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| United States Patent | 5050607 |
| Link to this page | http://www.wikipatents.com/5050607.html |
| Inventor(s) | Bradley; William G. (Pasadena, CA);
Jones; Lawrence W. (San Marino, CA) |
| Abstract | A magnetic resonance (MR) imaging system includes a magnet for producing a
magnetic field to which a patient is subjected, a radio frequency (RF)
transmitter coupled to a body coil within the magnet, an RF receiver
coupled to a surface coil within the magnet and placed as close as
possible to tissue being analyzed by the MR imaging system, and a computer
controlled system for generating RF signals sent from the transmitter and
detected by the receiver for use in producing nuclear excitation and
corresponding detected induced currents in the surface coil sent to an
analog-to-digital converter and then to the computer for processing into
an image display of the tissue under analysis. A preferred embodiment of
the invention comprises surface coil apparatus for use in analyzing tissue
within a body cavity of the patient, and a preferred system for use in
analyzing the tissue of the prostate gland includes an elongated hollow
tube for transrectal insertion, and expandable balloon sealed to the
exterior of the tube, and a loop antenna surface coil wire secured to the
exterior wall of the balloon. Fluid pressure applied to the inside of the
tube and then to the interior of the balloon expands the balloon and
thereby expands opposite sides of the surface coil wire and holds the
surface coil antenna in a spaced apart expanded position useful in serving
as a means for obtaining high resolution imaging of prostatic tissue. |
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Title Information  |
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Drawing from US Patent 5050607 |
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High resolution magnetic resonance imaging of body cavities |
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| Publication Date |
September 24, 1991 |
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| Filing Date |
September 1, 1989 |
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| Parent Case |
Cross-Reference to Related Applications
This is a continuation of application Ser. No. 07/021,758, filed 03/04/87
now abandoned. |
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Title Information  |
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Claims  |
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We claim:
1. An MR imaging system which includes:
a magnet for producing a magnetic field to which a patient is subjected,
an RF transmitter coupled to a body coil within the magnet,
an RF receiver wherein RF signals generated by the RF transmitter are sent
from the RF transmitter and detected by the RF receiver,
a surface coil apparatus for use in producing high resolution MR images of
tissue within a body cavity of the patient, the surface coil apparatus
comprising:
(a) support means adapted for insertion into and withdrawal from said body
cavity;
(b) a flexible antenna wire mounted on the support means and having a
normal position in which portions of the antenna wire are spaced apart
from one another;
(c) means mounted on the support means for expanding said portions of the
antenna wire apart from one another to an expanded position wherein said
portions of the antenna wire are held in their expanded spaced apart
relation so that the expanded position of the antenna wire can be used for
detection of RF signals generated by said transmitter to produce an image
of body tissues located adjacent the antenna wire; and
(d) means for contracting said portions of the antenna wire to the normal
position for use in withdrawing the supporting means and the antenna wire
thereon from the body cavity;
the RF receiver being coupled to the antenna wire for detecting RF signals
induced in the antenna wire; and
processing means coupled to the RF receiver for converting the detected
signals induced in the antenna wire into an MR image display of the body
tissues located adjacent the antenna wire of the surface coil apparatus.
2. Apparatus according to claim 1 in which the means for expanding the
antenna wire comprises a fluid inflatable balloon positioned inside the
antenna wire.
3. Apparatus according to claim 2 including means for applying fluid
pressure to the inside of the balloon from a remote location.
4. Apparatus according to claim 3 in which the means for contracting the
antenna wire comprise means for depressurizing inside the balloon to
collapse the balloon.
5. Apparatus according to claim 2 in which the support means includes an
elongated tube, and including means for sealing the balloon to the wall of
the tube so the tube extends through the hollow interior of the balloon;
and in which the means for expanding the balloon includes means for
passing fluid under pressure into the tube and from the tube to the
interior of the balloon for expanding the balloon.
6. Apparatus according to claim 5 in which the antenna wire comprises a
loop antenna in which opposite portions of the loop extend through the
tube and pass out an end of the tube and then around opposite sides of the
outer wall of the balloon so that fluid under pressure passing into the
balloon expands the opposite portions of the loop antenna apart from one
another.
7. Apparatus according to claim 6 including a tuning and matching circuit,
the output of which is coupled to the RF receiver, and in which conductive
ends of the loop antenna are coupled to the tuning and matching circuit.
8. Apparatus according to claim 1 in which the MR imaging system includes a
tuning and matching circuit, and in which the body coil and antenna wire
are tuned and matched by the tuning and matching circuit.
9. Apparatus according to claim 1 in which said portions of the antenna
wire extend separately and axially along opposite sides of the support
means.
10. An MR imaging system which includes:
a magnet for producing a magnetic field to which a patient is subjected,
an RF transmitter coupled to a body coil within the magnet,
an RF receiver coupled to a surface coil apparatus within the magnet, the
surface coil apparatus providing means for obtaining high resolution MR
images of tissue within a body cavity of the patient, and wherein RF
signals generated by the RF transmitter are sent from the RF transmitter
and detected by the RF receiver, the surface coil apparatus comprising:
(a) an elongated narrow profile hollow tube adapted for insertion into and
withdrawal from the body cavity;
(b) an expandable balloon sealed to the exterior of the tube, the balloon
having a normal relaxed position generally matching the normal profile of
the tube and an expanded position spaced apart from the outer wall of the
tube;
(c) an antenna wire secured to the wall of the balloon so that portions of
the antenna wire extend at least on opposite sides of the balloon wall;
and
(d) means for applying fluid pressure to the inside of the tube and then to
the interior of the balloon to expand the balloon and thereby expand said
opposite portions of the antenna wire apart from one another to an
expanded position useful for serving as a detection coil for detecting the
RF signals generated by said RF transmitter for use in producing high
resolution imaging of adjacent tissue within said body cavity;
the receiver being coupled to the antenna wire for detecting the RF signals
induced in the antenna wire; and
processing means coupled to the RF receiver for converting the detected
signals induced in the antenna wire into an MR image display of the tissue
located within said body cavity adjacent the antenna wire.
11. Apparatus according to claim 10 in which the opposite portions of the
antenna wire are secured to diametrically opposed exterior wall portions
of the balloon.
12. Apparatus according to claim 11 in which the antenna wire is in the
configuration of a loop antenna.
13. Apparatus according to claim 10 in which the antenna wire comprises a
loop antenna in which opposite portions of the loop extend through the
tube and pass out an end of the tube and then around opposite sides of the
outer wall of the balloon so that fluid under pressure passing into the
balloon expands the opposite portions of the loop antenna apart from one
another.
14. Apparatus according to claim 13 in which conductive ends of the loop
antenna are coupled to a tuning and matching circuit of the MR imaging
system.
15. Apparatus according to claim 10 in which the MR imaging system includes
a tuning and matching circuit, and in which the body coil and antenna wire
are tuned and matched by the tuning and matching circuit.
16. Apparatus according to claim 10 in which said opposite portions of the
antenna wire extend separately and axially along opposite sides of the
balloon wall.
17. A method for obtaining high resolution MR imaging of the tissue within
a body cavity of a patient in an MR imaging system which includes a magnet
for producing a magnetic field to which the patient is subjected, an RF
transmitter coupled to a body coil within the magnet, an RF receiver
coupled to a surface coil within the magnet, and means for generating RF
signals sent from the transmitter and detected by the receiver for use in
producing an MR image display of a portion of the tissue within the body
cavity of the patient, the method comprising:
positioning a surface coil apparatus in the body cavity, wherein said
apparatus includes a flexible surface coil wire having a normal
low-profile position and an expanded position, the surface coil apparatus
being positioned with the surface coil wire in said normal position, and
thereafter expanding the surface coil wire to its expanded position,
wherein said expanded surface coil wire is useful in producing high
resolution imaging of the tissue in or adjacent to the body cavity when
serving as said surface coil for detection of RF signals in said MR
imaging system.
18. The method according to claim 17 in which the surface coil wire
comprises an MR surface coil antenna loop having diametrically opposite
sides expanded outwardly and retained in that position by outward pressure
applied from within the loop.
19. A method according to claim 18 in which the diametrically opposed sides
of the loop antenna are held spaced apart by a distance equal to at least
about the maximum width of the body tissue under diagnosis.
20. A method according to claim 18 in which the diametrically opposed sides
of the loop antenna are retained in their expanded position via an
expandable balloon to which the loop antenna is secured.
21. The method according to claim 20 in which the expandable balloon is
inflated to the expanded position remotely by fluid pressure, which can be
removed to return the balloon to its normal position for use in
withdrawing the surface coil apparatus from the body cavity of the
patient.
22. The method according to claim 17 including the step of maintaining the
surface coil wire expanded in a plane approximately parallel to the
coronal imaging plane of the prostate gland.
23. A method for obtaining high resolution MR imaging of the prostate gland
in an MR imaging system which includes a magnet for producing a magnetic
field to which a patient is subjected, an RF transmitter coupled to a body
coil within the magnet, an RF receiver coupled to a surface coil within
the magnet, and means for generating RF signals sent from the transmitter
and detected by the receiver for use in producing an MR image display of a
portion of the patient's prostate gland, the method comprising:
inserting a surface coil apparatus transrectally to a position adjacent the
patient's prostate gland wherein said apparatus includes a flexible
surface coil wire having a normal low profile position and an expanded
position, the surface coil apparatus being positioned with the surface
coil wire in said normal position, and
thereafter expanding the surface coil wire to its expanded position wherein
said expanded surface coil wire is useful in producing high resolution
imaging of the tissue in the prostate gland when serving as said surface
coil for detection of RF signals in said MR imaging system.
24. The method according to claim 23 in which the surface coil wire
comprises an MR surface coil antenna loop having diametrically opposite
sides, and including the step of expanding the opposite sides of the
antenna loop outwardly and retaining them in that position by outward
pressure applied from within the loop.
25. The method according to claim 24 including the step of maintaining the
diametrically opposed sides of the loop antenna spaced apart by a distance
equal to at least about the maximum width of the prostate gland.
26. The method according to claim 24 including the step of maintaining the
diametrically opposed sides of the loop antenna in their expanded position
via an expandable balloon to which the loop antenna is secured.
27. The method according to claim 26 including the step of inflating the
expandable balloon to the expanded position remotely by fluid pressure.
28. The method according to claim 27 including removing the fluid pressure
from the balloon to return the balloon to its normal position for use in
withdrawing the surface coil apparatus from the patient.
29. The method according to claim 23 including the step of maintaining the
surface coil wire expanded in a plane approximately parallel to the
coronal imaging plane of the prostate gland. |
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Claims  |
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Description  |
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FIELD OF THE INVENTION
This invention relates to magnetic resonance imaging, and more
particularly, to use of an improved surface coil for providing high
resolution magnetic resonance imaging of tissue in body cavities.
BACKGROUND OF THE INVENTION
In the background description to follow, the present invention is described
in relation to magnetic resonance (MR) imaging techniques used in the
examination and diagnosis of the prostate gland, although the invention
also may have application to MR imaging of tissues in other body cavities.
Carcinoma of the prostate is the second most common malignancy in the male
population, and it also has the second highest death rate. Diagnostic
blood tests for prostatic carcinoma are imperfect and the disease is often
well advanced by the time it is first diagnosed. The traditional methods
of diagnosing carcinoma of the prostate are mainly digital rectal
examination and estimation of serum acid phosphatase levels. The digital
examination remains the most useful diagnostic technique inasmuch as acid
phosphatase activity can be normal while the tumor is still confined to
the gland.
Sonographic examination has been reported to have good diagnostic results
in the detection of carcinoma. However, benign diseases such as benign
prostatic hypertrophy and chronic prostatitis can yield similar
sonographic appearances.
Magnetic resonance imaging has recently been shown to produce high quality
images of the human body. Briefly, MR imaging makes use of magnetic fields
and radio frequency waves to generate intensity-modulated images from
specific sections of the body. MR imaging systems generally include a
large magnet for generating a magnetic field. The patient being analyzed
is exposed to the magnetic field of the magnet. Hydrogen nuclei (protons)
in the magnetic field resonate when exposed to radio waves of a correct
frequency. For imaging purposes, the strong uniform magnetic field of the
magnet is selectively altered in one or more directions, preferably by
small magnetic fields produced by three separate gradient coils associated
with the magnet. Current passing through the gradient coils linearly
alters the magnetic field of the magnet in directions controlled by the
gradient coils. Signal transmission and reception are produced through use
of a radio frequency (RF) transmitter coupled to a transmitting coil or
antenna within the imaging unit and an RF receiver coupled to a receiving
coil or antenna also located in the imaging unit. The receiving coil is
positioned as close to the patient as possible for maximum imaging
sensitivity. The patient is often surrounded by a body coil which serves
both as a transmitting and receiving antenna. Alternatively, the body coil
can be used as a transmitting antenna only, and a separate surface coil is
used as a receiving antenna. The surface coil can usually be placed closer
to the tissues under examination than a single body coil. An RF oscillator
generates radio waves of different frequencies. By controlling the
magnetic field in a known way through a switching system that controls the
current in the gradient coils, and by generating radio waves of a select
frequency, the exact location at which the patient's body is imaged can be
controlled. When the frequency of the RF signal is set for the exact value
of the magnetic field, resonance occurs. Radio waves of the same frequency
are emitted from the portion of the patient being imaged, which induces
small currents in the receiving coil. The induced currents are detected to
produce an output signal dependent upon the number of protons involved in
the resonance and tissue-specific parameters T-1 and T-2. The variation in
proton density in different areas of the patient's body produces good
contrast in an MR image and is therefore useful in differentiating among
different tissues of the human body. The output signal from the RF
receiver is processed by a computer system to produce an image display so
that clinical diagnosis can be made by visual inspection of the displayed
image. The quality of the image display is critical. It is desirable to
obtain an image having high resolution so that clinical diagnosis can be
as precise as possible. High resolution imaging is also critical in
detecting tumor growth at its earlier stages where treatment of the
disease is still possible.
Use of a body coil as both the transmitter and receiver antenna yields MR
images of the body which can be useful in many clinical situations.
However, use of anatomically shaped surface coils for signal detection
yields images with higher signal-to-noise ratio in comparison to the usual
body coil. As a result, the surface coils yield MR images with much higher
sensitivity and therefore more detail in the critical anatomical areas.
Such surface coils are used for RF detection only and excitation is
produced by the standard body coil. These surface coils have been
successful in the past in obtaining reasonably good MR images for exterior
anatomical regions of the patient's body.
Use of a body coil (as both the transmitter and receiver coil) has not
yielded high resolution images of the prostate gland. Higher resolution
imaging of the prostate is desirable to obtain high detail images for
detecting prostatic carcinoma or benign prostatic hypertrophy at their
earlier stages. The prostate gland tissue has a capsule which forms an
outer wall of the gland. Present MR imaging techniques detect prostatic
carcinoma, but only after it is too far advanced, where the cancer has
passed through the capsule and invaded surrounding tissues. To date, MR
imaging techniques have not developed high resolution images that have
been shown to detect early malignant tumors within the prostate gland
routinely before they have passed through the outer capsule and invaded
surrounding structures.
The present invention provides an improved MR imaging system that produces
high resolution images of the prostate and tissues within other body
cavities. With the present invention, detection of prostatic carcinoma and
other malignant tumors at their earlier stages of growth is possible, when
compared with use of a single body coil as both the transmitter and
receiver in the MR imaging system.
SUMMARY OF THE INVENTION
Briefly, one embodiment of the invention comprises an improved surface coil
apparatus for use in an MR imaging system which includes a magnet for
producing a magnetic field to which a patient is subjected, an RF
transmitter coupled to a body coil within the magnet, an RF receiver
coupled to the surface coil, and means for generating RF signals sent from
the transmitter and detected by the receiver for use in producing an MR
image display of a portion of the patient's body. The improved surface
coil apparatus obtains high resolution MR images of tissues within a body
cavity of the patient. The apparatus includes a flexible electrically
conductive element adapted for use as the surface coil antenna portion of
the MR imaging system. The conductive element is movable between a normal
position and an outwardly expanded position in which portions of the
conductor are expanded apart from one another and held in their expanded
spaced apart position so that the electrically conductive element can be
effectively used as a surface coil for detection of RF signals in the MR
imaging system. The surface coil apparatus is passed into the body cavity
of the patient while the surface coil element is in its normal collapsed
position, after which the coil is expanded and held in that position while
the coil is operated as the receiver, antenna for the MR imaging system.
Means are also provided for retracting the electrically conductive element
back to its normal position for use in withdrawing the surface coil
element from the body cavity once MR imaging of the tissues is completed.
In a preferred form of the invention, the surface coil is secured to the
exterior of an inflatable balloon. Fluid such as air under pressure is
applied to the interior of the balloon from a remote location so as to
expand opposite sides of the surface coil apart to increase the area of
the tissue being imaged by the MR system. The inflating fluid then can be
removed from the balloon to retract the surface coil back to its normal
position prior to its being withdrawn from the patient.
This system is useful in placing the surface coil as close as possible to
the tissue under analysis in the body cavity. In one embodiment of the
invention involving MR imaging of the prostate gland, the expandable
surface coil is passed through the rectum to a position close to the
prostate gland. The surface coil is then expanded so that opposite sides
of the coil are held approximately parallel to a coronal plane through the
gland at which imaging is directed. The inflating pressure outwardly on
the opposite sides of the expanded surface coil can hold the coil in its
fixed parallel position to obtain high resolution MR imaging of the entire
transverse section of the prostate.
These and other aspects of the invention will be more fully understood by
referring to the following detailed description and the accompanying
drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a schematic block diagram illustrating a typical MR imaging
system with which the surface coil of this invention can be used.
FIG. 2 is a fragmentary cross-sectional view of an expandable surface coil
apparatus according to principles of this invention.
FIG. 3 is a schematic block diagram illustrating a tuning and matching
circuit for producing RF signals in the MR imaging system.
FIG. 4 is a schematic electrical diagram illustrating components of the
tuning and matching circuit.
FIG. 5 is a schematic cross-sectional view illustrating use of the surface
coil for MR imaging of the prostate gland.
DETAILED DESCRIPTION
FIG. 1 is a schematic block diagram illustrating basic components of an MR
imaging system 10. The present invention includes an expandable surface
coil apparatus 12 for use in diagnosing a patient 14 utilizing the MR
imaging system. The block diagram of FIG. 1 is simply an example of a
typical MR imaging system in which the surface coil apparatus can be used.
In the description to follow, the surface coil apparatus 12 of the present
invention will be described with reference to its use in an MR imaging
system known in the art as a 0.35 Tesla (15 MHz) superconducting Diasonics
MT/S Imaging System. However, the surface coil of this invention also can
be adapted for use in other similar MR imaging systems by techniques known
to those skilled in the art. Typical examples of MR imaging systems
currently available to which the present invention can be adapted are
those manufactured by General Electric, Philips, Picker, Siemens, CSG, El
Scint, and Fonar, to name a few. The system also is described in the
context of MR imaging of the prostate gland, but it will be apparent to
those skilled in the art that the present invention also is adaptable for
use in diagnosing tissues in other body cavities.
As illustrated in the block diagram of FIG. 1, the MR imaging system
includes a large magnet 16 for establishing a magnetic field. A variety of
magnets can be used. A superconducting magnet, resistive magnet or
permanent magnet, common to most clinical MR imaging systems are examples.
The patient being diagnosed is placed inside the magnet. The imaging
system also includes gradient coils (not shown) for selectively altering
the magnetic field in one or more directions. To accomplish this task
preferably three separate gradient coils are used so that current flow
through each of the gradient coils will linearly alter the magnetic field
in directions controlled by the gradient coils. Signal transmission and
reception for use in producing MR imaging are achieved through use of a
radio frequency (RF) transmitter 18 and receiver 20. The patient is
surrounded by a body coil 22 which is coupled to the RF transmitter and
serves as a transmitting coil or antenna. When imaging the prostate gland,
the body coil is positioned around the abdominal area of the patient. The
RF receiver 20 is coupled to the surface coil 12 which serves as a
receiving coil or antenna for signals generated by the RF system. The
surface coil is located inside the magnet and is positioned as close to
the patient as possible for maximum sensitivity. For MR imaging of the
prostate gland, the surface coil is placed as close to the prostate as
possible in a manner described in more detail below. A computer system 24
with a large memory, temporary (disk) and permanent (magnetic tape)
storage capabilities, processor, and a high-quality multiformat imager
acquire, process, store and display a large volume of data associated with
the imaging process. The computer system includes the conventional control
interface 26 for controlling the RF transmitter 18 and receiver 20. An RF
oscillator generates radio waves of different frequencies. When the
frequency is appropriate for the exact value of the magnetic field,
resonance occurs. Radio waves of the same frequency are emitted from the
patient, inducing small currents in the surface coil. The induced currents
are detected and sent to and analog--to-digital converter 28 which then
supplies digital signals to the computer system 24 for use in image
display. The computer system processes the signals produced by the RF
system to produce high resolution images on an image display 30.
FIG. 2 illustrates details of the expandable surface coil apparatus 12,
which includes a rigid elongated hollow tube 32 open at both ends. The
tube can be a conventional barium enema tube. An inflatable balloon 34 is
sealed at its ends around an exterior section of the tube so that the tube
passes generally through the diameter of the balloon. The balloon is made
from any suitable medical grade elastomer, and in one embodiment a Bardex
balloon commonly used with a barium enema rectal catheter is used. The
balloon is arranged relative to the outside diameter of the tube so that
the balloon can be inflated to expand outwardly from the tube. In its
normal collapsed position, the balloon wall loosely surrounds the outside
diameter of the tube so that the collapsed state of the balloon generally
matches the narrow profile of the tube outer wall. An air inlet 36 to the
interior passage 38 of the tube can be connected to a supply (not shown)
of air or other gas or inflating fluid under pressure for use in inflating
the balloon. As illustrated by the arrows in FIG. 2, the inflating fluid
flows from the interior passage 38 of the tube through ports 40
surrounding the tube to the interior of the surrounding balloon. The
flexible wall of the balloon is expanded outwardly by the inflating
pressure to progressively move outwardly away from the narrow profile tube
to the inflated position of the balloon (illustrated in FIG. 2) in which
the opposite walls of the balloon are spaced apart from the outside
diameter of the tube. By retaining the inflating pressure within the
balloon, the outer wall of the balloon can be held in its expanded
position spaced apart from the outside diameter of the tube.
The surface coil apparatus further includes a surface coil wire 42 in the
form of a loop also illustrated schematically in FIG. 3. The surface coil
wire preferably is an elongated flexible electrically conductive element
in the form of a single continuous wire made from copper or other metal
and electrically insulated in a conventional insulating jacket. In forming
the surface coil wire as a loop, the surface coil can be defined as having
opposite first and second lead portions 44 and 46, respectively, which
extend closely parallel to one another before transitioning into an outer
loop 48 expanded outwardly from the first and second lead portions of the
coil. The coil is coupled to the tube 32 and balloon 34 by passing the
long parallel first and second lead portions 44 and 46 of the coil through
the long hollow interior of the tube. The opposite lead portions of the
coil then emerge from the tip of the tube and pass over the outer wall of
the tube at 50, near the tip of the tube. The loop portion 48 of the coil
then passes around the exterior of the inflatable balloon 34 so that the
conducting wire portions 52 of the loop are spaced apart from one another
on opposite sides of the balloon. The portion of the loop farthest from
the tip of the tube passes around one side of the tube adjacent the inner
end of the balloon. Preferably, the portions 52 of the loop 48 in contact
with the outer wall of the balloon are on a common diameter through the
axes of the balloon (and through the central axis of the tube) so that the
portions of the loop carried on the balloon are spaced approximately 180
degrees apart around the circumference of the balloon. The portions 52 of
the loop carried on the balloon outer wall can be secured to the balloon
by various means for achieving a rigid connection thereto; and in one
embodiment, small sections of an adhesive tape (not shown) can be used to
bond portions of the wire to the balloon. Moreover, the flexible opposite
portions of the conductive wire are in a slack condition on the outside of
the balloon when the balloon is in its normal or collapsed state to
provide a sufficient axial dimension of the wire to accommodate outward
flexing and expansion of the loop portion of the wire when the balloon is
inflated. At the opposite end of the surface coil 42, the first and second
lead portions 44 and 46 of the surface coil are preferably contained
within a common electrically insulative outer jacket 54 which passes
through end seals 56 and 58 for sealing off the fluid pressure inside the
tube during inflation of the balloon. The lead portions 44 and 46 of the
surface coil wire then pass to a tuning and matching circuit 60
illustrated schematically in FIG. 3. The expandable surface coil apparatus
of FIG. 2 also includes an outer balloon 62 made of a suitable medical
grade elastomer which can be removable for reuse of the surface coil
apparatus on different patients.
The tuning and matching circuit 60 can be any of various circuit
configurations for adapting an MR imaging system for use with a surface
coil. As described above, the surface coil 42 is used for detection only.
Excitation is achieved by use of the standard body coil 22. Tuning and
matching of the surface coil and body coil are preferably controlled by
electronic capacitors used in the circuit illustrated in FIG. 4. During
excitation the receiver coil is detuned, and during signal detection the
transmitter coil is damped. This successive detuning and damping is
performed electronically via fast switching variable capacity diodes which
are controlled by an applied voltage. The method of electronic tuning,
matching and damping is described in further detail by Boskamp, Radiology
157:449-452 (1985), which is incorporated herein by this reference.
FIG. 4 illustrates a presently preferred tuning and matching circuit which
includes reverse biased diodes 64 and 66 which are preferably variable
capacitor diodes. These diodes are coupled to the surface coil input along
With a variable capacitor 68. The variable capacitor diodes behave as a
variable capacitor, the capacitance of which depends upon the reverse
voltage across each diode. The variable capacitor diodes are used for
fine-tuning the tuning and matching circuit in response to variable
voltage signals at a tuning input 70 and matching outputs 72. The
capacitor 68 is adjusted to the desired resonant frequency of the system.
The matching outputs 72 are back-biased to the same voltage. These
voltages are adjusted simultaneously. The tuning input is coupled to the
receiver through the input resistor 74, the reverse biased diode 64, and a
bridge circuit comprising resistors 75 and 76 having a common ground
connection, and a diode pair 78 in series with a reverse biased diode 80.
One matching output 72 is coupled to a second bridge circuit at a common
connection between a diode pair 82 and a reverse biased diode 84. The
second bridge circuit also includes a pair of resistors 86 and 88 with a
common ground connection. The other matching output 72 is coupled to the
first bridge circuit at a common connection between the diode pair 78 and
the reverse biased diode 80. Resistors in the circuit shown in FIG. 4 are
used to isolate the RF circuit from its environment. During an excitation
pulse the impedance of the surface coil circuit is increased by switching
the reverse voltage on the reverse biased diodes so as to increase the
resonant frequency of the circuit. This induces a current in the surface
coil coupled to the circuit. Tuning and matching are therefore achieved by
DC voltage signals under computer control and induced currents in the
surface coil are sent to the receiver and then to the analog-to-digital
converter 28.
Inasmuch as two coils operating at the same resonant frequency are used, a
coupling problem can develop. This problem can be solved by minimizing the
mutual inductance or maximizing the impedance of the surface coil or
resonant circuit during excitation, using a decoupling circuit described
in the Boskamp article referred to above.
In using the surface coil, the tube 32 is inserted transrectally with the
balloon 34 in its normal or collapsed condition. This step is best
illustrated in FIG. 5 which schematically illustrates the patient 14 with
the surrounding body coil 22 inside the outer magnet 16. For orientation
purposes, FIG. 5 also illustrates the prostate 90, rectum 92 and coccyx
94. The surface coil is inserted so that the coil is placed posterior to
the prostate, as close to the gland as possible. The tube is orientated so
that the opposite portions 52 of the loop formed by the surface coil are
essentially parallel to the coronal imaging plane in the prostate,
represented by the coronal axis 96 through the prostate gland, as
illustrated in FIG. 5. Fluid pressure such as air is then applied to the
interior of the tube to expand the balloon 34 outwardly so as to distend
the loop portion of the surface coil wire to enlarge its diameter to
approximately 5 cm. The balloon is held in its expanded condition for
holding the opposite sides of the surface coil wire in their fixed
expanded orientation during excitation by the body coil and detection of
RF energy by the surface coil. In one experimental use, the balloon was
positioned posterior to the prostate and images were acquired on a
256.times.256 matrix with 0.95 mm pixels. High resolution images of the
prostate were obtained giving good depiction of the prostatic zonal
anatomy. Images were substantially higher in resolution than corresponding
images obtained with an MR imaging system using a body coil only for
excitation and detection.
Test results indicated that lesions 3 to 4 mm. in size could be detected
with the expandable surface coil of this invention, whereas the same
lesions did not appear on images produced from the same patient by the use
of an exterior body coil only. Images developed by experimental use of the
invention have detected abnormal tissue with high resolution. It is
expected that, with continued research and pathological data, clinical
stages A or B of prostatic carcinoma may be detected. MR imaging using an
exterior body coil only does not provide the resolution necessary to
precisely detect stages A and B and has thus far only been able to detect
extracapsular malignant growth after it has invaded surrounding tissues.
Use of the surface coil of this invention also has shown that best results
are obtained when the expanded coil wires of the surface coil are
approximately parallel to the coronal imaging plane through the prostate.
This ensures uniformity of the image. Moreover, by expansion of the
surface coil wire portions 52 to a sufficiently large spacing relative to
the width of the prostate, the surface coil ensures a complete image of
the prostate tissue. Any twisting of the coil about the axis of the tube
to a position in which opposite sides of the loop are offset at an angle
to the coronal axis 96 through the prostate can produce high signal
rear-field artifact with image degradation (where the antenna coil is too
close to the gland) or produce image portions having poor resolution
(where the coil is positioned too far from the prostate).
Although the invention has been described in relation to its use in MR
imaging of the prostate gland, tissues in other body cavities, including
oral, vaginal, gastrointestinal and rectal uses of the expandable surface
coil are possible, without departing from the scope of the invention.
Moreover, although use of the surface coil in its expanded condition has
been illustrated in the context of an inflatable balloon for expanding the
surface coil loop outwardly once the coil is in place inside the body
cavity, other techniques for expansion and retraction of the flexible
surface coil also are possible without departing from the scope of the
invention. For instance, a spring-loaded electrically insulated surface
coil can be used. The coil can be inserted into the body cavity in a
collapsed or retracted position, after which the spring can be activated
remotely to expand opposite sides of the coil outwardly to a spaced apart
distance sufficient for imaging the desired area of the tissue under
analysis. The spring-loaded pressure remains applied on the coil,
preferably by outward pressure constantly applied from within the loop
formed by the coil. The spring force then can be released to retract the
coil.
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