Basics of echo & principles of doppler echocardiography


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Basics of echo & principles of doppler echocardiography

  1. 1. BASICS OF ECHOCARDIOGRAPHYAND PRINCIPLES OF DOPPLER ECHO<br />Abraha Hailu<br />August 29, 2010<br />
  2. 2. Topic outline<br />
  3. 3. 1. BASICS<br />ultrasound (1923) <br />vibrations of the same physical nature as sound but with frequencies above the range of human hearing, namely frequencies greater than 20,000 cycles per second.<br />the diagnostic or therapeutic use of ultrasound and esp. a noninvasive technique involving the formation of a two-dimensional image used for the examination and measurement of internal body structures and the detection of bodily abnormalities<br />a diagnostic examination using ultrasound<br />
  4. 4. Medical ultrasound imaging typically uses sound waves at frequencies of 1,000,000 to 20,000,000 Hz (1.0 to 20 MHz). In contrast, the human auditory spectrum (between 20 and 20,000 Hz)<br />Frequency and wavelength are mathematically related to the velocity of the ultrasound beam within the tissue:<br /> Velocity =  Wavelength (mm)  x  frequency (Hz)<br />The speed with which an acoustic wave moves through a medium is dependent upon the density and resistance of the medium. <br /><ul><li>Media that are dense will transmit a mechanical wave with greater speed than those that are less dense.</li></ul>The resolution of a recording, ie, the ability to distinguish two objects that are spatially close together, varies directly with the frequency and inversely with the wavelength<br />High frequency, short wavelength ultrasound can separate objects that are less than 1 mm apart. <br />
  5. 5. Imaging with higher frequency (and lower wavelength) transducers permits enhanced spatial resolution<br /><ul><li>However, because of attenuation, the depth of tissue penetration or the ability to transmit sufficient ultrasonic energy into the chest is directly related to wavelength and therefore inversely related to transducer frequency
  6. 6. As a result, the trade-off for use of higher frequency transducers is reduced tissue penetration</li></ul>The trade-off between tissue resolution and penetration guides the choice of transducer frequency for clinical imaging. <br /><ul><li>As an example, higher frequency transducers can be used in echocardiography for imaging of structures close to the transducer or the chest wall, such as the apex of the left ventricle with transthoracic imaging.</li></li></ul><li>INTERACTION OF ULTRASOUND WAVES WITH TISSUES<br />When an ultrasonic wave travels through a homogeneous medium, its path is a straight line. However, when the medium is not homogeneous or when the wave travels through a medium with two or more interfaces, its path is altered; either of the ff:<br /> Scattering:<br /><ul><li>Small structures, eg, less than 1 wavelength in lateral dimension, result in scattering of the ultrasound signal
  7. 7. Unlike a reflected beam, scattering results in the US beam being radiated in all directions, with minimal signal returning to the transducer</li></ul>Refraction: <br />Attenuation:<br /><ul><li>Signal strength is progressively reduced due to absorption of the US energy by conversion to heat (frequency and, wavelength dependent)
  8. 8. The depth of penetration:
  9. 9. 30 cm for a 1 MHz transducer,
  10. 10. 12 cm for 2.5 MHz transducer, and
  11. 11. 6 cm for a 5 MHz transducer
  12. 12. Air has a very high acoustic impedance, resulting in significant signal attenuation when imaging through lung tissue, especially emphysematous lung, or pathologic conditions such as pneumomediastinum or subcutaneous emphysema
  13. 13. In contrast, filling of the pleural space with fluid, generally enhances ultrasound imaging</li></li></ul><li>Ultrasound waves sent from chest wall<br />
  14. 14. ULTRASOUND TRANSDUCERS <br />US transducers use a piezoelectric crystal to generate and receive ultrasound wavesImage formation: is related to the distance of a structure from the transducer, based upon the time interval between ultrasound transmission and arrival of the reflected signalThe amplitude is proportional to the incident angle and acoustic impedance, and timing is proportional to the distance from the transducer<br />
  15. 15. SECOND HARMONIC IMAGING(improving resolution)<br />An ultrasound wave traveling through tissue becomes distorted, which generates additional sound frequencies that are harmonics of the original or fundamental frequency<br /><ul><li>produces more harmonics the further it travels through tissue
  16. 16. uses broadband transducers that receive double the transmitted frequency</li></ul>When compared to conventional imaging, it reduces variations in ultrasound intensity along endocardial and myocardial surfaces, enhancing these structures <br />of particular benefit for patients in whom optimal echocardiographic images are technically difficult to obtain<br /><ul><li>harmonic imaging improves interphase definition</li></li></ul><li>
  17. 17. 2. IMAGING MODALITIES<br />Two dimensional (2-D) imaging :<br />A 2D image is generated from data obtained mechanically (mechanical transducer) or electronically (phased-array transducer)<br />The signal received undergoes a complex manipulation to form the final image displayed on the monitor including signal amplification, time-gain compensation, filtering, compression and rectification.<br />M-mode:<br />Motion or "M"-mode echocardiography is among the earliest forms of cardiac ultrasound<br /> The very high temporal resolution by M-mode imaging permits:<br />identification of subtle abnormalities such as fluttering of the anterior mitral leaflet due to aortic insufficiency or movement of a vegetation. <br />dimensional measurements or changes, such as chamber size and endocardial thickening, can be readily appreciated<br />
  18. 18. A. 2-D ECHOCARDIOGRAPHY<br />
  19. 19. OPTIMIZATION OF 2-D IMAGESTechnical Factors I<br />TRANSDUCER:<br /><ul><li>High frequency increases backscatter and resolution but lacks depth penetration
  20. 20. Low-frequency transducers permit good penetration but reduced image resolution</li></ul>DEPTH:<br /><ul><li>The deeper the field of the image, the slower the frame rate
  21. 21. The smallest depth that permits display of the region of interest should be employed</li></ul>FOCUS:<br /><ul><li>Indicates the region of the image in which the ultrasound beam is narrowest
  22. 22. Resolution is greatest in this region</li></ul>GAIN:<br /><ul><li>This function adjusts the displayed amplitude of all received signals</li></li></ul><li>TRANSTHORACIC ACOUSTIC WINDOWS<br />
  23. 23. IMAGING PLANES<br />The long-axis plane is the plane perpendicular to the posterior and anterior surfaces of the body and parallel to the long axis of the heart<br />
  24. 24. Sweeping begins at the base of the heart which appears on the rt of the screenThe left atrium, the mitral valve and the right ventricular outflow tract are seen.<br />
  25. 25.
  26. 26. Parasternal WindowRight Long-Axis ViewSweeping begins at the right atrium which is on the right of the screen. In this view we can see the right atrium and the right ventricle, with the tricuspid valve in between<br />
  27. 27.
  28. 28. The short-axis plane is the plane that runs parallel to the posterior and anterior surfaces of the body and transects the heart from its apex to its base encompassing all four cardiac chambers<br />
  29. 29. Parasternal Short-Axis ViewsObtained from the parasternal window by rotating the transducer clockwise by 90ºHence, the image index marker is pointed toward the patient´s right supraclavicularfossa. A series of sweeps transect the heart from the base to the apex by changes in transducer position and angulation. There are three characteristic levels: 1) great vessels, 2) mitral valve, 3) ventricles.<br />
  30. 30. Parasternal Short-Axis ViewGreat Arteries LevelSweeping begins at the left edge of the atrium which appears on the right of the screen<br />
  31. 31. At aortic valve level it demonstrates all three aortic valve leaflets. The pulmonary valve, the right ventricular outflow tract, the right atrium and the left atrium are seen in this view.<br />
  32. 32. Parasternal Short-Axis ViewGreat Arteries LevelIn this view we can see the pulmonary valve (PV) and pulmonary artery (PA) with right (RPA) and left branches (LPA).<br />
  33. 33. Parasternal Short-Axis ViewMitral Valve LevelThe anterior and posterior mitral leaflets are seen as they open in diastole and close in systole<br />
  34. 34. Parasternal Short-Axis ViewMitral Valve Level<br />
  35. 35. The four-chamber plane is the plane that runs parallel to the posterior and anterior surfaces of the body and transects the heart from its apex to its base encompassing all four cardiac chambers<br />
  36. 36. Apical WindowSweeping begins at the left edge of the heart which appears on the right of the screen.<br />
  37. 37. 4-Chamber ViewIn this view we can see the left ventricle, the right ventricle, the left atrium and the right atrium. The tricuspid annulus lies slightly (up to 10 mm) closer to the apex than the mitral annulus. The septal and posterior tricuspid leaflets are seen in this view.<br />
  38. 38. Apical Window5-Chamber ViewBy tilting the transducer anteriorly, the aortic root is seen in an oblique long view.<br />
  39. 39. Apical Window2-Chamber ViewSweeping begins at the anterior face of the left ventricle which appears on the right of the screen. From the four-chamber view, the transducer is rotated anti-clockwise by 60º to obtain the two-chamber view of the left ventricle, the mitral valve and the left atrium.<br />
  40. 40. Apical Window2-Chamber ViewThis view shows the LV, the LA and the MV. The LV shows the inferior wall on the left and the anterior wall on the right.<br />
  41. 41. Subcostal Window4-Chamber ViewSweeping starts at the apex which appears on the right of the screen. A view of all four chambers shows the right ventricular free wall, the midsection of the interventricular septum and the posterolateral left ventricular wall. In this view, the interatrial septum is perpendicular to the direction of the ultrasound beam<br />
  42. 42. Subcostal WindowThe inferior vena cava as it enters the right atrium and the central hepatic vein are seen.<br />
  43. 43. Suprasternal Notch WindowSweeping begins at the descending aorta which appears on the right of the screen. The long-axis view shows the ascending aorta, the arch, the proximal descending aorta and the origins of the right brachiocephalic and left common carotid and subclavian arteries.<br />
  44. 44. Suprasternal Notch Window<br />
  45. 45. B. M-MODE ECHOCARDIOGRAPHY<br />a single line of sight is included, the repetition frequency of the pulse transmission is very high and sampling rates of around 1800 cycles/sec are usedContinuously-moving structures may be identified more accurately when motion versus time, as well as depth, is displayed clearly on the M-mode recording<br />
  46. 46.
  48. 48. AORTIC VALVE AND LEFT ATRIUM<br />The aortic root is moving anteriorly in systole and posteriorly in diastole. The left atrium is posterior to the aortic root. <br />The aortic leaflet coaptation point is seen as a thin line in diastole. <br />AO is measured in end-diastole and LA in end-systole.<br />
  49. 49.
  50. 50. In early diastole, the leaflets separate widely, with the maximum early diastolic motion of the anterior leaflet termed the E point. The leaflets move together in mid-diastole and then separate again with atrial systole, the A point. Closure at the end of diastole is termed C point.<br />
  51. 51. M-mode recording perpendicular to the long axis of and through the centre of the left ventricle at papillary muscle level provides standard measurements of systolic and diastolic thickness and chamber dimensions:<br />
  52. 52. Normal Values<br />Left ventricular end-diastole: 37 - 57 mm (23 -31 mm/m²)<br />Left ventricular end-systole: 21 - 40 mm (14 -21 mm/m²)<br />Interventricular septum: 7 - 11 mm<br />Posterior wall: 7 - 11 mm<br />
  53. 53. 3. DOPPLER ECHOCARDIOGRAPHY<br />BASIC PRINCIPLES:<br />utilizes ultrasound to record blood flow within the cardiovascular system (While M-mode and 2D echo create ultrasonic images of the heart)<br />is based upon the changes in frequency of the backscatter signal from small moving structures, ie, red blood cells, intercepted by the ultrasound beam<br />
  54. 54. A moving target will backscatter an ultrasound beam to the transducer so that the frequency observed when the target is moving toward the transducer is higher and the frequency observed when the target is moving away from the transducer is lower than the original transmitter frequency<br /><ul><li>This Doppler phenomenon is familiar to us as the sound of a train whistle as it moves toward (higher frequency) or away (lower frequency) from the observer
  55. 55. This difference in frequency between the transmitted frequency (F[t]) and received frequency (F[r]) is the Doppler shift:
  56. 56.   Doppler shift (F[d]) = F[r] - F[t]</li></li></ul><li><ul><li>Doppler effect(Pairs of transmitting (T) and receiving (R) transducers):
  57. 57. With a stationary target (panel A): the carrier frequency [f(t)] from the transmitting transducer strikes the target and is reflected back to the receiving transducer at the reflected frequency [f(r)], which is unaltered
  58. 58. with a target moving toward the transducer (panel B): An increase in f(r) is seen
  59. 59. with a target moving away from the transducer (panel C): f(r) is reduced
  60. 60. In all cases, the extent to which f(t) is increased or reduced is proportional to the velocity of the target</li></li></ul><li>A flow moving toward the transducer has a higher observed frequency than a flow moving away from the transducer.<br />
  61. 61. Blood flow velocity (V) is related to the Doppler shift by the speed of sound in blood (C) and ø (the intercept angle between the ultrasound beam and the direction of blood flow)<br /><ul><li>A factor of 2 is used to correct for the "round-trip" transit time to and from the transducer.
  62. 62.   F[d] = 2 x F[t] x [(Vx cos ø)] ÷ C</li></ul>This equation can be solved for V, by substituting (F[r] - F[t]) for F[d]:<br /><ul><li>  V = [(F[r] -F[t]) x C] ÷ (2 x F[t] x cos ø)</li></li></ul><li>the angle of the ultrasound beam and the direction of blood flow are critically important in the calculation<br /><ul><li>For ø of 0º and 180º (parallel with blood flow), cosine ø = 1
  63. 63. For ø of 90º (perpendicular to blood flow), cosine ø = 0 and the Doppler shift is 0
  64. 64. For ø up to 20º, cos ø results in a minimal (<10 percent) change in the Doppler shift
  65. 65. For ø of 60º, cosine ø = 0.50 </li></ul>The value of ø is particularly important for accurate assessment of high velocity jets, which occur in aortic stenosis or pulmonary artery hypertension<br />It is generally assumed that ø is 0º and cos ø is therefore 1<br /><ul><li>Ideally, the beam should be placed parallel to blood flow
  66. 66. When the beam does not lie parallel, it is possible to introduce a correction into the calculation of flow velocity by measuring the cosine of the angle of interrogation and introducing this value into the Doppler equation</li></li></ul><li>SPECTRAL ANALYSIS<br /> When the backscattered signal is received by the transducer, the difference between the transmitted and backscattered signal is determined by comparing the two waveforms with the frequency content analyzed by: fast Fourier transform (FFT)<br /><ul><li>The display generated by this frequency analysis is termed spectral analysis
  67. 67. By convention, time is displayed on the x axis and frequency shift on the y axis
  68. 68. Shifts toward the transducer are represented as "positive" deflections from the "zero" baseline, and shifts away from the transducer are displayed as "negative" deflections</li></li></ul><li><ul><li> Spectral information can be displayed in real time (Doppler figure)The Doppler signal portrays the entire period of flow, ie: acceleration (a), peak flow (pf), and deceleration (d). </li></li></ul><li>
  69. 69.
  70. 70.
  71. 71.
  72. 72.
  73. 73. Right Ventricular InflowCan be recorded from an apical approach. The pattern is similar to mitral flow.<br />
  74. 74. Left Ventricular OutflowAn apical window is used with a pulsed Doppler sample volume positioned on the left ventricular side of the aortic valve. Note the narrow band of the systolic velocities.<br />
  75. 75. Right Ventricular OutflowFrom a parasternal short-axis view, the sample volume is located in the right ventricular outflow tract. The Doppler shape is similar to the left ventricular outflow curve<br />
  76. 76. Suprahepatic Vein FlowFrom the longitudinal subcostal view, the sample volume is located at the main suprahepatic vein. There are two positive waves, (A) and (V), and two negative ones, (X) and (Y).<br />
  77. 77. DOPPLER MODALITIES <br />Doppler methods used for cardiac evaluation :<br />continuous wave doppler<br />Pulsed wave doppler<br />color flow doppler<br />
  78. 78. CONTINUOUS WAVE DOPPLER<br />employs two dedicated ultrasound crystals, one for continuous transmission and a second for continuous reception<br /><ul><li>This permits measurement of very high frequency Doppler shifts or velocities</li></ul>Limitations of this technique: <br /><ul><li>It receives a continuous signal along the entire length of the US beam
  79. 79. Thus, there may be overlap in certain settings, such as:
  80. 80. stenoses in series (eg, left ventricular outflow tract gradient and aortic stenosis) or
  81. 81. flows that are in close proximity/alignment (eg, AS and MR)</li></li></ul><li>
  82. 82.
  83. 83. An ideal Doppler profile is one with a smooth "outer" contour, well-defined edge and maximum velocity, and abrupt onset and termination<br />
  84. 84.
  85. 85.
  86. 86. PULSED DOPPLER <br />permits sampling of blood flow velocities from a specific region <br /><ul><li>In contrast to continuous wave Doppler which records signal along the entire length of the ultrasound beam</li></ul>is always performed with 2D guidance to determine the sample volume position<br />Particularly useful for assessing the relatively low velocity flows associated with:<br />transmitral or transtricuspid blood flow, <br />pulmonary venous flow, <br />left atrial appendage flow, or <br />for confirming the location of eccentric jets of aortic insufficiency or mitral regurgitation <br />
  87. 87. <ul><li>From a four-chamber view, a pulse wave Doppler signal is placed in the superior portion of the left atrium at the entry site of the right upper pulmonary veinNote that the outline of pulmonary flow signal is seen S: systolic wave; D: diastolic wave. </li></li></ul><li>
  88. 88. Because PWD repeatedly samples the returning signal, there is a maximum limit to the frequency shift that can be measured unambiguouslyThe maximum detectable frequency shift (the Nyquist limit) is one-half the PRFIf velocity exceeds the Nyquist limit, signal aliasing is seen with the signal cut off at the edge of the display and the top of the waveform appearing in the reverse partHigh-PRF increases the number of sample volumes<br />
  89. 89. COLOR FLOW IMAGING<br /><ul><li>With CF imaging, velocities are displayed using a color scale:
  90. 90. with flow toward the transducer displayed in orange/red
  91. 91. flow away from the transducer displayed as blue</li></li></ul><li>Colour DopplerThe option of displaying “variance” allows an additional colour (usually green) to be added to indicate that a mean velocity has excessive variability (turbulent flow).<br />
  92. 92. apical four chamber view with color flow Doppler during diastole This color signal is used to position a pulsed wave Doppler sample volume so that quantitatable signals of flow can be obtained from the pulmonary veins and from the mitral leaflet tips<br />
  93. 93.
  94. 94. The long axis parasternal view with superimposed color flow Doppler mapping of the left ventricular inflow and ouflow tracts obtained during diastole<br />
  95. 95. the long axis parasternal view of the left ventricular outflow tract during systole; a normal color flow signal (red-orange) is seen in the left ventricular outflow tract. The occasional blue patches in the signal represent aliasing and suggest that the signal is at or exceeds the Nyquist limit.<br />
  96. 96. Short axis view through the base of the heart with CFdoppler imaging <br />short axis view recorded from the base of the heart:<br />Color flow Doppler imaging during systole (panel A), demonstrates normal systolic flow from the right ventricular outflow tract (RVOT) to the main pulmonary artery (MPA). <br />The flow signal is red in the proximal RVOT as it travels towards the transducer. <br />As it moves at right angles to the interrogating beam the signal briefly disappears. When the flow turns away from the transducer and exits into the MPA it is coded blue.<br />short axis view through the base of the heart during diastole:<br />shows diastolic flow signal (red) from pulmonic valve (PV) denoting trivial pulmonary regurgitation (PR) which is found in 90 percent of normals.<br />
  97. 97. <ul><li>Color Doppler M-mode from the four-chamber view:In the normal ventricle, the flow propagation is rapid and the slope is steep (panel A)The rate at which flow propagates into the ventricle of a patient with cardiomyopathy and diastolic dysfunction is considerably slower (panel B)This observation is particularly useful when trying to differentiate normal from "pseudonormal" filling patterns in diastolic dysfunction. </li></li></ul><li>
  98. 98. Color flow Doppler of MR<br />Apical four chamber view in systole: <br />Mild MR & TR<br /><ul><li>The jets are central and do not penetrate the left atrium (LA) beyond the mid cavity</li></ul>severe MR:<br /><ul><li>the arrows outline the course of a jet during systole that adheres to and follows the contour of the LA(wall hugging jets)</li></li></ul><li>
  99. 99. Five chamber view from a 2-D echo shows a moderate amount of AR and left ventricular enlargement<br />
  100. 100. The parasternal long axis view with color Doppler demonstrates severe AR associated with marked dilatation of the aortic root<br />
  101. 101. DOPPLER VELOCITY AND PRESSURE GRADIENT<br /> Doppler echo can estimate the pressure difference across a stenotic valve or between two chambers<br />This r/n ship is defined by the Bernoulli equation and is dependent on :<br /><ul><li>velocity proximal to a stenosis (V1)
  102. 102. velocity in the stenotic jet (V2)
  103. 103. density of blood (p), acceleration of blood through the orifice (dv/dt), and viscous losses (R[v]): </li></ul>The pressure gradient (Δ P) can be calculated from:<br /><ul><li>  Δ P = [0.5 x p x (V2 x V2 - V1 x V1)] + [p x (dv/dt)] + R[v]</li></ul>(If one assumes that the last two terms (acceleration and viscous losses) are small, and then enter the constants, the formula is simplified to):<br /><ul><li>  Δ P (mmHg) = 4 x (V2 x V2 - V1 x V1)</li></ul>Thus, the Bernoulli formula may be further simplified:<br /><ul><li>  Δ P (mmHg) = 4V2</li></li></ul><li>
  104. 104. <ul><li> In TR, a CW Doppler can be passed from the apex to base across the tricuspid valve in the apical four chamber view & the Doppler shift caused by the TR displayedIn this example, the peak velocity of the TR jet is 3 M/sec ( 36 mm Hg grad. b/n RV & RA) If the RA pressure is known or can be estimated, the sum of RA pressure and the RA to RV gradient is equal to the peak PAP (assuming no PS ) </li></li></ul><li>The CW Doppler obtained across the mitral orifice records a peak velocity of 2.8 m/sec( Bernoulli equation: an initial diastolic gradient across the mitral valve of 31 mmHg)<br />
  105. 105.
  106. 106. REFERENCES<br />CLINICAL ECHOCARDIOGRAPHY; HOSPITAL UNIVERSITARI VALL D´ HEBRON BARCELONA, Arturo Evangelista and HerminioGarcía del CastilloCo-authors: Teresa González-Alujas, Gustavo Avegliano, ZamiraGómez-Bosch; February 2004<br />UpToDate 17.3<br />