Determination of specific absorption rate (SAR) in magnetic resonance imaging (MRI)

Patent metadata

Field	Value
Publication number	US-9714993-B2
Application number	US-201313739236-A
Country	US
Kind code	B2
Filing date	Jan 11, 2013
Priority date	Jan 11, 2013
Publication date	Jul 25, 2017
Grant date	Jul 25, 2017

Abstract

A magnetic resonance imaging (MRI) system includes static and gradient magnetic field generators, at least one radio frequency (RF) coil, at least one RF transmitter and at least one RF receiver. At least one power consumption monitor is coupled to locally measure power consumed by the RF coil. The MRI control system has at least one computer configured to determine a specific absorption rate (SAR) for a patient coupled to the RF coil based on at least: (a) RF power transmitted to said RF coil while the RF coil is inductively coupled to the patient, and (b) an electrical signal output from the at least one power consumption monitor while the RF coil is inductively coupled to the patient.

First claim

What is claimed is:

1. A magnetic resonance imaging (MRI) system comprising:
static and gradient magnetic field generators, at least one radio frequency (RF) coil, at least one RF transmitter and at least one RF receiver;
at least one power consumption monitor, inductively coupled directly to a respectively corresponding conductor of said RF coil so as to locally measure power actually being consumed by said RF coil due to current flowing within said RF coil conductor; and
an MRI control system having at least one computer configured to:
calculate during a patient imaging scan a specific absorption rate (SAR) for a patient coupled to said RF coil based on at least: (a) RF power transmitted to said RF coil while the RF coil is inductively coupled to the patient, and (b) electrical signals output from said at least one power consumption monitor while the RF coil is inductively coupled to the patient.

2. An MRI system as in claim 1 , wherein said at least one-power consumption monitor comprises plural pickup loops spatially distributed at respectively different positions on said RF coil and electrical signals output from said plural pickup loops are combined for use in said determination of a specific absorption rate.

3. An MRI system as in claim 1 , wherein said at least one-power consumption monitor comprises plural E-field probes spatially distributed at respectively different positions on said RF coil and electrical signals output from said plural E-field probes are combined for use in said determination of a specific absorption rate.

4. An MRI system as in claim 3 , wherein each said E-field probe comprises a monopole RF antenna probe fed by coaxial cable.

5. An MRI system as in claim 3 , wherein each said E-field probe comprises a dipole RF antenna probe fed by coaxial cable.

6. An MRI system as in claim 1 , wherein said at least one-power consumption monitor comprises plural voltage measurement connections across respectively corresponding plural capacitors that are spatially distributed at different positions within said RF coil and electrical signals from said voltage measurement connections are combined for use in said determination of a specific absorption rate.

7. An MRI system as in claim 1 , wherein said at least one-power consumption monitor comprises at least one butterfly or figure-eight shaped pickup loop electromagnetically coupled to current flowing in an RF coil conductor.

8. An MRI system as in claim 1 , wherein said SAR is calculated using at least: (a) patient weight; (b) RF power transmitted to said RF coil while the RF coil is inductively coupled to the patient; (c) RF power transmitted to said RF coil while the RF coil is not inductively coupled to the patient; and (d) a comparison of power consumption monitor outputs when the RF coil is and is not coupled to the patient.

9. An MRI system as in claim 8 , wherein said SAR is calculated using a corrected value for RF power transmitted to said RF coil while the RF coil is not inductively coupled to the patient based on comparison of RF power consumption when the RF coil is inductively coupled to the patient and when the RF coil is not inductively coupled to the patient.

10. An MRI system as in claim 9 , wherein said SAR is calculated using a corrected value for RF power transmitted to said RF coil while the RF coil is not inductively coupled to the patient based on comparison of (i) output from at least one power consumption monitor while the RF coil is inductively coupled to the patient, and (ii) output from the at least one power consumption monitor while the RF coil is not inductively coupled to the patient.

11. A magnetic resonance imaging (MRI) system comprising:
static and gradient magnetic field generators, at least one radio frequency (RF) coil, at least one RF transmitter and at least one RF receiver;
at least one power consumption monitor coupled to locally measure power consumed by said RF coil; and
an MRI control system having at least one computer configured to:
determine a specific absorption rate (SAR) for a patient coupled to said RF coil based on at least: (a) RF power transmitted to said RF coil while the RF coil is inductively coupled to the patient, and (b) an electrical signal output from said at least one power consumption monitor while the RF coil is inductively coupled to the patient,
wherein said SAR is calculated using the following formula:

SAR
=

1
weight

⁢

{

P
scan

-

P
unloaded

⁢

⁢
•
⁢

⁢

(

V
scan

V
unloaded

)

2

}

where:
weight=patient weight in kilograms;
P scan =RF power transmitted to the RF coil when loaded with the patient for an MRI scan;
P unloaded =RF power transmitted to the RF coil when not loaded with the patient for an MRI scan;
V scan =an electrical output from at least one power consumption monitor when RF coil is loaded with patient for an MRI scan; and
V unloaded =an electrical output from at least one power consumption monitor when RF coil is not loaded with patient for an MRI scan.

12. An MRI system as in claim 11 , wherein calibration values for P unloaded and V unloaded are determined and pre-stored in memory for ready use in calculating SAR during subsequent MRI patient imaging procedures.

13. A magnetic resonance imaging (MRI) method comprising:
configuring and using an MRI system having static and gradient magnetic field generators, at least one radio frequency (RF) coil, at least one RF transmitter, at least one RF receiver, at least one power consumption monitor, inductively coupled directly to a respectively corresponding conductor of said RF coil so as to locally measure RF power consumed by said RF coil due to current flowing within said RF coil conductor, and an MRI control system having at least one configurable computer to:
calculate during a patient imaging scan a specific absorption rate (SAR) for a patient coupled to said RF coil based on at least: (a) RF power transmitted to said RF coil while the RF coil is inductively coupled to the patient, and (b) an output from said at least one power consumption monitor while the RF coil is inductively coupled to the patient.

14. An MRI method as in claim 13 , wherein said at least one power consumption monitor comprises plural pickup loops spatially distribut

Assignees

• Toshiba Medical Sys Corp

Inventors

• Hamamura Yoshinori
• Chen Xin

Classifications

• G01R33/288 Primary

  Provisions within MR facilities for enhancing safety during MR, e.g. reduction of the specific absorption rate [SAR], detection of ferromagnetic objects in the scanner room · CPC title

• G01R33/44 Primary

  using nuclear magnetic resonance [NMR] (G01R33/24, G01R33/62 take precedence) · CPC title

• G01R33/36

  Electrical details, e.g. matching or coupling of the coil to the receiver · CPC title