Scanheads that were developed in the late 1970's and early 1980's for imaging human tissue are still useful for many ultrasound imaging applications. A transducer located in the scanhead comprises discs of piezoelectric material, which when excited electrically vibrated at a frequency usually chosen to be between 2 and 10 MHz. At these frequencies, the vibrational energy of the transducer was directional and radiated from two faces of a thin circular disc in reasonably well-defined beams. In general, the energy radiating from the back of the transducer is absorbed by a suitable material while that from the front is coupled to the patient by a fluid capable of transmitting ultrasound energy with low loss characteristics. Emerging through a thin, low-loss cap, the energy is further coupled to the patient with a sonolucent gel applied to the patient's skin. Echoes resulting from the interaction of the ultrasound energy with body tissue traverse the same path in reverse, and when they strike the transducer generate an electrical signal whose strength is a function of the echogenicity of a target within the patient and the target's depth below the patient's skin. The location in depth is determined from the time interval between the transmit pulse and the received echo. With this information and the directional information delivered by a position encoder coupled to the transducer, the scanheads generate a gray-scale image of the tissue lying in a scan plane within the patient, which is refreshed and updated with every sweep of the transducer across the image plane. Two sweeps of the transducer comprises one operating cycle, referred to as 1 Hz, and equates to two frames per second.
Two dimensional ultrasound images (also known as B-scans) are made up of a number of adjacent lines of ultrasound data called A-scans, which are acquired from the scanhead through successive sweeps of the transducer. The line of ultrasound data is acquired when a transducer transmits the ultrasound pulse into the tissue being studied and then receives the ultrasound signal reflected by the tissue along a beam axis of the transducer. The lines of ultrasound data are located within the same plane and are usually spaced at constant intervals. Each line of data is acquired with the ultrasound beam axis moved laterally within the plane by a known incremental distance. The ultrasound image may have a linear format, in which the lines are parallel to one another and equally spaced, or a sector format, in which the lines radiate from an apex with equal angles between them. To produce a linear format image, the transducer is moved laterally, without altering the angle between the transducer and the line along which it is moved. To produce a sector format image, the transducer is mounted to a fixture, which rotates about an apex, causing the transducer to move in an arc. As the transducer moves, the position within the scan plane is tracked so that an associated ultrasound system can display the ultrasound line data at the correct locations within the displayed image.
Early clinical diagnostic ultrasound systems used wobbler scanheads to produce the sector format images. These systems used low frequency ultrasound, in the 2 to 5 MHz range. The wobbler scanheads usually consisted of the transducer located within a fluid filled chamber, a motor, a position encoder, and an acoustic window through which the ultrasound passed. The motor drive mechanism usually moved the transducer through an arc, resulting in a sector scan type image format while the position encoder kept track of the transducer position. The wall of the fluid filled chamber, which faced the tissue being imaged, acted as an acoustic window, which was usually made of a hard plastic material. This window allowed ultrasound to pass through with little attenuation. Further, in general, there is a reflected ultrasound wave which does not pass through the window. This wave can reverberate between the transducer and the window several times before dissipating. The reverb components, which strike the transducer, can cause an undesirable artifact in the ultrasound image. The magnitude of the reflected wave is determined by the acoustic impedance mismatch between the material used for the window and the fluid in the transducer chamber. The amount of attenuation is determined by the window material, which occurs as the ultrasound energy passes through the window. Both attenuation and reflections at the window are undesirable.
In the 80's these mechanically scanned transducers began to be replaced by solid state devices which consist of a plurality of narrow piezoelectric elements which, when excited sequentially, can be used to build up an image. These “linear array” scanheads had been developed at the same time as the mechanical ones, but delivered poorer image quality. Further work, throughout the 80's and 90's resulted in the development of “phased array” scanheads, which have the ability to excite groups of elements in ways that allows electronic beam steering and focusing, which in general produce better images than any mechanical scanhead and at frame rates of 60 frames per second. Today, phased arrays are universally used for ultrasound imaging of human tissue. However, a typical phased array system using a transducer operating at five MHz might have a spatial resolution of 0.5 mm.
One disadvantage with higher operating frequencies is as the operating frequency increases, fabrication difficulties make it challenging to build a phased array type imaging system. As a result, current systems operating in the 30-40 MHz range typically use mechanically scanned single element transducers, in scanheads similar in operating principal to the mechanically scanned systems described above. However, high frequencies generally result in higher attenuation and thus the attenuation due to an acoustic window is increased significantly. Accordingly, current high frequency transducers use a non-encapsulated transducer, which is moved back and forth with a linear servo-motor and position encoder system. At higher frequencies (greater than 30 MHz), transducer encapsulation is impractical due to a breakdown of theoretical properties and characteristics of materials with higher frequencies.
For high frequency transducers, since it is not encapsulated, the moving transducer is exposed. Acoustic coupling to the tissue being imaged is accomplished by creating a mound of ultrasound gel on the surface of the tissue, into which the moving transducer is lowered. Satisfactory imaging depends on the existence of a continuous layer of gel between the transducer and the tissue. If the transducer loses contact with the gel, or if an air bubble forms on the surface of the transducer, imaging will be compromised or even impossible. This type of imaging is restricted to relatively low frame rates, because a rapidly moving transducer will disrupt the gel layer and is more likely to lose contact. Further disadvantages of exposed transducers are that they can create a hazard to delicate tissue, and can also expose the transducer to possible damage from impact.
A further disadvantage in mechanical ultrasound scanheads is the use of moving magnet motors. The attraction of the moving magnet type is that there is no need for flexible wires to deliver power to the drive coil because the drive coil is stationary and the permanent magnet is attached to the moving member or rotor. Furthermore, the magnet type motor is inefficient. The usual mechanical scanhead consumes up to three Watts of electrical power, which is converted into heat that must be dissipated through plastic walls of the scanhead housing. As the housing is generally a poor conductor of heat the internal temperature of the scanhead may rise, which in time can degrade materials, alter the acoustic properties of the device, and can even be uncomfortable to the subject. Another reason the magnet motor is inefficient is that in an effort to keep the oscillating mass low, the moving magnets are kept relatively small. To achieve a certain torque, motor currents are correspondingly high, which gives rise to a high I^2R loss. These losses increase roughly as the square of the scanning rate.
In one embodiment, the high-frequency, high frame-rate ultrasound imaging system comprises a scan head having a transducer capable of generating ultrasound energy at a frequency of at least 20 megahertz (MHz), and a processor for receiving ultrasound energy and for generating an ultrasound image at a frame rate of at least 15 frames per second (fps).
Related methods of operation are also provided. Other systems, methods, features, and advantages of the high-frequency, high frame-rate ultrasound imaging system will be or become apparent to one with skill in the art upon examination of the following figures and detailed description. It is intended that all such additional systems, methods, features, and advantages be included within this description, be within the scope of the high-frequency, high frame-rate ultrasound imaging system, and be protected by the accompanying claims.
The high-frequency, high frame-rate ultrasound imaging system can be better understood with reference to the following figures. The components within the figures are not necessarily to scale, emphasis instead being placed upon clearly illustrating the principles of the high-frequency, high frame-rate ultrasound imaging system. Moreover, in the figures, like reference numerals designate corresponding parts throughout the different views.
Referring to
Referring again to
The ultrasound system 131 includes a control subsystem 127, a scan converter 129, the transmit subsystem 118, the receive subsystem 120 and the user input device 136. The processor 134 is coupled to the control subsystem 127 and the display 116 is coupled to the processor 134. A memory 121 is coupled to the processor 134. The memory 121 can be any type of computer memory, and is typically referred to as random access memory “RAM,” in which the software 123 of the high-frequency, high frame-rate ultrasound imaging system executes.
The high-frequency, high frame-rate ultrasound imaging system can be implemented using a combination of hardware and software. The hardware implementation of the high frequency, high frame-rate ultrasound imaging system can include any or a combination of the following technologies, which are all well known in the art: discrete electronic components, a discrete logic circuit(s) having logic gates for implementing logic functions upon data signals, an application specific integrated circuit having appropriate logic gates, a programmable gate array(s) (PGA), a field programmable gate array (FPGA), etc.
The software for the high frequency, high frame-rate ultrasound imaging system comprises an ordered listing of executable instructions for implementing logical functions, and can be embodied in any computer-readable medium for use by or in connection with an instruction execution system, apparatus, or device, such as a computer-based system, processor-containing system, or other system that can fetch the instructions from the instruction execution system, apparatus, or device and execute the instructions.
In the context of this document, a “computer-readable medium” can be any means that can contain, store, communicate, propagate, or transport the program for use by or in connection with the instruction execution system, apparatus, or device. The computer readable medium can be, for example but not limited to, an electronic, magnetic, optical, electromagnetic, infrared, or semiconductor system, apparatus, device, or propagation medium. More specific examples (a non-exhaustive list) of the computer-readable medium would include the following: an electrical connection (electronic) having one or more wires, a portable computer diskette (magnetic), a random access memory (RAM), a read-only memory (ROM), an erasable programmable read-only memory (EPROM or Flash memory) (magnetic), an optical fiber (optical), and a portable compact disc read-only memory (CDROM) (optical). Note that the computer-readable medium could even be paper or another suitable medium upon which the program is printed, as the program can be electronically captured, via for instance optical scanning of the paper or other medium, then compiled, interpreted or otherwise processed in a suitable manner if necessary, and then stored in a computer memory.
The memory 121 also includes the image data obtained by the ultrasound system 100. A computer readable storage medium 138 is coupled to the processor for providing instructions to the processor to instruct and/or configure processor to perform steps or algorithms related to the operation of the ultrasound system 131, as further explained below. The computer readable medium can include hardware and/or software such as, by way of example only, magnetic disks, magnetic tape, optically readable medium such as CD ROM's, and semiconductor memory such as PCMCIA cards. In each case, the medium may take the form of a portable item such as a small disk, floppy diskette, cassette, or it may take the form of a relatively large or immobile item such as hard disk drive, solid state memory card, or RAM provided in the support system. It should be noted that the above listed example mediums can be used either alone or in combination.
The ultrasound system 131 includes a control subsystem 127 to direct operation of various components of the ultrasound system 131. The control subsystem 127 and related components may be provided as software for instructing a general purpose processor or as specialized electronics in a hardware implementation. The ultrasound system 131 includes a scan converter 129 for converting the electrical signals generated by the received ultrasound echoes to data that can be manipulated by the processor 134 and that can be rendered into an image on the display 116. The control subsystem 127 is connected to a transmit subsystem 118 to provide an ultrasound transmit signal to the ultrasound probe 106. The ultrasound probe 106 in turn provides an ultrasound receive signal to a receive subsystem 120. The receive subsystem 120 also provides signals representative of the received signals to the scan converter 129. The receive subsystem 120 is also connected to the control subsystem 127. The scan converter 32 is directed by the control subsystem 127 to operate on the received data to render an image for display using the image data 110.
The ultrasound system 131 transmits and receives ultrasound data through the ultrasound probe 106, provides an interface to a user to control the operational parameters of the imaging system 100, and processes data appropriate to formulate still and moving images that represent anatomy and/or physiology. Images are presented to the user through the interface display 116.
The human-machine interface 136 of the ultrasound system 131 takes input from the user, and translates such input to control the operation of the ultrasound probe 106. The human-machine interface 136 also presents processed images and data to the user through the display 116.
Referring to
Referring to
Further referring to
Referring again to
Referring to
Referring to
Referring to
Referring to
The position encoder 128 used in the scanhead 106 is, for example, an optical encoder capable of 1 micron (μm) resolution. The position encoder 128 works in conjunction with a reticulated tape strip referred to herein as the encoder code track 12. The position encoder 128 makes use of an optical sensor to count the passage of reticules on the encoder code track 12 as they pass a sensor associated with the position encoder 128. The sensor can sense both direction of travel of the proximal end 150 of the pivot tube 6, and track the position of the travel of the distal end 152 of the pivot tube 6 to within 1 micron.
Referring again to
The transducer 8 can be a high-frequency single-element focused piezoelectric ultrasonic transducer, with a frequency greater than 30 MHz and can be around 40 MHz. The transducer 8 receives the RF electrical pulse 104 as input and produces an ultrasonic acoustic pulse 104 as output during the transmit phase of operation of the circuit 102 (see
The pivot tube 6 can be an ultra light weight stainless steel tube fixed by the bearing assembly 4 in such a way that it pivots about its midpoint 154. The transducer 8 is connected to one end of the pivot tube 6, while the encoder code track 12 is connected to the other end of the pivot tube 6. The pivot tube 6 houses the coils of the torque motor 130 between the bearing assembly 4 and the encoder code track 12, thus forming an integral part of the torque motor 130. Made of tubing, the pivot tube 6 also acts as a conduit for the transducer coax cable 8a.
Referring to
The flexible seal 19 can be attached to the midpoint of the pivot tube 6, and the rear of the nose piece 20 bayonet quick release assembly comprising the locking plate 34 and the two screws 34a. The seal 19 can be made of an elastomer membrane that is fastened so that it forms a fluid tight seal between the pivot tube 6 and the nosepiece 20. The seal 19 separates the fluid filled nosepiece 20 from the remainder of the housing which remains dry.
Two Hall sensors 13 are placed in the housing of the scanhead 106 so that they sense the travel of the pivot tube 6 past their respective sensors 13. The sensors 13 are placed so that they produce a signal at the maximum safe travel of the torque motor 130. The limit switches 13 are also placed symmetrically about the pivot point 154 so that they can be used to home the system to a zero deflection, homed, or normal position.
The hollow cavity 15 in the nose piece 20 can be fluid filled. The nosepiece 20 provides a mounting structure to which the acoustic window 125 can be attached. The nosepiece 20 features a drain/fill screw as a fill port 35 through which fluid may be added or removed from the cavity 15. The nosepiece 20 can contain part of a bayonet style quick release assembly allowing it to be removed and changed quickly without the need for tools, while ensuring a fluid tight seal.
The acoustic window 125 comprises a thin membrane of a material well acoustically matched to the fluid in the cavity 15. The acoustic window 125 can be held in a position so that it remains close to and normal to the face of the transducer 8 over the full extent of transducer travel (approximately 0.5 mm to 1 mm, for example). Material from which to form the acoustic window were initially selected or rejected based on known bulk acoustic properties. The membrane can be chosen to exhibit acoustic impedance in the range of 1.3 to 1.7 megaRayles (MRayles), such as 1.5 megarayles. Mechanical constraints such as the manner in which the membrane is attached affect the acoustic impedance and the resulting suitability for use as the acoustic window 125. Material from which the acoustic window can be fabricated include polyester films ranging in thickness from about 0.9 um to 4.5 μm, polytetrafluoroethylene (PTFE) in thicknesses of 5 μm, 10 μm, 15 μm, and 25 μm, low density polyethylene (LDPE) in thicknesses of 15 μm, 25 μm, and 50 μm, polycarbonate in a thickness of 2 μm, polypropylene in a thickness of 4 μm, latex elastomer in a thickness of 60 μm, and silicone elastomer in a thickness of 25 μm were tested in a variety of configurations including varying the angle of incidence of the ultrasound beam to the membrane forming the acoustic window 125 from 90 degrees to 110 degrees. These materials and thicknesses were used with transducer frequencies of 30-40 MHz. Thinner membranes could be used as the frequency increases. In addition, the encapsulated coupling fluid can be varied to improve the acoustic match with the membrane of the acoustic window 125. For example, ethylene glycol, triethylene glycol, water, light paraffin oil and various aqueous solutions of glycols can be used. Water as a coupling fluid and a 25 μm thick membrane of LDPE can be used as the membrane for the acoustic window 125. Further, an acoustic window 125 formed of 5 μm thick or 15 μm thick PTFE are provided. In addition, thin silicone elastomer can also be provided for the membrane forming the acoustic window 125. The acoustic window 125 maintains a fluid tight seal between the nosepiece 20 and the outer environment of the scanhead 106. Accordingly, the acoustic window 125 used with a high frequency ultrasound transducer 8 is thin, and can be composed of a material that has an acoustic impedance very close to that of the fluid in the cavity 15.
The electronics circuit 102 provides both a low noise RF preamplifier and a proprietary high fidelity protection circuit to the scanhead 106. The electronics circuit 102 protects sensitive receive instruments in the receive subsystem 120 from the high energy pulse 104 used to drive the transducer 8. The low-noise preamplifier boosts the signal of the transducer 8 with minimal distortion.
Referring again to
For example, M-mode and Doppler are two other modes of operation for which the scanhead 106 is suited. For either of these modes, the rotor assembly 5 is electrically driven to a fixed position, usually under operator control using a joystick associated with the human-machine interface 136 for input commands. The operator (not shown) can view an image frozen in time on the display 116, or a series of images, which are periodically updated, and manipulate the direction in which the transducer 8 is pointing. An electronic representation 144 (
Further, the torque motor 130 in conjunction with the position encoder 29 and encoder code track 12 run in a closed loop. They act as a servo-motor and are controlled by a motor control system associated with the processor 134 so that the pivot tube 6, which can be fixed in place by the pivot bearings 4, rotates back and forth about the pivot axis 154 in a controlled manner. The transducer 8 can be fixed to the end of the pivot tube 6 opposite the encoder code track 12. The pivot tube 6 moves the transducer 8, which is scanned back and forth within the fluid filled nosepiece 20. The location of the transducer 8 is known at all times to within 1 micron. The transducer 8 transmits and receives ultrasonic information which is received and amplified via the circuit 102, and then sent to the processor 134. Due to the light-weight precision nature of the design, this process can be accomplished at 15 Hz allowing for the production of real-time images for display of the image data 110 on the display 116. Operating the transducer 8 at a frequency of 15 Hz equates to a frame rate of 30 frames per second, as two sweeps of the transducer 8 through its range of motion equates to one Hz. Further, the oscillating frequency of the transducer 8 may be increased to increase the frame rate. Further, depending on the frequency of the ultrasound energy transmitted by the transducer, the ultrasound system 131 provides images having a spatial resolution of less than 30 microns. For example, at a frequency of approximately 25 MHz, the spatial resolution is approximately 75-100 microns. As the transducer frequency increases, the spatial resolution improves. At high transducer frequencies in the range of 40 MHz to 60 MHz, spatial resolution may exceed 30 microns. The high operating frequency of the transducer and the precise mechanical positioning of the transducer with an accuracy of approximately 1 μm allow the ultrasound system 131 to provide real-time ultrasound images having spatial resolution in excess of 30 μm.
Further, the scanhead 106 can be designed for use either by hand or on a fixture. The scanhead 106 can also be used as an immersion style scanner in a water bath or it can be coupled with gel to the tissue to be scanned. In these situations, the membrane of the acoustic window 125 may be removed.
In summary, the scanhead 106 is an electrically driven handheld imaging device that oscillates the ultrasound transducer 8 in a fan-shaped arc while maintaining good acoustic coupling between the transducer 8 and the subject 108 being imaged. The position encoder 128 delivers real-time position information to the controlling system processor 134. As the transducer 8 moves, signals from the position encoder 128 trigger transmit pulses 104 and communicate to the system processor 134 the position at which the resulting data stream 110 collected between those pulses 104 should be displayed in the electronic image that comprises the visual output on the display 116. The scanhead 106 can move the transducer 8 continuously back and forth within a fluid environment over a distance of approximately 10 mm in a controlled manner at a rate up to and exceeding 15 Hz, which corresponds to a frame rate of 30 frames per second. The position encoder 128 in the scanhead 106 can record the position of the transducer 8 in real time with an accuracy of 1 μm, and can position the transducer 8 at an arbitrary location within the scan region to an accuracy of 1 μm. The scanhead 106 includes the acoustic window 125 through which the ultrasound energy can be directed towards the subject 108 being imaged. The acoustic window 125 allows the transmission of high frequency ultrasound with minimum attenuation and/or reflection. The scanhead 106 can be sufficiently compact to be easily hand held, and can achieve positioning accuracy to 1 μm with a 15 Hz mechanical pivoting scanning and positioning system. The acoustic window 125 can be compatible with the transmission of high frequency ultrasound energy, at frequencies in excess of 60 MHz. The scanhead 106 can have image resolution smaller than 30 μm, with an imaged region of approximately 8 mm by 8 mm for the scan plane 112 (see
The scanhead 106 uses a single moving part, the pivot tube 6, and a limited angle torque motor 130 of the moving coil type. The torque motor 130 produces large torque force with little current draw because the non-moving field magnets 28 and 28a are relatively large and are made of a high energy product material, such as, but not limited to, neodymium iron-boron, which maintains a very high B field across the rotor windings 24. Another benefit of using a moving coil type motor is that the rotor mass, and rotational inertia, can be minimized, which helps to reduce power consumption and vibration. Small structures within the subject 108 being imaged at 40 MHz or greater are often associated with rapid movement. Therefore, such a design allows for operating speeds of 30 Hz or higher, corresponding to 60 frames per second.
The flex seal 19 (see
The portion of the pivot tube 6 immersed in the acoustic fluid, and the transducer 8, which can be wholly immersed, can be designed to be neutrally buoyant. When in motion, neutral buoyancy helps cancel vibration that could otherwise be a consequence of the motion of the transducer 8 and pivot tube 6. In fact, in another embodiment of the present invention, the entire oscillating mechanism on either side of the pivot point 154 can be so adjusted to be neutrally buoyant and operates entirely immersed in the acoustic fluid. This can help to eliminate virtually all vibration that would otherwise be transmitted to the operator and the subject 108.
Further, the nosepiece 20 can be easily removed and replaced by the operator. The simplified removal and replacement of the nosepiece 20 facilitates the replacement of a damaged acoustic window 125 or contaminated acoustic fluid. The fill port can be provided on the side of the nosepiece 20 to initially fill the cavity 15 with acoustic fluid when the nosepiece 20 is installed and to displace any bubbles with additional fluid should they develop with use. A simple bayonet type twist lock can be used to secure the nosepiece 20 to the body of the scanhead 106. If the nosepiece 20 should be sterile, as it might for some uses, it can be disposable. An integral part of such a replaceable nosepiece 20 can be a sterile drape or sheath, made of thin plastic, heat sealed or otherwise attached to the base of the nosepiece 20, which could be an injection molded plastic part. The scanhead 106 can also be operated, if desired, with the acoustic window 125 removed.
Referring to
Another embodiment of the scanhead 106 is shown in
The chassis 215 supports a pivot frame 208 that in turn supports a yolk 212 attached to armature 240 (
A bayonet style lock plate 205a interfaces with a fixture on a nose 205 that is mounted to the pivot frame 208. The lock plate 205a is attached to a removable nosepiece 201a. The nosepiece 201a has an acoustic window including a membrane 201b mounted at one end thereof. The nosepiece 201a surrounds a coupling fluid cavity 201c. The assembly comprising the nosepiece 201a and lock plate 205a is mounted onto the scan head 206 via the bayonet style lock system.
The coupling fluid cavity 201c surrounds a transducer 202a, which is attached to the support arm 203. The transducer 202a is connected to a transducer coaxial cable 202b, which is connected at the opposite end to the circuit board 224. The nosepiece 201a includes a fill port to fill the coupling fluid cavity 201c with a coupling fluid. The fill port is sealed by a fill port screw 204. A molded rubber seal 207 is mounted on the support arm 203 and disposed between the fluid cavity 201c and a pivot frame 208.
A bearing assembly including a bearing preload screw 209, precision radial ball bearings 208a, and a fixing screw 210a affixes the armature assembly 240, to the pivot frame 208, with low radial drag and virtually no radial or axial play. A yoke 212 is provided straddling the support arm 203 and fixed to the rotor 218 with rotor adhesive pins 214.
A partial assembly 250 of the scan head 206 shown in
As shown in
A case comprising a case top 233, a case bottom 234 and a case gasket 228 provides a fluid-tight seal around the internal components of the scan head 206. The case top 233 and case bottom 234 as well as the case gasket 228 are coated with an electrically conductive coating 251 to improve RF shielding.
Referring to
The encoder code track 219 is made from a spring steel substrate. The encoder code track 219 can be installed using a technique which avoids prebending of the encoder code track 219. Prebending may damage the encoder code track 219. Two encoder code track retainers 230a hold the encoder code track 219 at each end, forcing the spring steel to take the exact curvature of the rotor 218. The encoder track retainers 230a are fixed in place using screws 230b. Alternatively, a light string may be tied around screws 230b and adhered, using, for example, a glue, to the ends of the encoder code track 219
The scanhead 206 of this embodiment provides a sweep angle greater than 22 degrees included. The sweep angle refers to the motion of the transducer 202a defined by the Hall sensor 13, the two Hall sensor magnets 26 and 26a, and the limit switches 221a. In addition to the increased sweep angle due to the removable support arm 203, the length of the support arm 203 may be changed, during manufacture or after, such as during field service, to accommodate different imaging requirements. The support arm 203 can be a length such that the transducer 202a is approximately 20 percent farther from the pivot point 154 than the encoder code track 219 (see
The scan head 206 in this embodiment is assembled on the rigid chassis 215. The scan head 206 can be assembled to complete functionality on the chassis 215 so that testing can be performed without the case 233, 234 in place. The design of the chassis 215 therefore allows verification of wire routing and strain relief, electrical inspection, tuning of the optical encoder read head 220, and function verification of the limit switches 221a.
Referring to
Referring to
The scanhead 206 includes an integral circuit board 224 that integrates motor control functions, position monitoring functions, and the transmission and reception of RF signals. In addition, the circuit board 224 houses the optical limit switches 221a. The circuit board 224 can be prefabricated and tested. The circuit board 224 allows the routing of the transducer coaxial cable 202b and the motor wires 232 to be made with a minimal drag on the motor by placing the connection points nearly over the pivot point.
The case 233, 234 can be non-load bearing and can be a purely protective part of the scanhead 206. It serves to waterproof and keep the internal components of the scanhead 206 free of contamination. The case 233, 234 can be secured to the chassis 215 by screws. Alternatively, the two halves 233, 234 of the case may be glued, or otherwise adhered, together to make the scanhead 206 tamper and water resistant.
The nosepiece 201a may include a disposable acoustic window. Referring to
As shown in
The acoustic window 330 can be designed to overcome the specific challenges of encapsulating a high frequency high-resolution ultrasonic probe in a variety of demanding environments. The acoustic window 330 provides an inexpensive means for protecting the transducer and allowing imaging in a sterile environment without unduly compromising acoustic performance. The acoustic window 330 can be constructed from a molded plastic frame comprising a fluid tight mechanical snap-on attachment structure. The acoustic window 330 can be a molded, disposable element, which ‘snaps’ onto a permanent machined nosepiece, yielding the fluid filled encapsulated nose of the probe. Tools are not required to remove or attach the acoustic window to the nosepiece. For example, the shape of the acoustic window permits attachment to the nosepiece of the transducer using a simple rolling motion. The acoustic window can be any shape depending upon the nosepiece to be covered. A thin film of a sonolucent material forms a membrane 352 that can be attached to the front face of a frame 350. The frame 350 and the membrane 352 comprise the acoustic window 330.
The characteristics and thickness of the material forming the membrane of the acoustic window are chosen to suit the characteristics of the specific probe to be encapsulated. Sonolucent materials, for example those disclosed in U.S. Pat. Nos. 5,479,927; 5,983,123; and 6,574,499, which are incorporated by reference in their entireties, can be used to produce the membrane 352 of the acoustic window 330. In one aspect, the sonolucent material can be a polyester, a polycarbonate, an acrylic, a thermoplastic elastomer, or a silicone elastomer. Examples of sonolucent materials include, but are not limited to, Surlyn® ionomers, such as Surlyn® 8940, and Kapton®, available from E.I. Du Pont de Nemours and Company, Wilmington, Del.; polymethyl pentenes, such as TPX® MX-002, TPX® 95 and MX-004, available from Mitsui & Co., Tokyo, Japan; Teflon®, Mylar®, polyethylene, such as low density polyethylene, polycarbonate, polypropylene, and various polyurethane films. In one embodiment, the sonolucent material can be extruded to a certain thickness and heat welded to the frame 350 of the acoustic window 330 to form a fluid tight seal. The thickness of the membrane 352 will vary depending upon the sonolucent material selected. In one aspect, the membrane 352 has a thickness of less than or equal to 25 μm. In another embodiment, the thickness of the membrane 352 can range from 1 μm to 25 μM. The technology used for sealing the membrane 352 to the frame 350 will vary depending on the sonolucent material selected. Examples of methods for sealing the membrane 352 to the frame 350 include, but are not limited to, adhesives, welding techniques (e.g., RF, ultrasonic, and thermal), and mechanical seals.
Referring to
For environments requiring complete isolation of the probe from the surroundings, a sheathed version of the acoustic window 330 includes a heat sealed sheath 340 of polyethylene film that can be designed to fit back over the probe and up the cable. The sheath can be formed as part of the disposable acoustic window 330, so that when sterilization is desired the entire window and sheath can be removed and discarded.
In an alternative embodiment, the high-frequency, high frame-rate ultrasound imaging system may be used to image a syringe, catheter, or other invasive element inserted into a subject.
In block 404, the ultrasound energy is transmitted by the transmit subsystem 118 into the subject 114 (
In block 408, the received ultrasound is processed by the processor 134 and the scan converter 129, under the direction of the software 123, to generate an image on the display 116. The image has a frame rate of at least 15 frames per second (fps).
Although the high-frequency, high frame-rate ultrasound imaging system has been described with reference to certain specific embodiments, various modifications thereof will be apparent to those skilled in the art without departing from the scope of the high-frequency, high frame-rate ultrasound imaging system as outlined in the claims appended hereto.
This application is a continuation of U.S. application Ser. No. 11/776,401, filed on Jul. 11, 2007, which is a continuation of U.S. application Ser. No. 10/683,890, filed on Oct. 10, 2003, now U.S. Pat. No. 7,255,678, which claims the benefit of U.S. Provisional Application No. 60/417,164, filed on Oct. 10, 2002; U.S. Provisional Application No. 60/468,958, filed on May 9, 2003; U.S. Provisional Application No. 60/468,956, filed on May 9, 2003; and U.S. Provisional Application No. 60/470,234, filed on May 14, 2003, each of which is hereby incorporated by reference.
Number | Name | Date | Kind |
---|---|---|---|
3886490 | Green | May 1975 | A |
3955561 | Eggleton | May 1976 | A |
3974826 | Eggleton et al. | Aug 1976 | A |
4034744 | Goldberg | Jul 1977 | A |
4065976 | Taenzer et al. | Jan 1978 | A |
4092867 | Matzuk | Jun 1978 | A |
4141347 | Green et al. | Feb 1979 | A |
4143554 | Nagy et al. | Mar 1979 | A |
4231373 | Waxman et al. | Nov 1980 | A |
4276491 | Daniel | Jun 1981 | A |
4282755 | Gardineer et al. | Aug 1981 | A |
4316271 | Evert | Feb 1982 | A |
4375818 | Suwaki et al. | Mar 1983 | A |
4399703 | Matzuk | Aug 1983 | A |
4407293 | Suarez, Jr. et al. | Oct 1983 | A |
4412147 | Nagura et al. | Oct 1983 | A |
4421118 | Dow et al. | Dec 1983 | A |
4424813 | Havlice et al. | Jan 1984 | A |
4431007 | Amazeen et al. | Feb 1984 | A |
4442715 | Brisken et al. | Apr 1984 | A |
4489729 | Sorenson et al. | Dec 1984 | A |
4524623 | Terwilliger | Jun 1985 | A |
4546771 | Eggleton et al. | Oct 1985 | A |
4612937 | Miller | Sep 1986 | A |
4649925 | Dow et al. | Mar 1987 | A |
4664123 | Iinuma | May 1987 | A |
4722346 | Chen | Feb 1988 | A |
4796632 | Boyd et al. | Jan 1989 | A |
4867169 | Machida et al. | Sep 1989 | A |
4893013 | Denen et al. | Jan 1990 | A |
5079752 | Bloomfield | Jan 1992 | A |
5099847 | Powers et al. | Mar 1992 | A |
5105814 | Drukarev et al. | Apr 1992 | A |
5119342 | Harrison, Jr. et al. | Jun 1992 | A |
5161536 | Vilkomerson et al. | Nov 1992 | A |
5192549 | Barenolz et al. | Mar 1993 | A |
5278757 | Hoctor et al. | Jan 1994 | A |
5313949 | Yock | May 1994 | A |
5313950 | Ishikawa et al. | May 1994 | A |
5318033 | Savord | Jun 1994 | A |
5329194 | Dow et al. | Jul 1994 | A |
5357963 | Mayol et al. | Oct 1994 | A |
5379642 | Reckwerdt et al. | Jan 1995 | A |
5379772 | Imran | Jan 1995 | A |
5402789 | Dow et al. | Apr 1995 | A |
5412854 | Lockwood et al. | May 1995 | A |
5456256 | Schneider et al. | Oct 1995 | A |
5474074 | Suorsa et al. | Dec 1995 | A |
5485845 | Verdonk et al. | Jan 1996 | A |
5488954 | Sleva et al. | Feb 1996 | A |
5505088 | Chandraratna et al. | Apr 1996 | A |
5513640 | Yamazaki et al. | May 1996 | A |
5524623 | Liu | Jun 1996 | A |
5588434 | Fujimoto | Dec 1996 | A |
5588435 | Weng et al. | Dec 1996 | A |
5615680 | Sano | Apr 1997 | A |
5629865 | Roth | May 1997 | A |
5636632 | Bommannan et al. | Jun 1997 | A |
5647364 | Schneider et al. | Jul 1997 | A |
5651366 | Liang et al. | Jul 1997 | A |
5655537 | Crowley | Aug 1997 | A |
5678552 | Savord | Oct 1997 | A |
5690110 | Tanaka | Nov 1997 | A |
5724312 | Oppelt | Mar 1998 | A |
5776068 | Silverman et al. | Jul 1998 | A |
5792058 | Lee et al. | Aug 1998 | A |
5839442 | Chiang et al. | Nov 1998 | A |
5844140 | Seale | Dec 1998 | A |
5865650 | Marian, Jr. et al. | Feb 1999 | A |
5879305 | Yock et al. | Mar 1999 | A |
5921931 | O'Donnell et al. | Jul 1999 | A |
6001062 | Masters | Dec 1999 | A |
6036647 | Suorsa et al. | Mar 2000 | A |
6042545 | Hossack et al. | Mar 2000 | A |
6055861 | Banta, Jr. et al. | May 2000 | A |
6063030 | Vara et al. | May 2000 | A |
6064628 | Uhlendorf et al. | May 2000 | A |
6066099 | Thomenius et al. | May 2000 | A |
6073045 | Dyson et al. | Jun 2000 | A |
6139502 | Fredriksen | Oct 2000 | A |
6152877 | Masters | Nov 2000 | A |
6186963 | Schwarze et al. | Feb 2001 | B1 |
6193662 | Hwang | Feb 2001 | B1 |
6198956 | Dunne | Mar 2001 | B1 |
6201900 | Hossack et al. | Mar 2001 | B1 |
6221016 | Hayakawa | Apr 2001 | B1 |
6228030 | Urbano et al. | May 2001 | B1 |
6228031 | Hwang et al. | May 2001 | B1 |
6241672 | Hochman et al. | Jun 2001 | B1 |
6245017 | Hashimoto et al. | Jun 2001 | B1 |
6251073 | Imran et al. | Jun 2001 | B1 |
6261231 | Damphousse et al. | Jul 2001 | B1 |
6267734 | Ishibashi et al. | Jul 2001 | B1 |
6312382 | Mucci et al. | Nov 2001 | B1 |
6315725 | Masters | Nov 2001 | B1 |
6315732 | Suorsa et al. | Nov 2001 | B1 |
6325759 | Pelissier | Dec 2001 | B1 |
6344023 | Fukukita et al. | Feb 2002 | B1 |
6346079 | Haider et al. | Feb 2002 | B1 |
6360027 | Hossack et al. | Mar 2002 | B1 |
6379304 | Gilbert et al. | Apr 2002 | B1 |
6406428 | Mittelstaedt | Jun 2002 | B1 |
6491637 | Foster et al. | Dec 2002 | B2 |
6494835 | Ciezki et al. | Dec 2002 | B1 |
6508768 | Hall et al. | Jan 2003 | B1 |
6511430 | Sherar et al. | Jan 2003 | B1 |
6530887 | Gilbert et al. | Mar 2003 | B1 |
6540681 | Cheng et al. | Apr 2003 | B1 |
6544187 | Seward | Apr 2003 | B2 |
6547731 | Coleman et al. | Apr 2003 | B1 |
6558326 | Pelissier | May 2003 | B2 |
6569102 | Imran et al. | May 2003 | B2 |
6572549 | Jong et al. | Jun 2003 | B1 |
6574499 | Dines et al. | Jun 2003 | B1 |
6579122 | Chen | Jun 2003 | B1 |
6589174 | Chopra et al. | Jul 2003 | B1 |
6629929 | Jago et al. | Oct 2003 | B1 |
6679845 | Ritter et al. | Jan 2004 | B2 |
6837855 | Puech | Jan 2005 | B1 |
6923767 | Saied et al. | Aug 2005 | B2 |
6949071 | Saied et al. | Sep 2005 | B1 |
7255678 | Mehi et al. | Aug 2007 | B2 |
20010031922 | Weng et al. | Oct 2001 | A1 |
20020007119 | Pelissier | Jan 2002 | A1 |
20020050169 | Ritter et al. | May 2002 | A1 |
20020128550 | Van Den Brink et al. | Sep 2002 | A1 |
20020173719 | Zhao et al. | Nov 2002 | A1 |
20020173720 | Seo et al. | Nov 2002 | A1 |
20030088182 | He et al. | May 2003 | A1 |
20030097068 | Hossack et al. | May 2003 | A1 |
20030100833 | He et al. | May 2003 | A1 |
20030114755 | Jong et al. | Jun 2003 | A1 |
20040082858 | Fukuda et al. | Apr 2004 | A1 |
20040111026 | Schoenfeld | Jun 2004 | A1 |
20040176789 | Lee et al. | Sep 2004 | A1 |
20040193048 | Tsoref | Sep 2004 | A1 |
20040193054 | Leblanc et al. | Sep 2004 | A1 |
20040225215 | Querleux et al. | Nov 2004 | A1 |
20040236219 | Liu et al. | Nov 2004 | A1 |
20050010111 | Kristoffersen | Jan 2005 | A1 |
20050070796 | Tsujita | Mar 2005 | A1 |
20050124894 | Puech | Jun 2005 | A1 |
20050131289 | Aharoni et al. | Jun 2005 | A1 |
20050154287 | Schluter | Jul 2005 | A1 |
20050154305 | Kamiyama | Jul 2005 | A1 |
20050240102 | Rachlin et al. | Oct 2005 | A1 |
Number | Date | Country |
---|---|---|
0727963 | Jun 2005 | EP |
WO-9427501 | Dec 1994 | WO |
WO-2004007098 | Jan 2004 | WO |
WO-2004034694 | Apr 2004 | WO |
Entry |
---|
Gniadecka, M. et al, “Age-related diurnal changes of dermal oedeme: evaluation by high-frequency ultrasound,” British Journal of Dermatology 131:849-855 (1994). |
Gniadecka, M., et al. “Effects of ageing on dermal echogenicity,” Skin Research and Technology, 7:204-207 (2001). |
Harland, C.C., et al. “Differentiation of common benign pigmented skin lesions from melanoma by high-resolution ultrasound,” British Journal of Dermatology 143:1-10 (2000). |
Lucassen, G.W., et al. “The effectiveness of massage treatment on cellulite as monitored by ultrasound imaging,” Skin Research and Technology, 3:154-160 (1997). |
Seidenari, S., et al. “Ultrasound B scanning with image analysis for assessment of allergic patch test reactions,” Contact Dermatitis 24:216-222 (1991). |
Seidenari, S., et al. “Echographic Evaluation with Image Analysis of Normal Skin: Variations according to Age and Sex,” Skin Pharmacal, 7:201-209 (1994). |
Serup, J. “‘Ten Years’ Experience with High-Frequency Ultrasound Examination of the Skin: Development and Refinement of Technique and Equipment,” Ultrasound in Dermatology, Berlin: Springer, 41-54 (1992). |
Berson et al. “High frequency ultrasonic devices: advantages and applications,” European Journal of Ultrasound, 10:53-63 (1999). |
Erickson et al., Institute of Electrical and Electronics Engineers: “A hand-held, high frequency ultrasound scanner.” 2001 IEEE Ultrasonics Symposium Proceedings, Atlanta, GA; Oct. 7-10, 2001. IEEE Ultrasonics Symposium Proceedings, New York, NY: IEEE, US vol. 2 of 2, Oct. 7, 2001. |
Turnbull et al. “In vivo ultrasound biomicroscopy in developmental biology,” Trends in Biotechnology, 20(8): S29-S33 (2002). |
Berson et al. “High-Resolution Real-Time Ultrasonic Scanner,” Ultrasound in Med. & Biol., vol. 18, No. 5, pp. 471-478, 1992. |
International Searching Authority, International Search Report, PCT Application PCT/US2003/032320, mailed Apr. 28, 2004, 2 pages. |
International Searching Authority, Preliminary Examination Report, PCT Application PCT/US2003/032320, completed Sep. 21, 2006, 3 pages. |
European Patent Office, Supplementary Partial European Search Report, EP Application 03776327.3, dated Dec. 16, 2004, 7 pages. |
European Patent Office, Supplementary Partial European Search Report, EP Application 03776327.3, dated Mar. 14, 2005, 7 pages. |
European Patent Office, Examination Report, EP Application 03776327.3, mailed Jul. 18, 2005, 5 pages. |
European Patent Office, Examination Report, EP Application 03776327.3, mailed Feb. 21, 2006, 4 pages. |
European Patent Office, Examination Report, EP Application 03776327.3, mailed Oct. 27, 2006, 6 pages. |
European Patent Office, Decision of Technical Board of Appeal, EP Application 03776327.3, mailed Oct. 19, 2011, 18 pages. |
Number | Date | Country | |
---|---|---|---|
20110021919 A1 | Jan 2011 | US |
Number | Date | Country | |
---|---|---|---|
60417164 | Oct 2002 | US | |
60468958 | May 2003 | US | |
60468956 | May 2003 | US | |
60470234 | May 2003 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 11776401 | Jul 2007 | US |
Child | 12769419 | US | |
Parent | 10683890 | Oct 2003 | US |
Child | 11776401 | US |