Embodiments described herein relate generally to a magnetic resonance imaging device and a gradient coil.
Magnetic resonance imaging is an imaging method of magnetically exciting a nuclear spin of a subject placed in a static magnetic field with a radio frequency (RF) pulse of the Larmor frequency, and generating an image from data of a magnetic resonance signal generated due to the excitation.
In such magnetic resonance imaging, a temperature of a metal shim (for example, an iron shim) arranged in a gradient coil tends to be increased in high-resolution imaging or high-speed imaging. The iron shim is essentially arranged to correct nonuniformity of the static magnetic field. However, when the temperature of the iron shim is increased, a center frequency of the static magnetic field may be affected because magnetic susceptibility is changed. Specifically, the iron shim arranged near the center in a long axis direction of the gradient coil acts to raise the center frequency when the temperature is increased, and the iron shim arranged near an end in the long axis direction acts to lower the center frequency when the temperature is increased.
An imaging region is near the center in the long axis direction, and it receives a large influence especially from a temperature rise in the iron shim arranged near the imaging region, which may cause deterioration in fat suppression or deterioration in image quality such as N/2 artifact in echo planar imaging (EPI) and image distortion. Unfortunately, piping of a cooling pipe in a gradient coil in the related art still cannot suppress the temperature rise in the iron shim arranged near the center in the long axis direction.
A magnetic resonance imaging device according to an embodiment includes a static magnetic field magnet that generates a static magnetic field, and a gradient coil in which a cooling pipe is laid. The cooling pipe is laid so as to preferentially cool a part near a uniform region in which uniformity of the static magnetic field is kept.
With reference to the drawings, the following describes a magnetic resonance imaging device (hereinafter, appropriately referred to as a “magnetic resonance imaging (MRI) device”) and a gradient coil according to embodiments. The embodiments are not limited to the following embodiments. Content described in each of the embodiments can be similarly applied to other embodiments in principle.
The static magnetic field magnet 101 is a magnet formed into a hollow, substantially cylindrical (including an elliptical) shape, and generates a static magnetic field in a space inside the substantially cylindrical shape. The static magnetic field magnet 101 is, for example, a superconducting magnet, and is excited by receiving an electric current supplied from the static magnetic field power supply 102. The static magnetic field power supply 102 supplies the electric current to the static magnetic field magnet 101. The static magnetic field magnet 101 may also be a permanent magnet. In this case, the MRI device 100 does not necessarily include the static magnetic field power supply 102. The static magnetic field power supply 102 may be provided separately from the MRI device 100.
The gradient coil 103 is a coil that is arranged on the inner side of the static magnetic field magnet 101 and formed into a hollow, substantially cylindrical shape. The gradient coil 103 receives the electric current supplied from the gradient magnetic field power supply 104, and generates a gradient magnetic field. The gradient coil 103 will be described in detail later. The gradient magnetic field power supply 104 supplies the electric current to the gradient coil 103.
The RF coil 105 is arranged on the inner side of the gradient coil 103, and receives an RF pulse supplied from the transmitter 106 to generate a high-frequency magnetic field. The RF coil 105 receives a magnetic resonance signal (hereinafter, appropriately referred to as a “magnetic resonance (MR) signal”) emitted from the subject P due to influence of the high-frequency magnetic field, and outputs the received MR signal to the receiver 107.
The RF coil 105 described above is merely an example. The RF coil 105 may be configured by combining one or more of a coil having a transmission function alone, a coil having a reception function alone, and a coil having a transmission and reception function.
The transmitter 106 supplies, to the RF coil 105, an RF pulse corresponding to the Larmor frequency determined due to a type of a target atom and magnetic field intensity. The receiver 107 detects the MR signal output from the RF coil 105, and generates MR data based on the detected MR signal. Specifically, the receiver 107 digitally converts the MR signal output from the RF coil 105 to generate the MR data. The receiver 107 transmits the generated MR data to the sequence controller 120. The receiver 107 may also be provided on a base device side including the static magnetic field magnet 101, the gradient coil 103, and the like.
The couch 108 includes a couchtop on which the subject P is placed. For convenience of explanation,
The sequence controller 120 drives the gradient magnetic field power supply 104, the transmitter 106, and the receiver 107 to image the subject P based on sequence information transmitted from the calculator 130. In this case, the sequence information defines a procedure of imaging. The sequence information defines intensity of the electric current supplied from the gradient magnetic field power supply 104 to the gradient coil 103 and timing for supplying the electric current, intensity of the RF pulse supplied from the transmitter 106 to the RF coil 105 and timing for applying the RF pulse, timing when the receiver 107 detects the MR signal, and the like.
For example, the sequence controller 120 is an integrated circuit such as an application specific integrated circuit (ASIC) and a field programmable gate array (FPGA), or an electronic circuit such as a central processing unit (CPU) and a micro processing unit (MPU).
The sequence controller 120 drives the gradient magnetic field power supply 104, the transmitter 106, and the receiver 107 to image the subject P, receives the MR data from the receiver 107, and transfers the received MR data to the calculator 130.
The calculator 130 controls the entire MRI device 100. The calculator 130 performs reconstruction processing such as a Fourier transformation on the MR data transferred from the sequence controller 120 to generate an MR image and the like. For example, the calculator 130 includes a controller, a storage unit, an input unit, and a display unit. The controller is an integrated circuit such as an ASIC and an FPGA, or an electronic circuit such as a CPU and an MPU. The storage unit is a semiconductor memory element such as a random access memory (RAM) and a flash memory, a hard disk, an optical disc, or the like. The input unit is a pointing device such as a mouse and a trackball, a selection device such as a mode changeover switch, or an input device such as a keyboard. The display unit is a display device such as a liquid crystal display.
In the shim layer 103c, a plurality of (for example, twenty-four) shim tray insertion guides 103f are formed. As illustrated in
Although not illustrated in
In this manner, in the gradient coil 103, the cooling pipes are laid in intermediate layers of the gradient coil 103 with the shim layer 103c interposed therebetween to cool the iron shim arranged in the shim layer 103c and the entire gradient coil 103. For example, heat generated in the main coil 103a is shielded by the cooling pipe in the cooling layer 103d, and is hardly transmitted to the iron shim arranged in the shim layer 103c. For example, heat generated in the shield coil 103b is shielded by the cooling pipe in the cooling layer 103e, and is hard to transmit to the iron shim arranged in the shim layer 103c.
Next,
In the first embodiment, the cooling pipe is laid so as to preferentially cool a part near a uniform region in which uniformity of the static magnetic field is kept. Here, the uniform region is a region specific to the MRI device 100 that is defined when the static magnetic field magnet is designed, and is also referred to as an “imageable region” and the like. The uniform region is arranged near the center between the first end and the second end, that is, near the center in the long axis (z-axis) direction of the gradient coil 103, and is represented, for example, as a cylindrical region of 50 cm×50 cm×45 cm in the x-axis direction, the y-axis direction, and the z-axis direction, respectively. That is, the cooling pipe is laid so as to preferentially cool the part near the center in the long axis direction of the gradient coil 103.
Specifically, in the first embodiment, the cooling pipe is laid to be separated into two systems of cooling pipe as illustrated in
The other system is a second cooling pipe 20 that is laid in a spiral manner to extend straight from the second end toward the first end, and to bend near the center in the long axis direction to return to the second end. As illustrated in
In the piping of such cooling pipes, the cooling water supplied from the cooling device (not illustrated) is first branched at an inlet manifold 10a and flows into each of the three cooling pipes in the first cooling pipe 10. The cooling water flowed into the three cooling pipes is conveyed at the shortest distance to the part near the center in the long axis direction of the gradient coil 103 and is flown subsequently from the part near the center toward the first end in a spiral manner along the substantially cylindrical shape of the gradient coil 103. Thereafter the cooling water branched into the three cooling pipes merges again at an outlet manifold 10b, and returns to the cooling device.
Similarly, the cooling water supplied from the cooling device is first branched at an inlet manifold 20a and flows into each of the three cooling pipes in the second cooling pipe 20. The cooling water flowed into the three cooling pipes is conveyed at the shortest distance to the part near the center in the long axis direction of the gradient coil 103 and is flown subsequently from the part near the center toward the second end in a spiral manner along the substantially cylindrical shape of the gradient coil 103. Thereafter the cooling water branched into the three cooling pipes merges again at an outlet manifold 20b, and returns to the cooling device.
In the first embodiment, when the first cooling pipe 10 and the second cooling pipe 20 are made of conductive metal, each of the cooling pipes is connected to each manifold via a tube made of an insulating material. In this way, the tube made of an insulating material is provided between each cooling pipe and each manifold, which can prevent an electrically closed loop from being formed by each cooling pipe. A manifold made of an insulating material such as Teflon (registered trademark) and polyethylene terephthalate (PET) may be used in place of the manifold made of metal such as brass. In this case, the tube made of an insulating material is not required. In the first embodiment, the cooling pipe extending straight from the first end toward the part near the center in the long axis direction or from the second end toward the part near the center in the long axis direction is laid so as to be embedded in a groove provided between regions of the shim tray insertion guides 103f, for example.
As illustrated in
In this way, the cooling water having a low stable temperature supplied from the cooling device is conveyed from both of the first end and the second end to the part near the center in the long axis direction at the shortest distance to start cooling at this point, so that the part near the center is always cooled with the cooling water having a low stable temperature. As a result, a temperature rise is suppressed in the iron shim arranged near the center in the long axis direction of the gradient coil 103, and a constant temperature can be kept. Accordingly, an increase in a center frequency of the imaging region positioned near the center in the long axis direction can also be suppressed, so that an adverse effect on image quality can be reduced.
The iron shim arranged near the end of the gradient coil 103 can be heated with warm water the temperature of which is increased. However, the iron shim arranged at this position acts to reduce the center frequency when the temperature thereof is increased, so that the iron shim serves to suppress an increase in the center frequency in any case.
As described above, according to the first embodiment, the cooling pipe is laid so that the cooling water having a low temperature is conveyed to the part near the center in the long axis direction, so that the part near what is called the uniform region is preferentially cooled. Accordingly, a relative increase in the temperature near the imaging region can be suppressed to improve the image quality.
Different point from the piping conceptually illustrated in
In
Subsequently, the following describes a second embodiment. Similarly to the first embodiment, in the second embodiment, the cooling pipe is laid so as to preferentially cool the part near the uniform region in which the uniformity of the static magnetic field is kept. However, in the second embodiment, piping density is adjusted instead of adjusting the starting position of the spiral piping. The piping density means density of the number of windings in a certain range. When compared in the same range, the piping density increases as the number of windings increases, and the piping density decreases as the number of windings decreases.
The piping conceptually illustrated in
In short, in the second embodiment, laying the first cooling pipes 10 and the second cooling pipes 20 in a manner overlapped with each other near the uniform region increases the piping density around the uniform region, and strongly cools the part near the uniform region. On the other hand, for example, the pipes are intentionally “sparsely” wound near the end in the long axis direction to reduce the number of windings (the number of turns) of the cooling pipe and reduce the piping density.
As a result, the part near the center in the long axis direction is strongly cooled and the part near the uniform region is preferentially cooled, so that a relative increase in the temperature near the imaging region can be suppressed to improve the image quality. The part near the end in the long axis direction is not so cooled and may be heated in some cases, so that the center frequency is reduced. Thus an increase in the center frequency is suppressed.
As a result, also in this modification, the part near the center in the long axis direction is strongly cooled and the part near the uniform region is preferentially cooled, so that a relative increase in the temperature near the imaging region can be suppressed to improve the image quality. The part near the end in the long axis direction is not so cooled and may be heated in some cases, so that the center frequency is reduced. Thus an increase in the center frequency is suppressed.
With the magnetic resonance imaging device and the gradient coil according to at least one of the embodiments described above, a relative increase in the temperature near the uniform region can be suppressed to improve the image quality.
While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the inventions. Indeed, the novel embodiments described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the embodiments described herein may be made without departing from the spirit of the inventions. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the inventions.
Number | Date | Country | Kind |
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2013-041005 | Mar 2013 | JP | national |
This application is a continuation of PCT international application Ser. No. PCT/JP2014/055318 filed on Mar. 3, 2014 which designates the United States, incorporated herein by reference, and which claims the benefit of priority from Japanese Patent Application No. 2013-041005, filed on Mar. 1, 2013, the entire contents of which are incorporated herein by reference.
Number | Date | Country | |
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Parent | PCT/JP2014/055318 | Mar 2014 | US |
Child | 14812468 | US |