Sono Physics Ch.6-7

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Interactions of Sound and Media

Last updated 4:39 AM on 7/11/26
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30 Terms

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What is Attenuation?

The gradual weakening of a sound wave as it travels through tissue.

Decibel Notation (dBdB)

ā—¦ Measure a change in signal strength

ā—¦ Based on a logarithmic scale

ā—¦ Compare a starting value to a final value

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Why dB uses Logs?

Because ultrasound Intensity changes over extremely large ranges.

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What are Decibels - dB?

Measures how much a beam’s strength changes as it travels through the body.

Compares 2 Intensity Levels:

ā—¦ Original intensity (before)

ā—¦ New intensity (after)

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Common dB Values:

+3dB = Intensity x 2

-3dB = Intensity/ 2

+10dB = I x 10

-10dB = I / 10

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Decibels Measured as a Ratio

Ratio = New Intensity / Original Intensity

Ex: 100 → 10

Intensity decreased by a factor of 10

So, Change = -10dB Decibels measures a difference, not an actual Value

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Components of Attenuation:

Reflection, Scattering and Absorption

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What are two factors that Increase Attenuation?

-Distance (Path Length)

-Frequency

Higher Frequency = Greater Attenuation

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Frequency

Higher Frequency = Greater Attenuation

Lower frequency = less attenuation and deeper penetration

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Reflection

Occurs when sound encounters a boundary between two tissues

ā—¦ Part of the sound wave returns to the transducer

ā—¦ Reflection is the most important component of Attenuation because it creates the echoes used to form an image

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<p>Specular Reflection </p>

Specular Reflection

Occurs at smooth, flat boundaries

ā—¦ Vessel walls

ā—¦ Diaphragm

ā—¦ Organ capsules

Echoes return in a single organized direction

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Limitations of Specular Reflection

ā—¦ Requires the beam to strike surface nearly perpendicular

ā—¦ If beam is off-axis, echo may miss transducer

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<p>Diffuse Reflection (Back Scatter) </p>

Diffuse Reflection (Back Scatter)

Occurs when sound strikes an irregular surface

ā—¦ Echoes are scattered in many directions

ā—¦ Most Images are created from Backscatter

Advantage:

ā—¦ Produces echoes even when the beam is not perpendicular

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Limitation of Diffuse Reflection (Backscatter):

Weaker echoes than specular reflection

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<p>Scattering</p>

Scattering

Occurs when the reflecting surface is very small

ā—¦Sound waves are redirected in many directions

ā—¦About the same size or smaller than the sound's wavelength

ā—¦Lung tissue scatters sound strongly because of the many tiny air-filled alveoli.

ā—¦Higher frequency sound scatters more than lower frequency sound

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Scattering Relationship with Frequency is what?

Directly Related

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<p>Rayleigh Scattering </p>

Rayleigh Scattering

Occurs when scatterer is much smaller than wavelength

ā—¦ Sound is scattered equally in all directions

ā—¦ Omnidirectional scattering

Ex: Red Blood Cells

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Rayleigh Scattering Relationship with Frequency is what?

Inversely Proportional

Rayleigh Scattering āˆ Frequency⁓

ā—¦ If frequency doubles:

2⁓ = 16

ā—¦ Scattering increases 16-fold

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Absorption

Occurs when sound energy is converted into another form of energy

ā—¦ Most commonly converted into heat

Important Facts:

ā—¦ Bone absorbs more sound than any other tissue

ā—¦ Absorption is directly related to frequency

ā—¦ Absorption is the largest contributor to attenuation

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Absorption Relationship with Frequency is what?

Directly Related

Higher Frequency → More Absorption

Lower Frequency → Less Absorption

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Attenuation Coefficient

The amount of sound energy lost per centimeter traveled

Units: dB/cm

In Soft Tissue:

Attenuation Coefficient Formula:

ā‰ˆ Frequency Ć· 2

or 0.5 dB/cm/MHz

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Attenuation Coefficient Relationship with Frequency is what?

Directly Related

Higher Frequency → Higher Attenuation per cm

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<p>Attenuation Coefficient Example </p>

Attenuation Coefficient Example

12 Mhz Ć· 2 = 6 dB/cm

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Total Attenuation Formula

Total Attenuation (dB) = Attenuation Coefficient (dB/cm) x distance (cm

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Half-Value Layer Thickness (HVL)

The distance sound travels before its intensity is reduced by 50%

ā—¦ 50% intensity loss = 3 dB decrease

Units:

ā—¦Cm

ā—¦ Any unit of length

Also Known As:

ā—¦ Penetration Depth

ā—¦ Depth of Penetration

ā—¦ Half-Boundary Layer

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<p>Thin Half-Value Layer: </p>

Thin Half-Value Layer:

More Attenuation

ā—¦High-frequency sound

ā—¦Highly attenuating media

ā—¦Bone

ā—¦Lung

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<p>Thick Half-Value Layer: </p>

Thick Half-Value Layer:

Less Attenuation

ā—¦Low-frequency sound

ā—¦Low-attenuating media

ā—¦Water

ā—¦Fluids

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Acoustic Impedance

Resistance a medium offers to the transmission of sound.

Key Facts:

Symbol = Z

Measured in Rayls (MRayls)

ā—¦ Calculated, not directly measured

Typical Values in Soft Tissue = 1.25 – 1.75 MRayls

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Impedance Formula

Z = Density Ɨ Propagation Speed

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Tissue Impedance

ā—¦ Dense tissues resist sound more

ā—¦ Stiff tissues transmit sound faster & have higher impedance

Tissue Impedance is measured not calculated

Higher Density + Higher Speed = Higher Impedance

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<p>Why is Impedance Important? </p>

Why is Impedance Important?

Reflection occurs when sound encounters a boundary between tissues with different impedances.

Small Difference:

ā—¦ Little reflection

ā—¦ Most sound transmitted

Large Difference:

ā—¦ Strong reflection

ā—¦ Less transmission