Chapter 1 Introduction
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Equipment Considerations and Image Formation
One of the primary physical components of an ultrasound machine is the transducer, which is connected by a cable to the other components, including the image screen or monitor and the computer processing unit. The transducer is placed on the skin surface and determines the imaging plane and structures that are imaged. Ultrasound is a unique imaging method in that sound waves are used rather than ionizing radiation for image production. An essential principle of ultrasound imaging relates to the piezoelectric effect of the ultrasound transducer crystal, which allows electrical signal to be changed to ultrasonic energy and vice versa. An ultrasound machine sends the electrical signal to the transducer, which results in the production of sound waves. The transducer is coupled to the soft tissues with acoustic transmission gel, which allows transmission of the sound waves into the soft tissues. These sound waves interact with soft tissue interfaces, some of which reflect back toward the skin surface and the transducer, where they are converted to an electrical current used to produce the ultrasound image. At soft tissue interfaces between tissues that have significant differences in impedance, there is sound wave reflection, which produces a bright echo. A sound wave that is perpendicular to the surface of an object being imaged will be reflected more than if it is not perpendicular. In addition to reflection, sound waves can be absorbed and refracted by the soft tissue interfaces. The absorption of a sound wave is enhanced with increasing frequency of the transducer and greater tissue viscosity.1
An important consideration in ultrasound imaging is the frequency of the transducer because this determines image quality. A transducer is designated by the range of sound wave frequencies it can produce, described in megahertz (MHz). The higher the frequency, the higher the resolution of the image; however, this is at the expense of sound beam penetration as a result of sound wave absorption.1 In contrast, a low-frequency transducer optimally assesses deeper structures, but it has relatively lower resolution. Transducers may also be designated as linear or curvilinear (Fig. 1-1). With a linear transducer, the sound wave is propagated in a linear fashion parallel to the transducer surface (Video 1-1). This is optimum in evaluation of the musculoskeletal system to assess linear structures, such as tendons, to avoid artifact. A curvilinear transducer may be used, although less commonly in evaluation of deeper structures because this increases the field of view (Video 1-2), or it may provide guidance of a needle for biopsy or aspiration. A small footprint linear probe is very important for imaging the hand, ankle, and foot given the contours of these body parts that allow only limited contact with the probe surface (see Fig. 1-1C). A small footprint transducer with an offset is helpful when performing procedures on the distal extremities.
Scanning Technique
To produce an ultrasound image, the transducer is held on the surface of the skin to image the underlying structures. Ample acoustic transmission gel should be used to enable the sound beam to be transmitted from the transducer to the soft tissues and to allow the returning echoes to be converted to the ultrasound image. I prefer a layer of thick transmission gel over a more cumbersome gel standoff pad. Gel that is more like liquid consistency is also less ideal because the gel tends not to stay localized at the imaging site. The transducer should be held between the thumb and fingers of the examiner’s dominant hand, with the end of the transducer near the ulnar aspect of the hand (Fig. 1-2A). It is very important during imaging to stabilize or anchor the transducer on the patient with either the small finger or the heel of the imaging hand (see Fig. 1-2B). This technique is essential to maintain proper pressure of the transducer on the skin, to avoid involuntary movement of the transducer, and to allow fine adjustments in transducer positioning. Remember that the sound beam emitted from the transducer is focused relative to the short end of the transducer, and side-to-side movement of the transducer should only be a millimeter at a time.
Various terms describe manual movements of the transducer during scanning. The term heel-toe is used when the transducer is rocked or angled along the long axis of the transducer (Fig. 1-3A). The term toggle is used when the transducer is angled from side to side (see Fig. 1-3B). With both the heel-toe and toggle maneuvers, the transducer is not moved from its location, but rather the transducer is angled. The term translate is used when the transducer is moved to a new location while maintaining a perpendicular angle with the skin surface. The term sweep is used when the transducer is slid from side to side while maintaining a stable hand position, similar to sweeping a broom.
Image Appearance
Once the transducer is placed on the patient’s skin with intervening gel, a rectangular image (when using a linear transducer) appears on the monitor. The top of the image represents the superficial soft tissues that are in contact with the transducer, and the deeper structures appear toward the lower aspect of the image (Fig. 1-4). To understand the resulting ultrasound image, consider the sound beam as a plane or slice that extends down from the transducer along its long axis. It is this plane that is portrayed on the image. The left and right sides of the image can represent either end of the transducer, and this can usually be switched by using the left-to-right invert button on the ultrasound machine or by simply rotating the transducer 180 degrees. When imaging a structure in long axis, it is common to have the proximal aspect on the left side of the image and the distal aspect on the right.
Image optimization is essential to maximize resolution and clarity. The first step is to select the proper transducer and frequency. Higher-frequency transducers (10 MHz or greater) optimally evaluate superficial structures, whereas lower-frequency transducers are used for deep structures. Linear transducers are typically used, unless the area of interest is deep, such as the hip region, where a curvilinear transducer may be chosen. After the proper transducer is selected and placed on the patient, the next step is to adjust the depth of the sound beam; this is accomplished by a button or dial on the ultrasound machine. The depth of the sound beam is adjusted until the structure of interest is visible and centered in the image (Fig. 1-5A and B). The next step in optimization with many ultrasound machines is to adjust the focal zones of the ultrasound beam, if present on the ultrasound machine. This feature is typically displayed on the side of the image as a number of cursors or other symbols. It is optimum to reduce the number of focal zones to span the area of interest because increased focal zones will decrease the frame rate that produces a windshield-wiper effect. It is also important to move the depth of the focal zones to the depth where the structure is to be imaged to optimize resolution (see Fig. 1-5C). Some ultrasound machines have a broad focal zone that may not have to be moved. Finally, the overall gain can be adjusted by a knob on the ultrasound machine to increase or decrease the overall brightness of the echoes, which is in part determined by the ambient light in the examination room (see Fig. 1-5D). The gain should ideally be set where one can appreciate the ultrasound characteristics of normal soft tissues (as described later).
Sonographic Appearances of Normal Structures
Normal musculoskeletal structures have characteristic appearances on ultrasound imaging.2 Normal tendons appear hyperechoic with a fiber-like or fibrillar echotexture (see Fig. 1-4).3 At close inspection, the linear fibrillar echoes within a tendon represent the endotendineum septa, which contain connective tissue, elastic fibers, nerve endings, blood, and lymph vessels.3 Continuous tendon fibers are best appreciated when they are imaged long axis to the tendon. On such a long axis image, by convention the proximal aspect is on the left side of the image, with the distal aspect on the right. Normal muscle tissue appears relatively hypoechoic (Fig. 1-6). At closer inspection, the hypoechoic muscle tissue is separated by fine hyperechoic fibroadipose septa or perimysium, which surrounds the hypoechoic muscle bundles. The surface of bone or calcification is typically very hyperechoic, with posterior acoustic shadowing and possibly posterior reverberation if the surface of the bone is smooth and flat (see Fig. 1-6). The hyaline cartilage covering the articular surface of bone is hypoechoic and uniform (Fig. 1-7A and B), whereas the fibrocartilage, such as the labrum of the hip and shoulder, and the knee menisci are hyperechoic (see Fig. 1-7B). Ligaments have a hyperechoic, striated appearance that is more compact compared with tendons (Fig. 1-8). In addition, ligaments are also identified in that they connect two osseous structures. Often normal ligaments may appear relatively hypoechoic when surrounded by hyperechoic subcutaneous fat; however, a compact linear hyperechoic ligament can be appreciated when imaged in long axis perpendicular to the ultrasound beam.