Ultrasound Imaging Systems

Ultrasound Imaging Systems1.1 INTRODUCTIONAn ultrasonography scans also cognise as ultrasonography. Ultrasound allow for form the image by scanning using the high frequency sound flutters. This device suitable to evaluate rough part inside of the body. In physics, ultrasound is a sound with a frequency humans cannot hear. In diagnostic sonography, the ultrasound is vernacularly between 2 and 18 MHz. (Anon 2012)2.0 THE ULTRASOUND IMAGING SYSTEMFigure 1 The principal turn tailal comp iodinents of an ultrasound imaging system.(Perry Sprawls n.d.)2.1 TRANSDUCERThe ultrasound transducer converts an electrical auspicate into the ultrasound ray of light. The signal transmitted into the patients body, and then alters the returning echo into an electrical signal for processing and display. It use single-element circular disk to both transmit and start out ultrasound. (Hedrick et al. 2005)2.1.1 CONSTRUCTION OF TRANSDUCERCrystal of piezoelectric material with electrodes is the main part of the transducer. The electrodes ar formed by plating a thin film of gold or silver on the crystal surface. The matching layer is located adjacent to the electrodes. The lean is to improve the deportation of brawn to and from the patient. All this part of the transducer is placed in an electrically insulating casing. This casing will give structural support. An acoustical insulator is made of rubber or cork it works to prevents the transmission of ultrasound dynamism into the casing. (Hedrick et al. 2005)2.1.1.1 PIEZOELECTRIC MATERIALSWhen we change the transducer it will change the frequency too. A higher frequency transducer that produces a shorter wave length has a thinner crystal. Normally the material that always virtually used in transducer is lead zirconate titanate (PZT). PZT represents a piezoelectric ceramics with various extracts. It will change the properties to equal a particular application. In medical, PZT-5 is used because it has the properties of high el ectromechanical coupling coefficient, high dielectric constant, and ability to be formed in a particular size and shape. (Hedrick et al. 2005)2.1.1.2 BACKING MATERIALThe functions of backing material will deliver the utmost amount of susceptibility in the form of heat to the patient. This is will give a continuous output of ultrasound waves from the transducer. The other function is to absorb all the energy except for the whizz cycle of sound. Meanings that one that produced from the front face of the transducer. Backing materials should have acoustic resistivity so that maximum energy transfer will occur. Besides that, backing material should have a high absorption coefficient. This is to prevent ultrasonic energy from reentering the crystal. In the backing material, they will use an epoxy resin and tungsten powder combination to damp the ultrasonic wink. Next, the rear surface of the backing materials is one-sided to prevent reflection of sound energy into the crystal. (Hedr ick et al. 2005)2.1.1.3 MATCHING LAYERThe matching layer is placed in the transducer on the exit side of the crystal. This material with acoustic impedance is placed between the crystal and the patient. The function of the acoustic impedance to produced ultrasonic energy to be largely reflected at this interface. This creates a long pulse and reduces the beam impregnation that enters the patient, which is we did not want it in the ultrasound. The reason why we need the matching layer is to shorten the pulse and the improve energy transfer across the crystal- wander interface. However, the matching layer must have low-loss properties since high attenuation would stabilize the desired effect of high transmission. (Hedrick et al. 2005)2.2 PULSE GENERATORThe pulse reservoir produces the electrical pulses. The size of the electrical pulses can be used to change the intensity and energy of the ultrasound beam. (Perry Sprawls n.d.)2.3 AMPLIFICATIONAfter the echo is stimulated by the tra nsducer, amplification is used to intensification the size of the electrical pulses. Gain setting will controls the amount of amplification. The time gain compensation function is to alter the increase in relationship to the distance of echo sites inside the body. (Hedrick et al. 2005)2.4 SCAN GENERATORControlling the scanning of the ultrasound beam is done by the scan generator. The way is by control the procedure when electrical pulses are functional to the piezoelectric elements in the transducer. (Perry Sprawls n.d.)2.5 IMAGE PROCESSORThe digital imageis to produce the chosenforms for display. This includes giving it specific contrast characteristics and reformatting the image. (Perry Sprawls n.d.)2.6 vauntingThe digital ultrasound images are observed on the monitor and transmitted to work station. The other part of the ultrasound system is the digital storage device. The function is to store images for later viewing.(Perry Sprawls n.d.)3.0 THE ULTRASOUND PULSEFigure 3 The pro duction of the ultrasound pulse. (Perry Sprawls n.d.)4.0 ULTRASOUND CHARACTERISTIC4.1 FREQUENCYFrequency is the number of wave cycles departure a given point in a given increase of time. The unit is cycles/ second or hertz. Frequency is the inverse of the period. (Hedrick et al. 2005)Figure 4 The ultrasound pulse frequency. (Perry Sprawls n.d.)4.2 VELOCITYVelocity is the consecrate and direction at which sound propagates through a medium. The average velocity of sound in soft tissue is 1540 m/s. (Hedrick et al. 2005)Figure 5 The ultrasound of velocity. (Perry Sprawls n.d.)4.3 WAVELENGTHWavelength is a physical characteristic of a wave that is the distance for one complete wave cycle. (Hedrick et al. 2005)Figure 6 The wavelength of the ultrasound. (Perry Sprawls n.d.)4.4 AMPLITUDEAmplitude used to refer to the particle displacement, particle velocity or acoustic pressure of a sound wave. Amplitude also manoeuvre the strength of the detected echo or the voltage induced in a crys tal by a pressure wave. (Hedrick et al. 2005)5.0 INTENSITY AND POWER durability is a physical parameter that describes the amount of energy flowing through a unit cross-sectional area of a beam severally second. This is the rate at which the wave transmits the energy everyplace a small area. The unit of intensity is the watt per public square centimeter or joule per second per square centimeter. (Hedrick et al. 2005)Power is a measure of the total energy transmitted jibemed over the entire cross-sectional area of the beam per unit time. The unit of power is the watt. (Hedrick et al. 2005)5.1 secular CHARACTERISTICSAs the transducer emits pulses, it causes large instabilities of intensity in the region through which the pulse move. Each pulse consists of multiple cycles that produce intensity variations indoors the pulse itself-the maximum intensity, designated temporal peak (TP). Pulse average (PA) will controls the intensity averaged over the duration of a single pulse. Tempo ral average (TA) will controls the intensity averaged over the longer interval of the pulse repetition period. The TA intensity is related to the PA intensity by the duty factor (DF)TA = DFPA or by the pulse duration (PD) and pulse repetition frequency (PRF)TA =PD PRF PA.(Hedrick et al. 2005)5.2 SPATIAL CHARACTERISTICSThe maximum intensity of all measured values at bottom the sound field is designated as the spatial peak (SP). The designation of spatial peak is not well-defined. In some applications it refers to the maximum intensity in a plane perpendicular to the beam axis at a particular distance from the transducer. The maximum intensity throughout the ultrasonic field which usually occurs along the beam axis. The tensioning of the transducer is the most important determinant of spatial peak.(Hedrick et al. 2005)5.3 TEMPORAL/SPATIAL COMBINATIONSpatial averaging over the cross-sectional area of the beam for each temporal intensity is also specified. A cutoff point of 0.25 tim es the SP intensity has been established to the limit area over which the intensity is averaged. These three combinations are possible to happen are I(SATP)-spatial average, temporal peak intensity, I(SAPA)-spatial average, pulse average intensity and I(SATA)-spatial average, temporal average intensity.(Hedrick et al. 2005)6.0 INTERACTIONS OF ULTRASOUNDFigure 7 The interaction within a body of ultrasound (Perry Sprawls n.d.).6.1 ABSORPTION AND ATTENUATIONAbsorption is the procedure whereby energy is placed in a medium by converting ultrasonic energy into other energy forms, primarily heat. It is an exponentially decreasing function and is the major factor in the total attenuation of the beam. (Hedrick et al. 2005)Attenuation is the decrease in intensity as a sound beam travels through the medium. Attenuation depends on all the interactions of ultrasound with tissues which include scattering, divergence, and absorption. (Hedrick et al. 2005) Scattering is the rerouting of sound energ y resulting from the sound beam striking an interface whose physical dimension is less than one wavelength. It is also called non specular reflection. (Hedrick et al. 2005)6.2 REFLECTIONReflection is an interaction that results when the sound being redirected into the medium later on striking an acoustic interface. The angle of incidence equals the angle of reflection. The intensity of the reflected wave is depends on the com correct of the interface. (Hedrick et al. 2005)6.3 REFRACTIONRefraction is a process whereby sound enters one medium from another that will result in a bending or deviation of a sound beam from the predictable straight- place path. Refraction obeys Snells law, which is based on the ratio of the velocity of the sound in the respective media. Refraction will make artifacts in the image by the misregistration of structures (Hedrick et al. 2005)7.0 PULSE diam AND BEAM WIDTHA low-Q transducer has a short pulse length and a broad bandwidth while a high-Q transducer has a long pulse length and narrow bandwidth. The objectives beam width is to transmit a beam that would be directional with a narrow beam width. An echo is created anyway of the lateral position of the object in the ultrasonic field. The lateral dimension of the object in the image is defined as the same size as the beam width. ninefold small objects equidistant from the transducer are not resolved when encompassed by the beam. Focusing reduces the beam width at specific depth to enhance the spatial mapping of received echoes.(Ding et al. 2014) Sampling is restricted laterally by the width of the beam. Objects located outside the beam do not contribute signals. (Small 1971)7.1 TRANSDUCER centerSINGThe focusing transducer be with an indented active element exhibits much broader bandwidth and higher sensitivity. To fabricate focusing transducers, we can add a lens and determine the piezoelectric element. Among the focusing transducer designing methods, the shaping element used in transducers was reported to be much effective for fabricating high sensitivity device. Hard pressing and pressure defection techniques are the usual ways to shape transducer elements. For the flexible composite and polymer materials, the focusing transducer can be easily fabricated using those techniques.(Chen et al. 2013)Figure 8 The width and pulse diameter characteristics of both unfocused and focused transducer. (Perry Sprawls n.d.)7.2 ADJUSTABLE TRANSMIT FOCUSTransmit focusing happen when the depth of the focal zone is altered by vary the delay times between crystal excitations. (Wright 1997)The scanning of the region of interest is conducted with a depth of focus selected by the operator. After review of the real-time image, a new focal zone may be certain to rescan the same area with dissimilar focusing in the scan plane. The beam is focused to a new depth simply by changing the delay times. The transducers that have the capabilities of this focusing are phased linear arr ays. (Kossoff Eng 2000)Electronic phasing of the elements allows variable focusing along the scan line which in turn controls beam width in the plane direction. High resolution images with multiple focal zones throughout the images are also possible using this adjustment delay lines. Multi zone transmit focusing reduces the frame rate, because the data must be composed for all the lines of sight across the array with a set focal zone depth before the lines of sight are repetitive with a different focal zone depth.7.3 DYNAMIC RECEIVE FOCUSDynamic focusing is in the receive mode. It does will reduce the effective sampling volume.(Kossoff Eng 2000) Dynamic focusing will operate at all depths. The wave front from the object appears to be in phase for all the crystals resulting in a focused beam from the depth of interest. Beam formation is the delay and sum of strategy. The master synchronizer sends timing messages to the receiver-delay lines to indicate the elapsed time from transmis sion to reception. The elapsed time determines the delay times for each crystal. The depth for receive focus is always known, and thus receive-delay times are constantly changed to yield continually focused beam at all depths. During acquisition of image data the receive times delays are varied dynamically to sweep the focal zone to each point along the scan line. (Hedrick et al. 2005)8.0 CONCLUSIONIn ultrasound, high frequencies extend better quality images, but cannot penetrate through skin and organ deeply. Low frequencies can penetrate deeper, but the image quality is poor. Ultrasound is effectual to view part inside of the body. They may also be useful in helping the surgeon when carrying out some types of biopsies. Ultrasound is a one of the safe procedure in imaging department.