Physics basic

325
PROF.DR SYED AMIR GILANI PROF.DR SYED AMIR GILANI

description

 

Transcript of Physics basic

Page 1: Physics basic

PROF.DR SYED AMIR GILANIPROF.DR SYED AMIR GILANI

Page 2: Physics basic
Page 3: Physics basic
Page 4: Physics basic
Page 5: Physics basic
Page 6: Physics basic
Page 7: Physics basic
Page 8: Physics basic
Page 9: Physics basic
Page 10: Physics basic

Basic UltrasoundBasic UltrasoundPhysicsPhysics

InstrumentationInstrumentation

Prof.Dr.Syed Amir GilaniProf.Dr.Syed Amir Gilani

Page 11: Physics basic

UltrasoundUltrasound

Page 12: Physics basic

UltrasoundUltrasound

The use of high frequency (inaudible) sound togenerate images

Page 13: Physics basic

UltrasoundUltrasound

The use of high frequency (inaudible) sound togenerate images

Ultrasound images are Tomographic, Real-time and in Grey scale

Page 14: Physics basic

Tomographic Images in sections or slices,

as in CT, MR, SPECT etc

Page 15: Physics basic

Tomographic Images in sections or slices,

as in CT, MR, SPECT etc

Real-time Physiological movements

within body are depicted

as such

Page 16: Physics basic

Tomographic Images in sections or slices,

as in CT, MR, SPECT etc

Real-time Physiological movements

within body are depicted

as such

Grey Scale Number of grey shades

between absolute white and

absolute black

Page 17: Physics basic

Mechanical energy producing alternating compression and rarefaction

Sound waves are Longitudinal waves unlike electromagnetic waves

SoundSound

Page 18: Physics basic

The audible frequency ranges from 20 Hz– 20 kHz. Ultrasound frequency is in the MHz range.

Mechanical energy producing alternating compression and rarefaction

Sound waves are Longitudinal waves unlike electromagnetic waves

SoundSound

Page 19: Physics basic

T

Time

Pre

ssur

eThe Sound WaveThe Sound Wave

Page 20: Physics basic

SOUND BEAMS & DISPLAY MODES

Page 21: Physics basic

Beam widthBeam width o As sound travels, the width of the beam changes:

o Starts out at exactly the same size as the transducer diameter,

o Gets progressively narrower until it reaches its smallest diameter, and then

o It diverges

Page 22: Physics basic

FocusFocus

o The location where the sound beam reaches its minimum diameter.

Page 23: Physics basic

Focal DepthFocal Depth

o The distance from the transducer face to the focus. Also called focal length or near zone length.

Page 24: Physics basic

Near ZoneNear Zone

o The region or zone in between the transducer and the focus.

Page 25: Physics basic

(Fresnel Zone)(Fresnel Zone)

o The beam converges in the near zone

Page 26: Physics basic

Far ZoneFar Zone

o The region or zone beyond the near field. The beam

o (Fraunhofer Zone) diverges in the far zone.

Near zone - short name - Fresnel

Far zone - long name - Fraunhofer

Page 27: Physics basic

Focal ZoneFocal Zone

o The region surrounding the focus where the beam is "sort of narrow" and the picture is relatively good.

Page 28: Physics basic

Note Note

o For an unfocused continuous wave disc transducer:

o At the end of the near zone, the beam diameter is ½ the transducer diameter.

o At two near zone lengths, the beam diameter is equal to the transducer diameter.

Page 29: Physics basic

Focal DepthFocal Depth

o Definition

o Distance from transducer to the narrowest part of the beam (the focus)

Page 30: Physics basic

Determined by two factorsDetermined by two factors

o 1. Transducer diameter and

o 2. Frequency of the ultrasound.

Page 31: Physics basic

Sound Beam DivergenceSound Beam Divergence

o Definition

o Describes the spread of the sound beam in the deep far zone. Determined by two factors:

o 1. The transducer diameter and

o 2. The frequency of the ultrasound,

Page 32: Physics basic

o Larger diameter crystals producing higher frequency sound produce beams that diverge less in the far field.

o Smaller diameter crystals producing lower frequency sound produce beams that diverge substantially in the far field.

Page 33: Physics basic

DiffractionDiffractiono Diffraction Pattern o a V-shaped wave, also called a Huygen's wavelet.

When produced by a tiny source, with a size near the wavelength of the sound, waves will diverge in this shape as they propagate. If sound waves produced by imaging transducers acted in this manner, the wave would be spread broadly as it travels.

Page 34: Physics basic

Huygen's PrincipleHuygen's Principle

•Definition

•Sound waves produced by imaging transducers are shaped like an hourglass and do not diffract because they obey Huygen's principle. Each tiny part of the surface of the large transducer face may be considered an individual sound source. The hourglass shape of a sound beam is the result of the constructive and destructive interference of the many sound wavelets emitted from these numerous sound sources.

Page 35: Physics basic

Lateral Resolution Lateral Resolution

o It has been found that when all of these multiple wavelets are combined according to Huygen's Principle, they produce an hourglass-shaped main sound beam. This principle explains the shape of an imaging transducer's sound beam.

Page 36: Physics basic

DefinitionDefinition

o The minimum distance that two structures are separated by side-to-side or perpendicular to the sound beam that produces two distinct echoes.

Page 37: Physics basic

SynonymsSynonyms

Lateral Angular Transverse Azimuthal

o LATA resolution.

Page 38: Physics basic

UnitsUnits

o mm, all units of length

o smaller number, more accurate image

Page 39: Physics basic

High Frequency Pulsed UltrasoundHigh Frequency Pulsed Ultrasound

o Special notes for pulses made of high frequencies:

o Beam Shape & Divergence—pulses of sound at higher frequencies tend to have less divergence in the far field. Higher frequency pulsed US has narrower beams compared to lower frequencies.

Page 40: Physics basic

FocusingFocusing

o Results in:

o 1. A narrower "waist" in the US beam.

o 2. A decrease in focal depth (the focus is shallower).

o 3. A reduction in the size of the focal zone. Effective mainly in the near field and the focal zone.

Page 41: Physics basic

Three Modes of FocusingThree Modes of Focusing

o 1. Lens - external focusing (fixed, mechanical or conventional)

Page 42: Physics basic

2. Curved Piezoelectric2. Curved Piezoelectric

o Crystal-internal focusing, (fixed, mechanical or conventional)

Page 43: Physics basic

o A lens or curvature of the crystal can focus a wave produced by a single PZT crystal. This is conventional,

o fixed, or mechanical focusing. The focal depth using either

o of these two methods cannot be changed.

Page 44: Physics basic

3. Electronic Focusing3. Electronic Focusing

o Phased array technology provides dynamic, variable (adjustable) focusing or multi-focusing.

Page 45: Physics basic

Single crystal transducers are always Single crystal transducers are always fixed focus.fixed focus.

o Phased array transducers generally have "better" lateral resolution because the focus is adjustable by the sonographer.

Page 46: Physics basic

o With phased arrays, the sonographer can locate the focus within the anatomic region of clinical importance.

o The greater the extent of focusing, the smaller the focal zone.

Page 47: Physics basic

Summary—Sound Beam AnatomySummary—Sound Beam Anatomy

CharacteristicCharacteristic DeterminantsDeterminantsFrequency (CW)Frequency (CW) Electronic frequency :Electronic frequency :

Frequency (Pulsed)Frequency (Pulsed) Thickness of ceramic & Speed of Thickness of ceramic & Speed of sound in ceramicsound in ceramic

Focal lengthFocal length Diameter of ceramic & Frequency Diameter of ceramic & Frequency of sound Diameter of sound Diameter

DivergenceDivergence Diameter of ceramic & Frequency Diameter of ceramic & Frequency of soundof sound

Lateral resolution Lateral resolution Beam width Beam width

Page 48: Physics basic

Graph AxesGraph Axes

Page 49: Physics basic

Display ModesDisplay Modeso A-Mode o Amplitude o Mode—When the US pulse is emitted, a dot

moves across the screen of an US machine at a constant speed. When the echo returns, an upward deflection proportional to the amplitude of the returning echo is observed. A-mode provides very precise measurements of distances between the probe and the reflector.

o Looks like a big-city skyline.

Page 50: Physics basic

o X-axis - reflector depth,

o measured by pulse's time-of-flighty

o Y-axis - amplitude of echo,

o measured by echo strength

Page 51: Physics basic

B-ModeB-Mode

o Brightness Mode—Returning echoes are presented as spots on the line of travel of the emitted US pulse. The stronger the returning echo, the brighter the spot. The brightness of the dot is proportional to the strength of the returning echo.

Page 52: Physics basic

o X-axis - depth of reflector

o measured by pulse's time-of-flight

o Z-axis - amplitude of echoes

o measured by echo strength

Page 53: Physics basic

M-ModeM-Mode

o Motion Mode or T-M mode Dragging a photosensitive across a B-mode produces squiggly lines. These lines represent the motion of the reflecting body surfaces as they occur in time. Not related to echo amplitude, related to location. displays the changing position of Mime reflectors with respect to time.

Page 54: Physics basic

••X-axis -X-axis - time time•Y-axis -•Y-axis - depth, measured by pulse's time-of- depth, measured by pulse's time-of-flightflight

Page 55: Physics basic

PULSED ECHO PULSED ECHO INSTRUMENTATION INSTRUMENTATION

Page 56: Physics basic

Information Information

o Time of flight

o Strength

Page 57: Physics basic

Ultrasound SystemUltrasound System

o The entire device that produces US beams, retrieves the echoes and produces visual images and audio signals.

o System Components

o Six interconnected components - information is transferred to and from each.

Page 58: Physics basic

Master SynchronizerMaster Synchronizer

o Communicates with all of the individual components of the ultrasound system.

o Organizes and times their functions.

o Prepares them to operate as a single integrated system.

Page 59: Physics basic

TransducerTransducer

o Converts electrical into acoustic energy during transmission

o Converts returning acoustic into electrical energy during reception.

Page 60: Physics basic

PulserPulser

o The component that controls the electrical signals sent to the transducer for sound pulse generation.

o Determines the PRF, pulse amplitude, and pulse repetition period.

o Creates the firing pattern for phased array systems. This is called the 'beam former.

Page 61: Physics basic

ReceiverReceiver

o The electronics associated with processing the electronic signal produced by the transducer during reception and producing a picture on an appropriate display.

Page 62: Physics basic

DisplayDisplay

o The device associated with the presentation of processed data for interpretation.

o CRT (television), audio speakers, a paper record.

Page 63: Physics basic

StorageStorage

o Any number of devices and "media" that are used to permanently archive the US data

o Video tape, paper, film, transparent film, computer discs.

Page 64: Physics basic

PulserPulser

o Function

o Receives timing signal from synchronizer

o Creates an electrical signal that will excite the PZT crystal.

o Produces electrical voltage, 10 - 500 volts, that excites piezoelectric crystal during transmission.

Page 65: Physics basic

o Greater electrical voltage increases sound intensity created by the transducer and sent into the patient.

o Pulser signals depend upon system and transducer.

o Do not" use a transducer with a crack in the housing because of the potential for electrical shock to the patient.

Page 66: Physics basic

Pulser ModesPulser Modeso Continuous Wave:o Constant electrical signal in the form of a sine wave,

electrical frequency = US frequency.o Pulsed Wave,o Short duration electrical "spike", one electrical spike per.o Single Crystal: ultrasound pulse.o Pulsed Wave, Many elements fired for each ultrasound

pulse.

Page 67: Physics basic

ArraysArrays

o Thus, for each sound pulse, many short duration electrical "spikes" are required—one electrical spike per fired element. ^ For phased array systems, the pulser is also called the 'beam former."

Page 68: Physics basic

Transducer OutputTransducer Output

o Synonyms: output gain, acoustic power, pulser power, energy output transmitter output.

Page 69: Physics basic

o Changes in transducer output affect the brightness of the entire image.

o Determined by the excitation voltage from the pulser.

o Piezoelectric crystal vibrates with a magnitude related to pulser voltage.

Page 70: Physics basic

Adjusted by sonographerAdjusted by sonographer

oYes

Page 71: Physics basic

Effect upon imageEffect upon image

o When transducer output changes, every pulse transmitted to the body changes.

o All reflections from structures in the body also change. The brightness of the entire image changes

Page 72: Physics basic
Page 73: Physics basic

Note:Note:

o Increasing transducer output improves improves signal – to- nose ratio.

o The meaningful signal strength is altered, while the noise level remains constant.

Page 74: Physics basic

Receiver and Its FunctionsReceiver and Its Functions

o Overall Function:

o The signals returning from the transducer are extremely weak. The receiver boosts the strength of these signals, processes them and prepares them for display.

Page 75: Physics basic

OrderOrder

o Amplification, compensation, compression, demodulation, rejection (hint: alphabetical order).

Page 76: Physics basic

AmplificationAmplification

o Purpose:

o Increasing the strength of all electrical signals in the receiver prior to further processing.

o Synonyms:

o receiver gain

Page 77: Physics basic

PreamplifierPreamplifier

o Preamplifier may condition signal before it is amplified, often performed in the probe.

Page 78: Physics basic
Page 79: Physics basic

CompensationCompensation

o Purpose:

o Used to create image of uniform brightness from top to bottom,

o Since attenuation is strongly related to path length, echoes returning from great depths have lower amplitudes than those returning from shallow depths.

Page 80: Physics basic

Effect upon imageEffect upon image

o Compensation makes all echoes from similar reflectors appear identical regardless of their depth.

Page 81: Physics basic

SynonymsSynonyms

o Time gain compensation (TGC), depth compensation (DGC), swept gain.

Page 82: Physics basic

IMPROPER TGC IMPROPER TGC

Page 83: Physics basic

NoteNote

o Compensation makes an image equally bright at all depths. Ask the question "Is the image of uniform brightness from the top to the bottom?"

Page 84: Physics basic

TGC & FrequencyTGC & Frequency

o Adjustments to TGC are related to transducer frequency:

o • With a higher frequency transducer the beam undergoes more attenuation. Therefore, more TGC must be used. On the diagram, the TGC curve is shifted upward & to the right.

Page 85: Physics basic

TGC & FrequencyTGC & Frequency

o • With a lower frequency transducer, the beam undergoes less attenuation. Therefore, less TGC is needed. On the diagram, the TGC curve is shifted downward and to the left.

Page 86: Physics basic

TQC CURVETQC CURVE ADJUSTING TGCADJUSTING TGC

Page 87: Physics basic

CompressionCompression

o Reducing the total range, the smallest to the largest signal.

Page 88: Physics basic

PurposePurpose

o Keeps signals within the operating range of the system's electronics and the gray scale within the range of what the human eye can see.

o • Done without altering the relative relationships between voltages; largest stays largest, smallest remains smallest.

o • Decreases the dynamic range of the signals,

Page 89: Physics basic

Effect upon imageEffect upon image

o Changes the gray scale mapping.

Page 90: Physics basic

DemodulationDemodulation

o Purpose

o Changes the signal's form to one more suitable for TV display.

Page 91: Physics basic

Adjusted by sonographerAdjusted by sonographer

o No. Fixed by the manufacturer. Has two steps:

Page 92: Physics basic

1. Rectification1. Rectification

o Turning all of the negative voltages into positive ones. Corrects for or eliminates negative voltages.

Page 93: Physics basic

2. Smoothing (or Enveloping)2. Smoothing (or Enveloping)

o Putting an envelope around the "bumps" to even them out.

Page 94: Physics basic

RejectionRejection

o Purpose:

o Displays low level echoes only when clinically meaningful.

Page 95: Physics basic

SynonymsSynonyms

o Suppression, threshold

o Very low level echoes may or may not be important. Reject determines whether they appear on the image.

o Effect upon image Affects all low level signals everywhere on the image,

o but does not affect bright echoes.

Page 96: Physics basic
Page 97: Physics basic

Order of Receiver OperationsOrder of Receiver Operations

o These five operations must be performed in the appropriate order for proper system function. Alphabetical order:

o 1. Amplification

o 2. Compensation

o 3. Compression

o 4. Demodulation

o 5. Reject

Page 98: Physics basic

Summary—Receiver FunctionsSummary—Receiver Functions

FunctionFunction Adjustable?Adjustable? Signals ProcessedSignals Processed

AmplificationAmplification Yes Yes All signals treated the same All signals treated the same

CompensationCompensation Yes Yes Signals treated differently Signals treated differently based on reflector depth based on reflector depth

Compression Compression Yes Yes Decreases dynamic range, Decreases dynamic range, changes gray scale map changes gray scale map

DemodulationDemodulation NoNo Changes form of signals Changes form of signals

RejectionRejection Yes Yes All weak signals manipulated All weak signals manipulated Strong signals not affected. Strong signals not affected.

Page 99: Physics basic

Dynamic Frequency TuningDynamic Frequency Tuning

o Pulses contain a wide range of frequencies (wide bandwidth).

o On some US systems, higher frequencies create shallow parts of the image and lower frequencies create deeper parts.

Page 100: Physics basic

o Eechoes arising from superficial structures are filtered to process only higher frequencies, since higher frequencies make better images.

o Lower frequency signals are used to image deeper structures, since the higher frequencies have attenuated and are no longer present.

Page 101: Physics basic

Harmonic ImagingHarmonic Imaging

Page 102: Physics basic

DefinitionDefinition

o Transmitting sound at a particular frequency (called the fundamental frequency), but creating an image from sound reflected at twice the fundamental frequency (called the harmonic or second harmonic).

Page 103: Physics basic

Fundamental frequencyFundamental frequency

o The frequency of the transmitted sound wave

Page 104: Physics basic

Harmonic frequencyHarmonic frequency

o Twice the transmitted frequency. Also called the second harmonic.

Page 105: Physics basic

ExampleExample

o A transducer transmits a sound pulse with a fundamental frequency of 2 MHz. In the harmonic mode, an image created from 4MHz sound reflections will be displayed.

Page 106: Physics basic

o As a sound wave travels in the body, a miniscule amount of energy is converted from the fundamental frequency to the harmonic frequency due to non-linear behavior.

Page 107: Physics basic

Contrast AgentsContrast Agents

o Also called "micro-bubbles" of gas entrapped in a shell.

o Contrast agents have a different acoustic fingerprint than blood or tissue.

Page 108: Physics basic

Contrast AgentsContrast Agents

o Injected into the circulation (usually intravenously). These agents create strong reflections that actually "light up" blood chambers or vessels.

o Currently indicated only for determining the borders of the left ventricle of the heart.

Page 109: Physics basic

Requirements Requirements

o • Safe

o • Long persistence

o • Metabolically inert

o • So small as to pass through capillaries

o • Strong reflector of ultrasound

Page 110: Physics basic

without contrast with contrast

Page 111: Physics basic

Output Power vs. Receiver GainOutput Power vs. Receiver Gain

o Adjustments to either output power or receiver gain change the brightness of the entire image.

Page 112: Physics basic

Output PowerOutput Power

o Affects brightness by adjusting the strength of the sound pulse sent to the body by the transducer.

o When the pulse is more powerful, all of the returning echoes from the body are stronger, and the image is brighter.

o When the image is too bright due to high output power, the lateral and longitudinal resolution degrade.

Page 113: Physics basic

Receiver GainReceiver Gain

o Affects the brightness by changing the amplification of the electronic signals after returning to the receiver.

o When amplification is increased, the electronic signals in the receiver are boosted, and the image will be brighter.

Page 114: Physics basic

Which one?Which one?

o To determine whether a control affects output power or receiver gain, look at the its description. When the term suggests "outgoing" the function is probably output power. When the word indicates "reception or incoming" the function is most likely receiver gain.

Page 115: Physics basic

ALARAALARA

o When an entire image is either too bright or too dark, changes in output power or receiver gain may correct the problem. As a first option, always choose the option that will minimize patient exposure.

Page 116: Physics basic

Use the ALARA Principle – As Low As Use the ALARA Principle – As Low As Reasonable Achievable Reasonable Achievable

Image too dark—first, image too bright—first, reduce increase receiver gain

Page 117: Physics basic

INTERACTION OF INTERACTION OF SOUND AND MEDIA SOUND AND MEDIA

Page 118: Physics basic

AttenuationAttenuationo Definition

o The decrease in intensity, power and amplitude of a sound wave as it travels.

o The farther US travels, the more attenuation occurs.

Page 119: Physics basic

UnitsUnits

o dB, decibels (must be negative, since the attenuation causes intensity to decrease)

Page 120: Physics basic

In soft tissueIn soft tissue

o Attenuation of sound in soft tissue depends upon the wave's 1) frequency and the 2) distance the wave travels.

o In soft tissue, higher frequency results in greater attenuation. Thus we can image deeper with lower frequency sound.

Page 121: Physics basic

NoteNote

o Attenuation is unrelated to propagation speed.

Page 122: Physics basic

Three ComponentsThree Components

o 1. Absorption (sound energy converted into heat energy)

o 2. Scattering

o 3. Reflection

Page 123: Physics basic

Media Media

o Air—much, much more attenuation than in soft tissue vo Bone—more than soft tissue, absorption & reflection y|/o Lung—more than soft tissue, due to scattering vo Water—much, much less than soft tissue yo Air >> Bone & Lung > Soft Tissue » Water

Page 124: Physics basic

Reflection and ScatteringReflection and Scattering

Page 125: Physics basic

ReflectionReflection

o Occurs when propagating sound energy strikes a boundary between two media and some returns to the transducer.

Page 126: Physics basic

Specular ReflectionSpecular Reflection

o Reflections from a very smooth reflector (mirror) are Specular

o Specular reflections also occur when the wavelength is much smaller than the irregularities in the boundary.

Page 127: Physics basic

ScatteringScattering

o If the boundary between two media has irregularities (with a size similar to or a bit smaller than the pulse's wavelength), then the wave may be chaotically redirected in all directions.

Page 128: Physics basic

Rayleigh ScatteringRayleigh Scattering

Page 129: Physics basic

o If a reflector is much smaller than the wavelength of sound, the sound is uniformly diverted in all directions. Higher frequency sound undergoes more Rayleigh scattering. A red blood cell is a Rayleigh scatterer.

o Rayleigh scattering is related to frequency

Page 130: Physics basic

Attenuation & ImagingAttenuation & Imaging DepthDepth

o Attenuation ultimately limits the maximum depth from which images are obtained. The goal in diagnostic imaging is to use the highest frequency that still allows us to image to the depth of the structures of clinical interest. That is why we use 2-l0Mhz sound waves.

Page 131: Physics basic

OrganizedOrganized

systematicsystematic

DisorganizedDisorganized

chaoticchaotic

ReflectionReflection

(back to Transducer)(back to Transducer)

SpecularSpecular DiffuseDiffuse

ScatteringScattering

(in all directions)(in all directions)

RayleighRayleigh ScatterScatter

Page 132: Physics basic

Attenuation CoefficientAttenuation Coefficient

o Definition The amount of attenuation per centimeter.

Page 133: Physics basic

UnitsUnits

o dB/cm, decibels per centimeter.

o In soft tissue

o • With higher frequency, the attenuation coefficient increases.

o • This is why lower frequencies are used to image to greater depths.

o As the frequency of a wave increases, attenuation coefficient increases.

Page 134: Physics basic

In soft tissueIn soft tissue

o In soft tissue, attenuation coefficient (dB/cm) is approx. half of the frequency (MHz), or 0.5dB/cm/MHz.

o Hint Attenuation coefficient is related to frequency.

Page 135: Physics basic

EquationEquation

o total attenuation (dB) = path length (cm) x attenuation coefficient (dB/cm)

Page 136: Physics basic

ImpedanceImpedance

o Characteristic of the medium only.

o Impedance is not measured, it is calculated,

Page 137: Physics basic

UnitsUnits

o Rayls, often represented by the letter "Z"

Page 138: Physics basic

Typical ValuesTypical Values

o Between 1,250,000 and l,750,000rayls (1.25 - 1.75Mrayls)

o Reflection of an ultrasound wave depends upon a difference In the acoustic impedances at the boundary between the two media.

Page 139: Physics basic

Oblique IncidenceOblique Incidence

o Anything other than 90 degrees; not at right angles,

Page 140: Physics basic

Reflection and TransmissionReflection and Transmission

o Incident Intensity

o The intensity of the sound wave at the instant prior to striking a boundary.

Page 141: Physics basic

Reflected IntensityReflected Intensity

o The portion of the incident intensity that, after striking a

o boundary, changes direction and returns back from where it came.

Page 142: Physics basic

Transmitted IntensityTransmitted Intensity

o The portion of the incident intensity that, after striking a boundary, continues on in the same general direction that it was originally traveling.

Page 143: Physics basic

At the boundary between two mediaAt the boundary between two media

o 1. When IRC and ITC are added, the result is l00%g

o 2. When reflected and transmitted intensities are added, the result is the incident intensity.

Page 144: Physics basic

o There is "conservation of energy" at a boundary.

Page 145: Physics basic

In soft tissueIn soft tissue

Typically, only 1% or less of the incident US energy is reflected at a soft-tissue boundary between different biologic media (such as blood and muscle).

99% is reflected at an air-tissue interface \y 50% at a bone-tissue interface^.

Thus, there is a great deal of attenuation at an air-tissue interface or a bone-tissue interface.

Page 146: Physics basic

Transmission With Normal IncidenceTransmission With Normal Incidence

o With NORMAL incidence:

o These are simply reflection questions, whatever remains after transmission, must be reflected!

Page 147: Physics basic

o Incident Intensity = Reflected Intensity + Transmitted Intensity

o Transmitted Intensity = Incident Intensity x Intensity Transmission Coefficient

Page 148: Physics basic

Reflection & Transmission With Reflection & Transmission With Oblique IncidenceOblique Incidence

o Extremely complex physics regarding transmission & reflection with obliquity.

Page 149: Physics basic

RememberRemembero With oblique incidence, we are uncertain as to

whether reflection will occur. Simply say "I don't know)

Specular reflections arise when the interface is smooth.

Page 150: Physics basic

RefractionRefraction

o Definition Refraction is a change in direction of wave propagation when traveling from one medium to another. A process associated with transmission (not reflection!)

o Refraction is transmission with a bend.

Page 151: Physics basic

Occurs when two conditions are metOccurs when two conditions are met

o 1. oblique incidence and

o 2. different propagation speeds

Page 152: Physics basic

o Cannot occur with normal incidence or with identical propagation speeds.

Page 153: Physics basic

Snell’s LawSnell’s Law

o The physics of refraction are described by Snell's Law

Page 154: Physics basic

TermsTerms

Frequency is the number of complete cycles/sec

Hertz is the frequency of sound, 1 Hz = 1cycle/sec

Audible sound 20 Hz – 20 kHz

Medical ultrasound frequency in MHz

Page 155: Physics basic

PiezoelectricityPiezoelectricity

1

2

3

4

Page 156: Physics basic

EchoesEchoesEchoes, arising from acoustic interfaces

form the basis of ultrasound images.

Interfaces are boundaries between materials

with different acoustic properties....

if the medium is totally homogenous, and has

no interfaces, no echoes will form and the

structure will appear anechoic.

Page 157: Physics basic

Echoes Echoes (cont’d)(cont’d)

The intensity of echoes depends

upon the difference in the acoustic

impedance of the material at the interface.

Page 158: Physics basic

Echoes Echoes (cont’d)(cont’d)

The intensity of echoes depends

upon the difference in the acoustic

impedance of the material at the interface.

Acoustic impedance (Z) is the product

of the density of the material () and the

propagation velocity of sound (c) so:

Z = cGreater the mismatch, greater the echoes

Page 159: Physics basic

Echoes Echoes (cont’d)(cont’d)

The echoes are not only related to the densityof the substance, so harder is not necessarilybrighter....it is the impedance mismatchwhich is important....so air:tissue interfaceis very echogenic as is air:bone interfacewhile muscle:fat interface is not very echogenic

Page 160: Physics basic

Velocity of SoundVelocity of Sound

0

1000

2000

3000

4000

5000

Air

Blo

o d

Liv

e r

Wa t

e r

Kid

n ey

Mu s

cle

Fat

So f

t Tis

sue

Bo n

e

4080m/sec

1540m/sec

330m/sec

Page 161: Physics basic

ReflectionReflection

Types of reflectors:

Specular.....large and smooth

will reflect like a mirror

(diaphragm).

Diffuse...the reflectors are

small; individually smaller

than the wavelength of

ultrasound, tissue substanceRememberSpecular reflection isangle dependent

Page 162: Physics basic

Ultrasound images are made up of small dots on the screen, the brightness of the individual dotcorresponds to the intensity of the echo receivedso the greater the echo, the brighter the dot...Theecho is translated into the Brightness in formingimages and this is called “B” mode ultrasound.

Page 163: Physics basic

Ultrasound images are made up of small dots on the screen, the brightness of the individual dotcorresponds to the intensity of the echo receivedso the greater the echo, the brighter the dot...Theecho is translated into the Brightness in formingimages and this is called “B” mode ultrasound.The position is calculated by accurately measuringthe time of return of the echo at the transducerafter an ultrasound pulse.

Page 164: Physics basic

Ultrasound ranging

depends on the

assumption that

sound speed is

constant and a

calibrated velocity

of 1540m/sec

Page 165: Physics basic

As sound passes through a tissue, the pressure wave diminishes in amplitude as energy is lost through absorption reflection and scattering...This is called Attenuation

Page 166: Physics basic

As sound passes through a tissue, the pressure wave diminishes in amplitude as energy is lost through absorption reflection and scattering...This is called Attenuation

Attenuation determines the depth at which structurescan be imaged and depends both on the tissue being examined as well as the transducer frequency...

Page 167: Physics basic

As sound passes through a tissue, the pressure wave diminishes in amplitude as energy is lost through absorption reflection and scattering...This is called Attenuation

Attenuation determines the depth at which structurescan be imaged and depends both on the tissue being examined as well as the transducer frequency...The higher the frequency, the higher the attenuation and lower the penetration

Page 168: Physics basic

• The higher the probe frequency the shallower

the tissue depth that can be imaged.

• The higher the probe frequency, the better

the resolution.

Use the highest frequency possible to image any structure

Page 169: Physics basic

TRANSDUCERSTRANSDUCERS

Page 170: Physics basic

DEFINITIONSDEFINITIONS

o Transducer

o Any device that converts one form of energy into another:

o Electric motor (electric to kinetic)

o Light bulb (electric to heat & light)

o Muscle (chemical to kinetic)

o Loudspeaker (electric to acoustic)

Page 171: Physics basic

Common Transducer TypesCommon Transducer Types

o Linear

o Convex

o Endocavitary

o Sector

Page 172: Physics basic

LinearLinear

Page 173: Physics basic

ConvexConvex

Page 174: Physics basic

EndocavitaryEndocavitary

Page 175: Physics basic

Piezoelectric EffectPiezoelectric Effect

o A property of certain materials to create a voltage when they are mechanically deformed.

o Also, these materials deform or change shape when a voltage is applied to them (the reverse piezoelectric effect).

Page 176: Physics basic

o PZT in ultrasound transducers is also called the ceramic, active element, or crystal.

Page 177: Physics basic

Curie TemperatureCurie Temperature

o If PZT is heated above this temperature (approximately 360C° or 680F°), it loses its piezoelectricity—i.e., the PZT is depolarized. Thus, we should not heat sterilize or autoclave transducers. Also called the Curie point.

Page 178: Physics basic

SterilizationSterilization

o The complete destruction of all living microorganisms by means of exposure to heat, chemical agents, or radiation,

Page 179: Physics basic

DisinfectionDisinfection

o Refers to the application of a chemical agent to reduce or eliminate infectious organisms on an object, such as a transducer.

Page 180: Physics basic

DisinfectionDisinfection

o With regard to infection control, the most critical instruments are those that are intended to penetrate skin or mucous membranes. These require sterilization.

Page 181: Physics basic

DisinfectionDisinfection

o Less critical instruments that simply come into contact with mucous membranes (such as fiber-optic endoscopes) require a lower level of disinfection than sterilization.

Page 182: Physics basic

DisinfectionDisinfection

o As a rule, transducers should be disinfected using Cidex™ or other cold germicides. Ultrasound transducers should never be sterilized using either dry or moist heat, or chemicals because this could likely damage the transducer

Page 183: Physics basic

Transducer ArchitectureTransducer Architecture

Active Element The piezoelectric crystal.

Page 184: Physics basic

CaseCase

o Protects the internal components from damage and insulates the patient from electrical shock.

Page 185: Physics basic

NoteNote

o Do not use a transducer with a cracked housing.

Page 186: Physics basic

WireWire

o Each active element in a transducer requires electrical contact so that the voltage from the US system can excite the crystal to vibrate thereby producing an ultrasonic wave. Similarly, during reception the sound wave deforms the crystal, producing a voltage. The voltage must be sent back to the ultrasound system for processing into an image.

Page 187: Physics basic

NoteNote

o Do not use a transducer with a frayed wire.

Page 188: Physics basic

Matching LayerMatching Layer

o Recall that impedance differences result in reflection at boundaries.

Page 189: Physics basic

Matching LayerMatching Layer

o The matching layer has an impedance between those of the skin and the active element to increase the percentage of transmitted US between the active element and the skin. Gel's impedance is in between those of the matching layer and the skin.

Page 190: Physics basic

Matching LayerMatching Layer

o The matching layer is one-quarter wavelength thick. Impedances: PZT > matching layer > gel > skin

Page 191: Physics basic

Damping ElementDamping Element

o A material that is bonded to the active element that limits the "ringing" of the PZT.

o Commonly made of epoxy resin impregnated with tungsten. Also called backing material.

Page 192: Physics basic

Damping material - advantagesDamping material - advantages

o Shortens spatial pulse length, pulse duration decreases numerical value of LARRD resolution.

o Increases picture accuracy by improving LARRD resolution

Page 193: Physics basic

Damping material - also causesDamping material - also causes

o Decreased transducer's sensitivity

o Increased bandwidth (range of frequencies) in the pulse - also called wide bandwidth

o Decreased "Q" factor. Imaging probes are low-Q

Page 194: Physics basic

Bandwidth and Quality Factor Bandwidth and Quality Factor

Page 195: Physics basic

BandwidthBandwidth

o It is uncommon for a transducer to emit a sound beam with only a single pure frequency. Rather, the pulse is more like a sound 'click' and contains a range of frequencies below and above the main frequency.

o The bandwidth is the range of frequencies^ between the highest and the lowest frequency emitted from the transducer.

Page 196: Physics basic

Quality FactorQuality Factor

o A unitless number representing the degree of damping. Imaging transducers are low-Q transducers when compared to therapeutic transducers because imaging transducers use backing material.

Page 197: Physics basic

Quality FactorQuality Factor

o The Q-factor of typical imaging transducers can be approximated by the number of cycles in the pulse produced by the transducer (approximately 2 - 4).

Page 198: Physics basic

When Q-factor is lowWhen Q-factor is low

o 1. damping is effective

o 2. pulse length & duration are short.

o 3. bandwidth is wide

o 4. axial resolution is improved

Page 199: Physics basic

Transducer FrequenciesTransducer Frequencies

o What determines the resonant frequency of a transducer?

Page 200: Physics basic

Continuous Wave TransducersContinuous Wave Transducers

o Sound wave's frequency equals the frequency of the voltage applied to the PZT by the machine's electronics.

Page 201: Physics basic

Pulsed TransducersPulsed Transducers

o The pulse repetition frequency (PRF) is determined by the number of electrical pulses the US machine delivers to the active element.

Page 202: Physics basic

The frequency of the US for a pulsed txr The frequency of the US for a pulsed txr is determined by 2 factorsis determined by 2 factors

o 1. The thickness and

o 2- The propagation speed of the piezoelectric material.

o propagation speed for PZT is approx. 4-6 mm.

Page 203: Physics basic

For Pulsed TransducersFor Pulsed Transducers

o The thinner the active element, the higher the transducer's resonant or natural frequency (think of a crystal glass.)

o The higher the active material's propagation speed, the higher the transducer's frequency.

Page 204: Physics basic

TWO-DIMENSIONALTWO-DIMENSIONAL IMAGING IMAGING

Page 205: Physics basic

o We desire "images" and slices of anatomy

o Ultrasound only travels in a straight line

o Narrow beams provide high quality imaging and good lateral resolution

Page 206: Physics basic

Solution NoteSolution Note

o construct a two dimensional image from multiple ultrasound pulses transmitted into the body in different directions.

o 2-D images may be referred to as "B-scans" or "B-modes" since they are gray scale.

Page 207: Physics basic

Mechanical ScanningMechanical Scanning

o Crystals Scanhead contains one active element

o Element Shape The crystal is circular and disc-shaped (like a coin).

Page 208: Physics basic

o Steering The active element is moved by a motor oscillating crystal or mirror through a pathway, automatically creating a scan plane.

o Focusing Conventional or Fixed: curvature (internal) of the PZT or an acoustic lens (external) focuses the beam at a specific depths

Page 209: Physics basic

Transducer ArraysTransducer Arrays

o Array A collection of active elements in a single transducer.

o Element A single slab of PZT cut into a collection of separate pieces called elements,

o Channel The electronic circuitry connected to each element.

Page 210: Physics basic

Linear ArrayLinear Arrayo A collection of elements in a line. There are 2 types:

o 1. linear switched (or sequential) array

o 2. linear phased array

Page 211: Physics basic

Annular ArrayAnnular Array

o A group of ringed elements with a common center.

Page 212: Physics basic

Convex, curved orConvex, curved or curvilinear curvilinear ArrayArray

o Elements arranged in an arc. There are 2 types:

o 1. convex switched (or sequential) array

o 2. convex phased array

Page 213: Physics basic

Linear Switched or Sequential Linear Switched or Sequential Arrays CrystalsArrays Crystals

o Large transducers with multiple elements arranged in a line. Image is no wider than the transducer.

Page 214: Physics basic

Element ShapeElement Shape

o Each element in a linear-switched array is rectangular.

Page 215: Physics basic

o A few elements (S-10), but not all, are fired at exactly the same time.

o The sound wavelets from the multiple crystals interfere with each other to create a single sound beam that travels straight ahead into the body. Then, the next group is fired.

Page 216: Physics basic

Switched arraysSwitched arrays are are also called also called sequential.sequential.o Steering No steering, pulses sent down parallel

lines.

o Focusing Fixed-focusing without steering.

o Image Shape Rectangular image shape, no wider than transducer.

o Defective Crystal Dropout extending from superficial to deep.

Page 217: Physics basic

Vertical focusing achieved conventionally with lens or Vertical focusing achieved conventionally with lens or curvature of active elements.curvature of active elements.

Page 218: Physics basic

Phased ArraysPhased Arrays

o Meaning Adjustable focus or multi-focus; achieved electronically,

Page 219: Physics basic

Crystals, Steering &Crystals, Steering & FocusingFocusing

o A collection of electric pulses is delivered to all of the transducer's elements in various patterns.

o The patterns ' focus & steer the US beam during transmission. Thus, focusing and steering are electronic.

Page 220: Physics basic

Image ShapeImage Shape

o The image is fan or sector-shaped.

o Electronic signals excite all of the elements and create only one sound pulse.

Page 221: Physics basic

o There are miniscule time delays (10 ns) between electronic pulses delivered to the individual array elements. The elements are fired nearly simultaneously.

o If we imagine the delays to represent the surface of a reflecting mirror, the direction and the shape of the wave become apparent.

Page 222: Physics basic

Defective CrystalDefective Crystal

o If one element malfunctions, the steering and focusing becomes erratic.

o Electrical Patterns no steering no transmit focusing steered upward no transmit focusing

Page 223: Physics basic
Page 224: Physics basic
Page 225: Physics basic

Beam FormerBeam Former

o The component of an US system that creates these electronic patterns is called the beam former.

Page 226: Physics basic

Dynamic ReceiveDynamic Receive

o Similarly, time delays during reception are also applied to the Focusing electrical signals from the transducer to the US system. This reception zone focusing relates to the depth of the returning echoes and optimizes image quality

Page 227: Physics basic

Annular Phased Arrays Annular Phased Arrays

o Crystals Concentric rings (donut shaped) cut from the same circular slab of PZT.

o Element Shape Ring (like a donut)

Page 228: Physics basic

o • Small diameter rings have a shallow focus but diverge rapidly.

o • Large diameter rings have a deep focal length,

Page 229: Physics basic

StrategyStrategy

o Selected focal zones, use inner crystals for shallow regions and outer crystals for deep regions,

Page 230: Physics basic

ImageImage

o The image is fan or sector-shaped. Shape

Page 231: Physics basic

FocusingFocusing

o Phasing provides electronic focusing in all planes at all

o Depths a core sample, This provides optimal lateral resolution at all depths.

Page 232: Physics basic

SteeringSteering

o Steering is performed mechanically. HINT: This is unlike other phased array transducers.

Page 233: Physics basic

Defective CrystalDefective Crystal

o Defective crystal causes a horizontal (side-to-side) band of dropout.

Page 234: Physics basic
Page 235: Physics basic

Convex or Curved ArraysConvex or Curved Arrays

o Piezoelectric crystals arranged in a curve to provide a natural sector image.

o May be sequential or phased array (just like a linear array). Image shape blunted-sector, fan-shaped image.

Page 236: Physics basic

Large transducerLarge transducer

o Convex sequential array that places a large acoustic footprint

o on the patient.

Page 237: Physics basic

Acoustic footprintAcoustic footprint

o Describes the area of contact between the transducer and the skin.

Page 238: Physics basic

Small transducerSmall transducer

o Typically a convex phased array.

Page 239: Physics basic

Dynamic ApertureDynamic Aperture

o A form of receive, electronic focusing,

o As the returning sound beam strikes the transducer, the size of the transducer surface listening for echoes is varied. This is accomplished by varying the number of elements used to receive the reflected signal,

Page 240: Physics basic

o Echoes arising early (from superficial structures) are received using only a few crystals from the array.

o As the echoes return from deeper structures, the aperture is increased. More and more elements in the array are used to listen.

Page 241: Physics basic

o This allows the beam to be as narrow as possible at all depths, and optimizes lateral resolution at all depths.

Page 242: Physics basic

Multidimensional ArraysMultidimensional Arrays

o Two-dimensional arrays provide real-time acquisition of data in three planes. Creates 3-D ultrasound images.

o Same number of elements in the up & down and side-to-side directions.

Page 243: Physics basic

o 1 ½ - dimensional arrays allow focusing in the plane of the beam width. Improves elevational resolution — makes a thinner slice, see "Slice Thickness" on page 149\|/

o More elements side-to-side than up & down.

Page 244: Physics basic
Page 245: Physics basic

Vector ArraysVector Arrays

o Vector arrays combine linear sequential and linear phased array technologies. Phasing is applied to a linear sequential array.

Page 246: Physics basic

Image ShapeImage Shape

o Trapezoidal, basically a sector with a flat top that does not come to a point.

Page 247: Physics basic

Summary—TransducersSummary—Transducers

Transducer Transducer TypeType

Image Image ShapeShape

Steering Steering TechniqueTechnique

Focusing Focusing TechniqueTechnique

Crystal Crystal DefectDefect

MechanicalMechanical SectorSector MechanicalMechanical fixedfixed Image tossImage toss

linear switchedlinear switched rectangulrectangularar

nonenone fixedfixed Vert line Vert line dropoutdropout

Linear phased Linear phased

array array

SectorSector Electronic Electronic Electronic Electronic Poor Poor steering & steering & focusing focusing

annular annular phasedphased

SectorSector MechanicaMechanical l

electronicelectronic horiz line horiz line dropoutdropout

Page 248: Physics basic

Summary—TransducersSummary—Transducers

Transducer Transducer TypeType

Image Image ShapeShape

Steering Steering TechniqueTechnique

Focusing Focusing TechniqueTechnique

Crystal Crystal DefectDefect

convex convex sequentialsequential

blunted blunted sectorsector

NoneNone FixedFixed vert line vert line dropout dropout

Convex Convex phasedphased

blunted blunted sectorsector

electronicelectronic electronicelectronic poor poor steering & steering & focusingfocusing

vectorvector flat top flat top sectorsector

electronicelectronic electronicelectronic poor poor steering & steering & focusing focusing

Page 249: Physics basic

AXIAL AXIAL RESOLUTIONRESOLUTION

Page 250: Physics basic

Resolution Resolution

o The ability to image accurately (accuracy, not merely quality)

Page 251: Physics basic

Axial ResolutionAxial Resolution

o The ability to distinguish two structures that are close to each other front to back, parallel to, or along the beam's main axis.

Page 252: Physics basic

UnitsUnits

o mm, cm — all units of distance

o The shorter the pulse, the smaller the number, the more accurate is the image

o The shorter the pulse, the better the LARRD resolution.

Page 253: Physics basic

LARRD resolution improves withLARRD resolution improves with

o Less ringing, fewer cycles in pulse (fewer cars in the train)

o Higher frequency sound (each car in the train is shorter), shorter wavelength (each car is shorter).

o changing either of these factors requires a new transducer

Page 254: Physics basic

Note Note

o As frequency increases, the numerical value of the LARRD resolution decreases. This means that we have improved LARRD resolution and higher quality images with high frequency transducers.

Page 255: Physics basic

BIOEFFECTS BIOEFFECTS

Page 256: Physics basic

Measuring the Output of Measuring the Output of Ultrasound MachinesUltrasound Machines

oHydrophone:o A small needle with a piezoelectric crystal

at its end. The needle is placed in the ultrasound beam.

Page 257: Physics basic

HydrophoneHydrophoneo It attaches to an oscilloscope and displays

acoustic signals received by the crystal. Can quantitate amplitude, period, pulse duration and pulse repetition period.

Page 258: Physics basic

Radiation ForceRadiation Forceo An incident sound wave can exert a small but

measurable force on an object. If the object is a balance or a float, we can measure the SATA intensity. If a small suspended ball is used, we can measure the SPTA intensity.

Page 259: Physics basic

Acoustic-OpticsAcoustic-Opticso Based on the interaction of two

types of waves, sound and light. It quantifies amplitude, period, pulse duration & pulse repetition period.

o A shadowing system, called a Schlieren, uses this principle to measure beam profiles.

Page 260: Physics basic

CalorimeterCalorimeter

o A transducer which turns acoustic energy into heat. When the total heat gain is measured along with the time that it took to obtain the heat, the total power of the US beam can be calculated.

Page 261: Physics basic

ThermocoupleThermocouple

o A small device embedded in an absorbing material. The US is absorbed, turned into heat, and the thermocouple measures the change in temperature. The US intensity at specific points in space are measured by a thermocouple.

Page 262: Physics basic

CrystalsCrystals

o Cholesteric liquid crystals or starch/iodine blue, when struck by different US intensities, turn different colors. The color of the crystals give us insight into the shape and strength of the beam.

Page 263: Physics basic

Biologic Effects & SafetyBiologic Effects & Safety

o In-vivo & In-vitro Bioeffects have been studied in experiments with:

o Living (in vivo) as well as in

o Nonliving settings {in vitro).

Page 264: Physics basic

DosimetryDosimetry

o The science of identifying and measuring those characteristics of an US field which are especially relevant to its potential for producing biological effects.

Page 265: Physics basic

Thermal MechanismThermal Mechanism

o Temperature elevation via absorption resulting from interaction of biologic tissue and US. A second mode of thermal injury may result from localized scattering of acoustic energy, especially at in homogencities within the medium (Rayleigh scattering.)

Page 266: Physics basic

Tissues BoneTissues Bone

o Tissue-bone interface is an absorber. Therefore temperature elevation at a tissue-bone interface is more likely.

Page 267: Physics basic

Fetal tissuesFetal tissues

o Temperature elevation in fetal soft tissue is considered of potentially greater harm than in adults. Thus, fetal soft tissues adjacent to bone is of great concern.

Page 268: Physics basic

Thermal IndexThermal Index

o The Thermal Index is a number proposed in the most recent AIUM guidelines that relates to tissue heating. Thermal index is a theoretical calculation related to the possible temperature elevation, measured in degrees centigrade, that could be produced by the sound beam.

Page 269: Physics basic

o TIS—thermal index calculated assuming that the sound beam travels in soft tissue.

o TIB—thermal index calculated assuming that bone is at the beam's focus, usually a higher number than the TIS

o TIC—thermal index calculated assuming that cranial bone is at or near the skin's surface.

Page 270: Physics basic

Focused vs. Unfocused Thermal Focused vs. Unfocused Thermal EffectsEffectso Focused beams are less likely to cause

temperature elevation in tissues.

o Unfocused beams are more likely to cause temperature elevation in tissues.

Page 271: Physics basic

o This phenomenon occurs because a narrow beam heats only a small region of tissue and the heat is rapidly transferred to and dissipated by adjacent tissues that were not heated by the US beam.

Page 272: Physics basic

Intensity LimitsIntensity Limits

o Therefore, the AIUM maximum intensity limit is lower for unfocused sound (lOOmW/cm2) than for focused sound (l,000)mW/cm2 or 1 watt/cm2.)

Page 273: Physics basic

Cavitation MechanismCavitation Mechanism

o Gaseous nuclei

o Microbubbles (gaseous nuclei) may be excited by US. This takes the form of shrinking and expanding of the bubble.

Page 274: Physics basic

o Potential of near total energy absorption where the nuclei exist may lead to thermal injury.

o So far, minimal evidence that cavitation really occurs in diagnostic US. Current data indicate cavitation can occur in mammals at SPTP intensities exceeding 3,500W/cm2.

Page 275: Physics basic

Mechanical IndexMechanical Index

o The Mechanical Index (MI) is a number proposed in the AIUM guidelines that relates to cavitation.

o Mechanical index is higher (more likely to produce cavitation) with:

o 1) Higher pressure beams

o 2) Lower frequency sound

Page 276: Physics basic

STABLE CAVITATIONSTABLE CAVITATION

o Bubbles tend to oscillate when exposed to acoustic waves of small amplitude. Bubbles do not burst. Bubbles that are a few micrometers in diameter double in size.

o Bubbles intercept, reradiate and absorb acoustic energy.

Page 277: Physics basic

TRANSIENT CAVITATIONTRANSIENT CAVITATION

o Bubbles expand and collapse violently. Bubbles burst.

o Depends upon the pressure of ultrasound pulses (MPa).

o Synonyms also called normal or inertial cavitation

Page 278: Physics basic

ThresholdThreshold

o Threshold for transient cavitation is only 10% greater than the pressure for stable cavitation.

Page 279: Physics basic

EffectsEffects

o Highly localized violent effects:

o Enormous pressures— shock wave— mechanical stress.

o Colossal temperatures—thousands of degrees.

Page 280: Physics basic

Bioeffects—General ConceptsBioeffects—General Concepts

o • In Vitro (out of the body) Studies—results are real; although important scientifically, "reports of in vitro studies which claim direct clinical significance should be viewed with caution" (AIUM statement.)

Page 281: Physics basic

o Very high US intensities—genetic alteration or damage which may be lethal to cells.

o Under controlled conditions, bioeffects are considered beneficial!

o Low level US intensities—no known effects.

Page 282: Physics basic

Epidemiology and StatisticsEpidemiology and Statistics

o Epidemiological Studies (population studies)

o Require large numbers of patients when the occurrence rate of the measure effect is small. This is the case in diagnostic imaging.

Page 283: Physics basic

o Randomized clinical studies require large data sets on each patient to account for other factors which may contribute to the finding.

o Using this method, diagnostic ultrasound has shown no adverse effects on fetal outcome or birth weight or any other measurement.

Page 284: Physics basic

Best study isBest study is

o 1. Prospective and

o 2. Randomized

Page 285: Physics basic

Limitations of Epidemiologic StudiesLimitations of Epidemiologic Studies

o 1. often retrospective (looking at charts and information acquired in the past); it is best to collect data prospectively so that the record is complete

Page 286: Physics basic

o 2. ambiguities —justification for exam, gestational age, number of exams, exposure, and mode

o 3. other risk factors —maternal age, nutrition, smoking, alcohol, drugs

Page 287: Physics basic

Statistical ConsiderationsStatistical Considerations

o The smaller the effect, the harder it is to detect

o Requires large number of patients

Page 288: Physics basic

AIUM Statement on Clinical SafetyAIUM Statement on Clinical Safety

o Approved: March 1988 o Diagnostic ultrasound has been in use since the

late 1950s.o Given its known benefits and recognized efficacy

for medical diagnosis, including use during human pregnancy, the American Institute of Ultrasound in Medicine herein addresses the clinical safety of such use:

Page 289: Physics basic

o No confirmed biological effects on patients or instrument operators caused by exposure at intensities typical of present diagnostic ultrasound instruments have ever been reported.

Page 290: Physics basic

o Although the possibility exists that such biological effects may be identified in the future, current data indicate that the benefits to patients of the prudent use of diagnostic ultrasound outweigh the risks, if any, that may by present.

Page 291: Physics basic

Benefits should outweigh the risks. Benefits should outweigh the risks.

o The AIUM suggests:o Do not perform studies without reason

o Do not prolong studies without reason

o Minimize exposure time (but perform a complete diagnostic exam).

o Use minimum output power and highest receiver gain required to produce optimal images

o ALARA Principle .

Page 292: Physics basic

Electrical and Mechanical HazardsElectrical and Mechanical Hazards

o Several different instruments as well as the individual components of the US system may be linked to a patient at any given time. Precautions such as proper electrical grounding should always be taken to avoid electrical hazard. Instruments should be routinely checked for proper condition.

Page 293: Physics basic

Shadowing Shadowing And

Enhancement

Page 294: Physics basic

Acoustic Shadowing

Acoustic Shadowing

Page 295: Physics basic

Acoustic Enhancement

Page 296: Physics basic

Controls

Page 297: Physics basic

Contrast and BrightnessContrast and Brightness

o Monitor specific

o Does not need to be adjusted very frequently

Page 298: Physics basic

GainGain

o This is the most important control for image optimization

Page 299: Physics basic

Attenuation causes amplitude lowering in deeper tissues....amplitude is translated into brightness

Similar lesionsat different depths should look the same!!

Page 300: Physics basic

Time Gain CompensationTime Gain Compensation

Page 301: Physics basic

The shape of the basic gain filtercan be altered and machines providevarious controls for altering the gain atspecific depths.

Page 302: Physics basic

Gain Gain

o Use high gain to get detail in dark areas

o Low gain for detail in bright areas

Page 303: Physics basic

Gain ControlsGain Controls

Page 304: Physics basic

Gain ControlsGain Controls

Page 305: Physics basic

Gain Gain

Page 306: Physics basic

Gain Gain

Page 307: Physics basic

Gain Gain

Page 308: Physics basic

Gain Gain

Page 309: Physics basic

FocusFocus

Ensure that the structure of interestis in the focal zone

Page 310: Physics basic

FocusFocus

Ensure that the structure of interestis in the focal zone

Page 311: Physics basic

TransducersTransducers

o Piezoelectric

o Both the transmitter and receiver of ultrasound

o Central or preferential frequency, the range of frequency is the “Bandwidth”

Page 312: Physics basic

Classification of TransducersClassification of Transducers

o Method of beam steering, mechanical or electronico Element arrangement and shape of field...linear,

sector (phased), convex or annularo Special probes, encocavitary, intravascular probes

Page 313: Physics basic

Transducer SelectionTransducer Selection

o The higher the frequency, the better the resolutiono The higher the frequency, the lower the penetrationo THI combines the advantages of better resolution and

higher penetration

Page 314: Physics basic

Select the highest frequency transducer

permitting penetration to the required depth.....

for superficial structures like breast, thyroid,

scrotum and for appendix use 7.5 – 10 MHz,

for abdomen 3.5 – 6 MHz and for heart 2.5-5 MHZ

Transducer selectionTransducer selection

Page 315: Physics basic

oProbe frequency

oFreeze

oDynamic Range

oPost processing

Page 316: Physics basic

Transducer FrequencyTransducer Frequency

Page 317: Physics basic

Transducer FrequencyTransducer Frequency

Page 318: Physics basic

Transducer FrequencyTransducer Frequency

Page 319: Physics basic

Transducer selection Transducer selection (Cont’d)(Cont’d)

o Select the foot-print appropriate for the structure size and depth and intervening obstacles

o For heart, a micro-convex or sector probe that will allow scanning between ribs; for small parts a linear face and for abdomen a linear or convex face

Page 320: Physics basic

Dynamic RangeDynamic Range

o Use the highest possible dynamic range without making the picture too soft

Page 321: Physics basic

Dynamic RangeDynamic Range

DR 90 65 30

Page 322: Physics basic

Image QualityImage Quality

o Spatial resolution

o Contrast resolution

o Temporal resolution

Page 323: Physics basic

Contrast

Page 324: Physics basic

Contrast

N=16

Page 325: Physics basic

EEndnd