the amplitude of
- 2:26rarefaction, but for practical purposes,
- 2:28we will represent a sound wave like this
- 2:30within the talks, and you'll see that in
- 2:32textbooks as well.
- 2:33Now, the energy here is transferring
- 2:35from left to right, but the molecules
- 2:37are not moving all the way across. They
- 2:40are staying in the same place
- 2:41oscillating back and forth. When I'm
- 2:43speaking to someone, the air molecules
- 2:45leaving my mouth is not the same air
- 2:47that is reaching someone's eardrum
- 2:49there. The energy has passed through.
- 2:51It's not the molecules going all the way
- 2:53through. It's a transfer of energy.
- 2:55Now, when we look at these waves, as
- 2:57with electromagnetic radiation, as with
- 2:58any wave, we can define some properties
- 3:01of that wave. The first being
- 3:02wavelength. The distance between
- 3:05successive regions on a wave. So, from
- 3:07one region of compression to the next
- 3:10region of compression, or one region of
- 3:12rarefaction to the next region of
- 3:13rarefaction, that distance there is the
- 3:17wavelength.
- 3:18The next thing we can look at is the
- 3:19frequency of the wave. How many cycles
- 3:22of that wave pass a particular point in
- 3:25a given period of time, and we measure
- 3:26frequency in hertz. 1 hertz is one wave
- 3:30passing a point in 1 second.
- 3:33Now, as we looked at when we looked at
- 3:35electromagnetic radiation, we can
- 3:37calculate the speed of the wave by
- 3:39looking at the product of the frequency
- 3:41and the wavelength of that wave.
- 3:43Now, as you see throughout this
- 3:45ultrasound physics module, we are going
- 3:46to be looking at a lot of formulas. And
- 3:48without context to to formulas, we can
- 3:50go about misinterpreting these formulas.
- 3:53When we looked at electromagnetic
- 3:55radiation, electromagnetic radiation
- 3:57traveled at a constant speed. It
- 3:59traveled at the speed of light. No
- 4:01matter if it was x-rays or radio waves,
- 4:03the speed stayed constant. When we're
- 4:05looking at sound, this is not the case.
- 4:07The speed of a sound wave is purely
- 4:09determined by the medium through which
- 4:12it is traveling. We cannot control the
- 4:14speed of a sound wave, but it changes as
- 4:17it goes through different mediums. What
- 4:19we can control is the frequency of the
- 4:22wave.
- 4:23When we are speaking, we set the
- 4:24frequency with our vocal cords. When we
- 4:26are using an ultrasound transducer, we
- 4:29set the frequency of that wave.
- 4:31Now, independent of that frequency, the
- 4:33sound wave will travel at a set speed
- 4:36depending on the material it is
- 4:37traveling through. And the wavelength
- 4:39will be the compensatory mechanism to
- 4:42link that frequency and that speed.
- 4:44Speed and frequency in sound are
- 4:46completely independent of one another.
- 4:48And don't worry, we're going to be going
- 4:49through this in some depth in the
- 4:51following talks.
- 4:52Now, when we are looking at
- 4:53electromagnetic radiation and the
- 4:55acoustic spectrum, there are some subtle
- 4:57differences. And these subtle
- 4:59differences make marked differences when
- 5:01we're looking at how these waves
- 5:02interact with tissue. And from what I've
- 5:04seen with the types of question that
- 5:06gets asked in exams, they're trying to
- 5:08test, do you understand the unique
- 5:10properties of sound and how they differ
- 5:12from electromagnetic radiation? And a
- 5:14lot of people get tripped up by not
- 5:16understanding these differences.
- 5:18So, when we looked at the
- 5:18electromagnetic spectrum, we divided it
- 5:20up multiple different sections. And we
- 5:23classify these sections by the
- 5:25wavelength of the wave. We could do that
- 5:28in electromagnetic radiation because
- 5:30speed stayed constant. So, our
- 5:32wavelength acted as a proxy for
- 5:34frequency. And when we looked at the
- 5:36energy of a wave, the frequency
- 5:38determined the energy of that wave.
- 5:41Now, sound waves are a little bit
- 5:42different. We set the frequency of the
- 5:45wave, and the speed of that wave is
- 5:47dependent on the material it travels
- 5:49through.
- 5:50Now, depending on the material, the
- 5:52wavelength will change. We don't have a
- 5:54tight link between wavelength and
- 5:56frequency if the material is changing,
- 5:59like we had in electromagnetic
- 6:00radiation.
- 6:01So, depending on the frequency and
- 6:03depending on the medium through which
- 6:05it's traveling, our wavelength will
- 6:07change. We can't use wavelength to
- 6:09subcategorize the acoustic spectrum.
- 6:12So, we use frequency. That is what we
- 6:14said. That's the variable that we have
- 6:16control over. Now, audible sound is
- 6:18between the region of 20 hertz and 20
- 6:21kilohertz, 20,000 hertz. So, 20 cycles
- 6:25of a wave passing a point in 1 second to
- 6:2820,000 cycles of a wave passing a point
- 6:31in a second. Anything with a frequency
- 6:33lower than that is known as infrasound.
- 6:35We can't hear the sound.
- 6:38Frequencies higher than that is called
- 6:40ultrasound. Anything over 20,000 hertz
- 6:43is known as ultrasound. We can't hear
- 6:45these frequencies. Now, diagnostic
- 6:48ultrasound is between 2 and 20
- 6:50megahertz, 2 and 20 million hertz, 2 and
- 6:5420 million cycles going past a
- 6:56particular point in 1 second. We are
- 6:59dealing with really high frequency waves
- 7:01here, and that's an important point to
- 7:02remember.
- 7:03Now, we can represent electromagnetic
- 7:05waves and sound waves graphically. We've
- 7:07seen this here if you've done the x-ray
- 7:09module. An electromagnetic wave is a
- 7:11transverse wave, orthogonal waves that
- 7:14self-propagate through space.
- 7:16They can travel in a vacuum. They don't
- 7:18need a medium. The movement of the
- 7:20electric wave and the movement of the
- 7:22magnetic wave self-propagate one
- 7:24another. They have a constant velocity,
- 7:27no matter the frequency or the
- 7:28wavelength, the velocity of that wave is
- 7:30exactly the same, and the energy being
- 7:33transferred through time and space is
- 7:34the electromagnetic energy. Now, when we
- 7:37look at a sound wave, it's known as a
- 7:38longitudinal wave. The movement of the
- 7:41units within that medium happen in the
- 7:43same direction as the movement of energy
- 7:45within that medium. These units
- 7:48oscillate in this direction, parallel to
- 7:51the movement of energy, unlike our
- 7:53electromagnetic wave where the
- 7:54oscillation of the energy happen in a
- 7:57perpendicular fashion to the movement of
- 7:59energy in that wave.
- 8:01Now, as we've said, sound waves require
- 8:03a medium to travel in that medium needs
- 8:05to be continuous and elastic. And
- 8:07depending on that medium, depending on
- 8:09various properties of that medium, the
- 8:11speed of that sound wave will change and
- 8:14the wavelength will change accordingly.
- 8:16The frequency will not change. If we set
- 8:19a frequency of an ultrasound probe, the
- 8:21speed of that sound will change as it
- 8:22goes through various tissues, but the
- 8:24frequency will remain the same. Here,
- 8:26our frequency is constant. In
- 8:28electromagnetic radiation, our speed was
- 8:30constant. And the last is that energy
- 8:32transferring through is a mechanical
- 8:34energy. It requires a mechanical force
- 8:37to propagate that wave, to move energy
- 8:40through the medium. Now, I've spent some
- 8:42time discussing this concept and I
- 8:43really want you to have a good
- 8:45understanding of what acoustic waves are
- 8:47and what they aren't. Cuz when we look
- 8:49at more complex topics in future talks,
- 8:51if you don't have this core basic
- 8:53fundamental knowledge, you're going to
- 8:54fall short when it comes to those more
- 8:56complicated calculations. So, in our
- 8:58next talk, we're going to have a closer
- 8:59look at the wavelength, frequency,
- 9:01period, and speed of waves as they
- 9:04travel through a medium. So, I'll see
- 9:05you all there. Goodbye, everybody.
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