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Medical Imaging Ultrasound Edwin L. Dove 1412 SC [email protected] 335-5635 3D Reconstruction Why Ultrasound in Cardiology? • Portable, relatively cheap • Non-ionizing • During the echocardiogram, it is possible for the cardiologist to: – Watch the heart’s motion – in 2D real-time – Ascertain if the valves are opening and closing properly, and view any abnormalities – Determine the size of the heart chambers and major vessels – Measure the thickness of the heart walls – Calculate standard metrics of health/disease • e.g., Volume, EF, SV, CO – Dynamic evaluation of abnormalities Sinusoidal pressure source Quantitative Description p pressure applied in z-direction density viscosity p p p k k z t z t 2 k p Pm exp az cos t kz 2 k 2 f c k k cf Speed of Sound in Tissue • The speed of sound in a human tissue depends on the average density (kg·m3) and the compressibility K (m2·N-1) of the tissue. 1 c 0 K Sound Velocity for Various Tissues Tissue Air Fat Human tissue (mean) Brain Blood Skull bone Water Mean Velocity (m·s-1) 330 1450 1540 1541 1570 4080 1480 Tissue Characteristics • Engineers and scientists working in ultrasound have found that a convenient way of expressing relevant tissue properties is to use characteristic (or acoustic) impedance Z (kg·m-2 ·s-1) Z 0 c Pressure Generation • Piezoelectric crystal • ‘piezo’ means pressure, so piezoelectric means – pressure generated when electric field is applied – electric energy generated when pressure is applied Charged Piezoelectric Molecules Highly simplified effect of E field Piezoelectric Effect Piezoelectric Principle Vibrating element Transducer Design Transducer Reflectance and Refraction Snells’ Law sin i 1 c1 sin t 2 c2 (Assumes i = r) Reflectivity Z2 Z1 _ pr cos t cos i R Z2 Z1 pi cos t cos i At normal incidence, i = t = 0 and Z 2 Z1 R Z2 Z 1 Reflectivity for Various Tissues Materials at Interface Brain-skull bone Fat-muscle Fat-kidney Muscle-blood Soft tissue-water Soft tissue-air Reflectivity 0.66 0.10 0.08 0.03 0.05 0.9995 Specular Reflection • The first, specular echoes, originate from relatively large, strongly reflective, regularly shaped objects with smooth surfaces. These reflections are angle dependent, and are described by reflectivity equation . This type of reflection is called specular reflection. Scattered Reflection • The second type of echoes are scattered that originate from small, weakly reflective, irregularly shaped objects, and are less angledependent and less intense. The mathematical treatment of non-specular reflection (sometimes called “speckle”) involves the Rayleigh probability density function. This type of reflection, however, sometimes dominates medical images, as you will see in the laboratory demonstrations. Circuit for Generating Sharp Pulses Pressure Radiated by Sharp Pulse Ultrasound Principle Echoes from Internal Organ Attenuation • Most engineers and scientists working in the ultrasound characterize attenuation as the “half-value layer,” or the “half-power distance.” These terms refer to the distance that ultrasound will travel in a particular tissue before its amplitude or energy is attenuated to half its original value. Attenuation • • • • Divergence of the wavefront Elastic reflection of wave energy Elastic scattering of wave energy Absorption of wave energy Ultrasound Attenuation Material Water Blood Soft tissue except muscle Bone Air Lung Half–power distance (cm) 380 15 5 to 1 1 to 0.6 0.7 to 0.2 0.08 0.05 Attenuation in Tissue • Ultrasound energy can travel in water 380 cm before its power decreases to half of its original value. Attenuation is greater in soft tissue, and even greater in muscle. Thus, a thick muscled chest wall will offer a significant obstacle to the transmission of ultrasound. Non-muscle tissue such as fat does not attenuate acoustic energy as much. The halfpower distance for bone is still less than muscle, which explains why bone is such a barrier to ultrasound. Air and lung tissue have extremely short half-power distances and represent severe obstacles to the transmission of acoustic energy. Attenuation • As a general rule, the attenuation coefficient is doubled when the frequency is doubled. I avg I 0 exp 2 z Pressure Radiated by Sharp Pulse Beam Forming • Ultrasound beam can be shaped with lenses • Ultrasound transducers (and other antennae) emit energy in three fields – Near field (Fresnel region) – Focused field – Far field (Fraunhofer region) Directing Ultrasound with Lens Beam Focusing • A lens will focus the beam to a small spot according to the equation lf d 2.44 D Linear Array Types of Probes Modern Electronic Beam Direction Beam Direction (Listening) Wavefronts Add to Form Acoustic Beam Phased Linear Array A-mode Ultrasound Amplitude of reflected signal vs. time A-mode M-mode Ultrasound M-mode B-mode Ultrasound Fan forming B-mode Example Cardiac Ultrasound Standard Sites for Echocardiograms Conventional Cardiac 2D Ultrasound Short-axis Interrogation B-mode Image of Heart Traditional Ultrasound Images End-diastole End-systole B-mode Ventricles Mitral stenosis Geometric problems New developments of Phase-arrays 2D Probe Elements Recent 2D array • 5Mz 2D array from Stephen Smith’s laboratory, Duke University 2D and 3D Ultrasound a. Traditional 2D b, c. New views possible with 3D 3D Pyramid of data 3D Ultrasound • • • • 2D ultrasound transmitter 2D phased array architecture Capture 3D volume of heart 30 volumes per second 3D Ultrasound Traditional 2D New 3D Real-time 3D Ultrasound Real-time 3D Ultrasound Velocity of Contraction Normal Abnormal Normal artery Progression of Vascular Disease CAD Severe re-canalization Intravascular Ultrasound (IVUS) • Small catheter introduced into artery • Catheter transmits and receives acoustic energy • Reflected acoustic energy used to build a picture of the inside of the vessel • Clinical assessment based on vessel image IVUS Catheter • • • • 1 - Rotating shaft 2 - Acoustic window 3 - Ultrasound crystal 4 - Rotating beveled acoustic mirror Slightly Diseased Artery in Cross-section Plaque Catheter An array of Images 3D IVUS Doppler Principle Doppler Doppler measurements fDc V 2 f cos f D Doppler shift f Excitation frequency c Speed of sound in tissue Angle of excitation Doppler angle Normal flow Diseased flow Blood Flow Measurements