JPH0815439A - Blood flow measuring device - Google Patents
Blood flow measuring deviceInfo
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- JPH0815439A JPH0815439A JP17340594A JP17340594A JPH0815439A JP H0815439 A JPH0815439 A JP H0815439A JP 17340594 A JP17340594 A JP 17340594A JP 17340594 A JP17340594 A JP 17340594A JP H0815439 A JPH0815439 A JP H0815439A
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- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B6/00—Apparatus or devices for radiation diagnosis; Apparatus or devices for radiation diagnosis combined with radiation therapy equipment
- A61B6/50—Apparatus or devices for radiation diagnosis; Apparatus or devices for radiation diagnosis combined with radiation therapy equipment specially adapted for specific body parts; specially adapted for specific clinical applications
- A61B6/507—Apparatus or devices for radiation diagnosis; Apparatus or devices for radiation diagnosis combined with radiation therapy equipment specially adapted for specific body parts; specially adapted for specific clinical applications for determination of haemodynamic parameters, e.g. perfusion CT
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Abstract
(57)【要約】
【目的】 採血することなく完全に非侵襲に正確な血流
量を測定する。
【構成】 被検者4の頭部をSPECT装置1でスキャ
ンし、データ収集メモリ2において脳における対象部位
および参照部位の放射能濃度の時間的経過データを得
る。演算装置3はこれらのデータからそれらの時間積分
値を求め、時間経過データと積分値とから近似法により
対象領域の血流量を算出する。
(57) [Summary] [Purpose] Completely non-invasive measurement of accurate blood flow without collecting blood. [Structure] The head of the subject 4 is scanned by the SPECT apparatus 1, and time-series data of the radioactivity concentrations of the target site and the reference site in the brain are obtained in the data collection memory 2. The arithmetic unit 3 obtains the time integrated value from these data, and calculates the blood flow volume of the target region by the approximation method from the time elapsed data and the integrated value.
Description
【0001】[0001]
【産業上の利用分野】この発明は、核医学の分野に関す
るものであり、とくに脳などの臓器の血流量を測定する
装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to the field of nuclear medicine, and more particularly to a device for measuring blood flow in organs such as the brain.
【0002】[0002]
【従来の技術】脳内の123I-IMP(トレーサ)の挙動が図
4に示すような2コンパートメントモデルにしたがうも
のと仮定すると、つぎの数式1で示される基本微分方程
式が成立する。2. Description of the Related Art Assuming that the behavior of 123 I-IMP (tracer) in the brain follows a two-compartment model as shown in FIG. 4, the following basic differential equation is established.
【数1】 ここで、Ca(t)、Cb(t)はそれぞれ半減期補正
された動脈血中放射能濃度、脳組織放射能濃度であり、
K1は局所脳血流量、k2は脳から血液プールへの洗い
出し係数を表わす。そこで、従来では、Cb(t)につ
いては、SPECT(シングルフォトンエミッション型
コンピュータトモグラフィ)装置やPET(ポジトロン
エミッション型コンピュータトモグラフィ)装置等のエ
ミッション型CT装置によるダイナミック測定によって
データ収集するとともに、Ca(t)については動脈の
採血を行なってウェルカウンタなどの放射線検出器で測
定することにより求め、これらのデータからK1、k2
の2つのパラメータを算出するようにしている。[Equation 1] Here, Ca (t) and Cb (t) are the arterial blood radioactivity concentration and brain tissue radioactivity concentration, respectively, whose half-life has been corrected,
K1 represents the local cerebral blood flow, and k2 represents the washout coefficient from the brain to the blood pool. Therefore, conventionally, for Cb (t), data is collected by dynamic measurement using an emission CT device such as a SPECT (single photon emission type computer tomography) device or a PET (positron emission type computer tomography) device, and Ca (T) was obtained by collecting blood from the artery and measuring it with a radiation detector such as a well counter, and based on these data, K1, k2
The above two parameters are calculated.
【0003】この場合、1回の測定につき約10〜30
回程度の頻繁な採血を行なう必要があって患者および医
師の負担が大きく、そのため非侵襲な測定ができること
が望まれている。この点から、従来より、Ca(t)を
標準関数として作成しておいて、実際の被検者について
1回の採血を行なって得た放射能濃度データによりその
標準関数を較正することにより各個人のCa(t)など
を求めることが提案されている(撫中正博、飯田秀博、
村上松太郎「N-isopropyl-p-[123I]iodoamphetamine (
123I-IMP)と回転型ガンマカメラによる局所脳血流定量
法」核医学29巻2号(1992)p263〜26
7)。In this case, about 10 to 30 per measurement
Since it is necessary to perform frequent blood collection about once, the burden on patients and doctors is large, and therefore it is desired to be able to perform non-invasive measurement. From this point, conventionally, Ca (t) is created as a standard function, and the standard function is calibrated by calibrating the standard function with radioactivity concentration data obtained by collecting blood once for an actual subject. It has been proposed to obtain personal Ca (t) etc. (Masahiro Nashinaka, Hidehiro Iida,
Matsutaro Murakami "N-isopropyl-p- [ 123 I] iodoamphetamine (
123 I-IMP) and rotary gamma camera for regional cerebral blood flow quantification ”, Nuclear Medicine Vol. 29, No. 2 (1992) p263-26.
7).
【0004】[0004]
【発明が解決しようとする課題】しかしながら、従来の
ように頻繁に採血を行なうのでは患者および医師の負担
が大きいという問題がある。他方、従来の採血回数を減
らす方法はあくまで簡便法であり、各個体ごとに異なる
動脈血中放射能濃度を正確に求めるものではなく、個人
差に基づく誤差が生じるという問題がある。However, there is a problem that the burden on the patient and the doctor is large if blood is collected frequently as in the conventional case. On the other hand, the conventional method of reducing the number of times of blood sampling is merely a simple method, and does not accurately obtain the arterial blood radioactivity concentration different for each individual, but has a problem that an error due to individual difference occurs.
【0005】この発明は上記に鑑み、採血することなく
完全に非侵襲に検査を行なうことができ、しかも誤差を
最小にすることができる、血流量測定装置を提供するこ
とを目的とする。In view of the above, it is an object of the present invention to provide a blood flow measuring device capable of completely non-invasively performing a test without collecting blood and minimizing an error.
【0006】[0006]
【課題を解決するための手段】上記目的を達成するた
め、この発明による血流量測定装置においては、被検体
の対象領域および参照領域の放射能濃度の時間的経過を
測定する手段と、これら対象領域および参照領域につい
ての各時点の放射能濃度値および測定開始からその各時
点までのその2つの領域についての放射能濃度の積分値
を求めるとともに、これらのデータと既知の血液分配定
数を用いて近似法により上記対象領域の血流量を算出す
る演算手段とを備えることが特徴となっている。In order to achieve the above object, in the blood flow measuring device according to the present invention, means for measuring the time course of the radioactivity concentration in the target area and the reference area of the subject, and these objects are provided. The radioactivity concentration value at each time point for the reference region and the reference region and the integrated value of the radioactivity concentration for the two regions from the start of measurement to each time point were obtained, and these data and known blood distribution constants were used. It is characterized in that it comprises a calculation means for calculating the blood flow volume in the target region by an approximation method.
【0007】[0007]
【作用】被検体の対象領域および参照領域の放射能濃度
の時間的経過は、エミッション型CT装置によって測定
することができる。2コンパートメントモデルにおいて
成立する注目領域と参照領域のそれぞれについての基本
微分方程式を時間積分して線形化すると、これら2つの
領域に関する式のうち動脈血中放射能濃度の項が共通で
あることから、その項を消去して1つの式を導き出すこ
とができる。上記の2つの領域について測定された各時
点の放射能濃度と、測定開始からその時点までのその2
つの領域についての放射能濃度の積分値とを上記の式に
当てはめ、既知の血液分配定数を用いるなら、近似法に
より上記対象領域の血流量を算出することができる。The time course of the radioactivity concentration in the target region and the reference region of the subject can be measured by the emission type CT device. When the basic differential equations for the attention area and the reference area that hold in the two-compartment model are integrated by time and linearized, the term of the arterial blood radioactivity concentration is common in the equations related to these two areas. The terms can be eliminated to derive an equation. The radioactivity concentration measured at each time point for the above two areas, and the 2 from the start of measurement to that time point
If the integral value of the radioactivity concentration for one region is applied to the above formula and a known blood distribution constant is used, the blood flow volume in the target region can be calculated by the approximation method.
【0008】[0008]
【実施例】以下、この発明の好ましい一実施例について
図面を参照しながら詳細に説明する。図1において、被
検者4に対して123I-IMPが静注され、SPECT装置1
により頭部のダイナミック測定が行なわれる。これによ
り時間経過ごとに、図2に示すような頭部のECT画像
5が得られる。このECT画像5は、被検者4の頭部の
所定断面における放射能濃度(カウント)の分布を示す
ものであり、このようなECT画像5が時間ごとに順次
得られる。データ収集メモリ2には、このECT画像5
の着目する狭い領域6と適当な参照領域7のそれぞれに
おける全ピクセルのカウント値の総和が各時間ごとに格
納される。つまり、ある時間tにおける注目領域6およ
び参照領域7のそれぞれの放射能濃度Cb(t)、Cb
ref(t)がデータ収集メモリ2において収集され
る。このCb(t)、Cbref(t)が各時間tごと
に収集されるため、Cb(t)、Cbref(t)は図
3に示すように時間に応じて変化するカーブとなる。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, a preferred embodiment of the present invention will be described in detail with reference to the drawings. In FIG. 1, 123 I-IMP was intravenously injected to the subject 4, and the SPECT device 1
Gives a dynamic measurement of the head. As a result, the ECT image 5 of the head as shown in FIG. 2 is obtained every time the time passes. This ECT image 5 shows the distribution of radioactivity concentration (count) in a predetermined cross section of the head of the subject 4, and such ECT images 5 are sequentially obtained every hour. The ECT image 5 is stored in the data collection memory 2.
The total sum of the count values of all pixels in each of the narrow area 6 of interest and the appropriate reference area 7 is stored for each time. That is, the radioactivity concentrations Cb (t) and Cb of the attention area 6 and the reference area 7 at a certain time t, respectively.
ref (t) is collected in the data collection memory 2. Since Cb (t) and Cbref (t) are collected at each time t, Cb (t) and Cbref (t) are curves that change with time as shown in FIG.
【0009】演算装置3はこれらのデータCb(t)、
Cbref(t)を用いて注目領域6の血流量K1を求
める演算を行なう。まず、トレーサの脳内挙動が2コン
パートモデルにしたがうと仮定すると、上記の数式1で
表わされた基本微分方程式が注目領域6および参照領域
7のそれぞれについて成立する。これら注目領域6およ
び参照領域7についての基本微分方程式の微分項を消去
するために、それらの両辺を初期条件Cb(0)=0で
時間積分してつぎの数式2および数式3を得る。The arithmetic unit 3 receives these data Cb (t),
Using Cbref (t), a calculation for obtaining the blood flow volume K1 in the attention area 6 is performed. First, assuming that the behavior of the tracer in the brain complies with the two-compartment model, the basic differential equation represented by the above mathematical formula 1 holds for each of the attention area 6 and the reference area 7. In order to eliminate the differential terms of the basic differential equation for the attention area 6 and the reference area 7, both sides thereof are time-integrated under the initial condition Cb (0) = 0 to obtain the following equations 2 and 3.
【数2】 [Equation 2]
【数3】 これらの式で(Equation 3) In these formulas
【数4】 は動脈血中の放射能濃度の測定開始からある時間tまで
の積分値であり、[Equation 4] Is the integrated value from the start of measurement of the radioactivity concentration in arterial blood to a certain time t,
【数5】 は注目領域6についての放射能濃度の測定開始からある
時間tまでの積分値であり、(Equation 5) Is the integrated value from the start of measurement of the radioactivity concentration for the attention area 6 to a certain time t,
【数6】 は参照領域7についての放射能濃度の測定開始からある
時間tまでの積分値である。(Equation 6) Is the integrated value from the start of measurement of the radioactivity concentration for the reference region 7 to a certain time t.
【0010】ここで、Vdを脳血液分配定数とすると、 k2=K1/Vd,k2ref=K1ref/Vdre
f が成り立つ。今、 Vd=Vdref と仮定しても支障がないので、これを導入すると、上記
数式2、数式3においてHere, when Vd is a cerebral blood distribution constant, k2 = K1 / Vd, k2ref = K1ref / Vdre
f holds. Now, there is no problem even if it is assumed that Vd = Vdref, so if this is introduced,
【数4】は共通であるため、これを消去したつぎの数式
7が導き出せる。Since Eq. 4 is common, the following Equation 7 can be derived by eliminating it.
【数7】 (Equation 7)
【0011】この数式7から、上記データCb(t)、
Cbref(t)と、From the equation 7, the data Cb (t),
Cbref (t),
【数5】、[Equation 5],
【数6】で表わされるそれらの積分値とを用いて、近似
法によりK1/Vdを算出することが可能であることが
わかる。ここでは、Cb(t)、Cbref(t)とそ
れらの積分値をグラフにプロットして線形最小2乗法に
よりK1/Vdを算出することとしている。まず、数式
7の両辺をCbref(t)で割ってつぎの数式8を得
る。It can be seen that it is possible to calculate K1 / Vd by the approximation method using the integrated value expressed by the following equation. Here, C1 / Vd is calculated by the linear least square method by plotting Cb (t) and Cbref (t) and their integrated values on a graph. First, both sides of Expression 7 are divided by Cbref (t) to obtain Expression 8 below.
【数8】 ここで、(Equation 8) here,
【数9】 、[Equation 9] ,
【数10】 とおくと、数式8はつぎの数式11となる。[Equation 10] Then, the equation 8 becomes the following equation 11.
【数11】 この数式11は簡単な1次関数を示している。そこで、
各々のtにおけるCb(t)、Cbref(t)とそれ
らの積分値からX(t),Y(t)を求め、それらで示
されるX(t)−Y(t)座標上の各点をプロットし、
その各点が1つの直線に乗るような直線を近似する。す
ると、この直線が上記の数式11を表わすことになるの
で、その傾きがK1/Vdを表わすことがわかる。そこ
で、線形最小2乗法により上記の近似直線を求めればK
1/Vdが求められる。[Equation 11] This formula 11 shows a simple linear function. Therefore,
X (t) and Y (t) are obtained from Cb (t) and Cbref (t) at each t and their integrated values, and each point on the X (t) -Y (t) coordinates indicated by them is determined. Plot,
A straight line in which each of the points rides on one straight line is approximated. Then, since this straight line expresses the above-mentioned formula 11, it can be seen that the inclination thereof represents K1 / Vd. Therefore, if the above approximate straight line is obtained by the linear least squares method, K
1 / Vd is required.
【0012】一方、脳血液分配定数Vdはトレーサによ
ってほぼ決まっている。つまり、トレーサが123I-IMPの
場合約30ml/g、H2 15Oでは約0.9ml/gで
ある。そこでこのVdの値を、上記のようにして求めた
K1/Vdに代入すれば、注目領域6に関する血流量K
1が求められることになる。On the other hand, the cerebral blood distribution constant Vd is almost determined by the tracer. That is, when the tracer is 123 I-IMP, it is about 30 ml / g, and when H 2 15 O is about 0.9 ml / g. Then, by substituting the value of Vd into K1 / Vd obtained as described above, the blood flow K related to the attention area 6
1 will be required.
【0013】このような、Cb(t)、Cbref
(t)の積分値の算出、線形最小2乗法による近似直線
の算出、その直線の傾きの算出、および既知のVdの値
を用いた血流量K1の算出が演算装置3で行なわれるこ
とになる。Cb (t), Cbref
The calculation device 3 performs calculation of the integrated value of (t), calculation of an approximate straight line by the linear least squares method, calculation of the inclination of the straight line, and calculation of the blood flow K1 using the known value of Vd. .
【0014】なお、上記は一つの実施例に関するもので
あり、この発明の趣旨を逸脱しない範囲で種々に変更可
能である。すなわち、ここでは脳組織の放射能濃度Cb
(t)をリング型あるいは検出器回転型SPECT装置
1で測定しているが、PET装置等の他のエミッション
型CT装置を用いることもできる。また、演算装置3に
おいて行なう注目領域6に関する血流量K1の算出アル
ゴリズムは上記のものに限られない。すなわち上記数式
7を用いて行なう近似法によるK1/Vdの算出方法は
上記のような線形最小2乗法に限定されるわけではな
い。トレーサも他の種類のものが使用可能である。さら
に、脳以外の他の臓器の血流量測定にも適用できること
はもちろんである。The above description relates to one embodiment, and various modifications can be made without departing from the spirit of the present invention. That is, here, the radioactivity concentration Cb of the brain tissue is
Although (t) is measured by the ring type or detector rotating type SPECT apparatus 1, other emission type CT apparatus such as a PET apparatus may be used. Further, the calculation algorithm of the blood flow K1 regarding the attention area 6 performed in the arithmetic unit 3 is not limited to the above. That is, the method of calculating K1 / Vd by the approximation method using Equation 7 is not limited to the linear least square method as described above. Other types of tracers can be used. Furthermore, it is needless to say that the method can be applied to blood flow measurement in organs other than the brain.
【0015】[0015]
【発明の効果】以上実施例について説明したように、こ
の発明の血流量測定装置によれば、採血をまったく行な
わず被検者に負担を与えないことができるとともに、医
師の負担をも軽減できる。しかも個人差による誤差も生
じることはなく、正確な血流量測定を行なうことができ
る。As described above with reference to the embodiments, according to the blood flow measuring device of the present invention, the blood is not collected at all and the burden on the subject can be reduced and the burden on the doctor can be reduced. . Moreover, an error due to an individual difference does not occur, and an accurate blood flow measurement can be performed.
【図面の簡単な説明】[Brief description of drawings]
【図1】この発明の一実施例の模式図。FIG. 1 is a schematic view of an embodiment of the present invention.
【図2】ECT画像を表わす図。FIG. 2 is a diagram showing an ECT image.
【図3】脳組織の放射能濃度曲線を表わすグラフ。FIG. 3 is a graph showing a radioactivity concentration curve of brain tissue.
【図4】2コンパートメントモデルの模式図。FIG. 4 is a schematic diagram of a two-compartment model.
1 SPECT装置 2 データ収集メモリ 3 演算装置 4 被検者 5 ECT画像 6 注目領域 7 参照領域 1 SPECT Device 2 Data Collection Memory 3 Computing Device 4 Subject 5 ECT Image 6 Area of Interest 7 Reference Area
Claims (1)
能濃度の時間的経過を測定する手段と、これら対象領域
および参照領域についての各時点の放射能濃度値および
測定開始からその各時点までのその2つの領域について
の放射能濃度の積分値を求めるとともに、これらのデー
タと既知の血液分配定数を用いて近似法により上記対象
領域の血流量を算出する演算手段とを備えることを特徴
とする血流量測定装置。1. A means for measuring the time course of radioactivity concentration in a target region and a reference region of a subject, and a radioactivity concentration value at each time point for these target region and reference region and from the start of measurement to each time point thereof. And an arithmetic means for calculating an integrated value of the radioactivity concentration in the two regions of the target region and calculating the blood flow volume of the target region by an approximation method using these data and a known blood distribution constant. Blood flow measuring device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17340594A JPH0815439A (en) | 1994-06-30 | 1994-06-30 | Blood flow measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17340594A JPH0815439A (en) | 1994-06-30 | 1994-06-30 | Blood flow measuring device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0815439A true JPH0815439A (en) | 1996-01-19 |
Family
ID=15959822
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17340594A Pending JPH0815439A (en) | 1994-06-30 | 1994-06-30 | Blood flow measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0815439A (en) |
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2005095340A (en) * | 2003-09-24 | 2005-04-14 | Toshiba Corp | Blood flow analysis device and blood flow analysis method |
| JP2005537096A (en) * | 2002-08-27 | 2005-12-08 | ケネディー クリーガー インスティチュート | Magnetic resonance imaging of blood volume in microvessels |
| WO2009101759A1 (en) * | 2008-02-13 | 2009-08-20 | Nihon Medi-Physics Co., Ltd. | Cerebral blood flow quantification device, cerebral blood flow quantification method and program |
| JP2010005456A (en) * | 2009-10-13 | 2010-01-14 | Toshiba Corp | Blood flow analyzer and blood flow analysis method |
| JP2012013665A (en) * | 2010-06-30 | 2012-01-19 | Nihon Medi Physics Co Ltd | Apparatus, program and method for brain blood flow quantitation |
| JP2012108105A (en) * | 2010-10-19 | 2012-06-07 | Nihon Medi Physics Co Ltd | Device, program and method for quantitating cerebral blood flow |
| JP2013255811A (en) * | 2004-11-16 | 2013-12-26 | Medrad Inc | Systems and methods of determining injection protocols for image diagnosis procedure |
-
1994
- 1994-06-30 JP JP17340594A patent/JPH0815439A/en active Pending
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2005537096A (en) * | 2002-08-27 | 2005-12-08 | ケネディー クリーガー インスティチュート | Magnetic resonance imaging of blood volume in microvessels |
| JP2005095340A (en) * | 2003-09-24 | 2005-04-14 | Toshiba Corp | Blood flow analysis device and blood flow analysis method |
| US7756562B2 (en) | 2003-09-24 | 2010-07-13 | Kabushiki Kaisha Toshiba | Apparatus and method for analyzing blood flow |
| JP2013255811A (en) * | 2004-11-16 | 2013-12-26 | Medrad Inc | Systems and methods of determining injection protocols for image diagnosis procedure |
| WO2009101759A1 (en) * | 2008-02-13 | 2009-08-20 | Nihon Medi-Physics Co., Ltd. | Cerebral blood flow quantification device, cerebral blood flow quantification method and program |
| JP2010005456A (en) * | 2009-10-13 | 2010-01-14 | Toshiba Corp | Blood flow analyzer and blood flow analysis method |
| JP2012013665A (en) * | 2010-06-30 | 2012-01-19 | Nihon Medi Physics Co Ltd | Apparatus, program and method for brain blood flow quantitation |
| JP2012108105A (en) * | 2010-10-19 | 2012-06-07 | Nihon Medi Physics Co Ltd | Device, program and method for quantitating cerebral blood flow |
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