MRI-Magnetic Resonance Imaging Tris Budiyono (ATRO CB) PPT - 翻译版
MRI-Magnetic Resonance Imaging Tris Budiyono (ATRO CB) PPT - 翻译版
MRI-Magnetic Resonance Imaging Tris Budiyono (ATRO CB) PPT - 翻译版
shell shell
N N
S S
external magnetic field 外部磁场
N N
The protons may align with their 质子可能与它们的
South and North poles in the 向外场方向的南极和北极,与之平
direction of the external field,parallel 行。
to it.
Or they may point exactly in the 或者它们可能正好指向完全相
complete opposite direction,anti- 反的方向,反平行。
parallel.
S S
These types of alignment are on different energy 这些类型的对齐方式具有不同的能级
levels
要得到一个粗略的想法
To get a rough idea
for about 10million protons ”Opposite direction, anti - 约1000万质子"相反方向,反平行",约有10000007"
parallel”,there are about 10000007”direction of the external 外场方向"。
field”.
10million 10million
10million 10million
10million 10million
Opposite direction, anti -parallel 相反方向,反平行
20million ΔE 20million ΔE
10million+6 10million+6
10million+9 10million+9
0T 0.5T 1.0 T 1.5 T 0T 0.5T 1.0 T 1.5 T
Bφ Bφ
N N
The protons do not just lay there, 质子不只是躺在那里,对齐平行或
aligned parallel or anti-pallarel to the 反帕拉雷尔的磁场线。
magnetic field lines.
S S
It is important to know how fast the protons process. 了解质子过程的速度是很重要的。
The stronger the magnetic field, the faster the procession 磁场越强游行越快
rate and higher the procession frequency. 速度和更高的游行频率。
Larmor equation Larmor equation
ω0=γB0 ω0=γB0
ω0 is the precession frequency (in Hz or MHz). ω0是进动频率(以Hz或MHz为单位)。
It is possible and necessary to precisely 精确计算这个频率是可能和必要的。
calculate this frequency.
This is done by using an equation called 这是通过使用一个叫做
Larmor equation. Larmor equation.
B0 is the strength of the external magnetic field, B0是外部磁场的强度,在Tesla(T)中给出
which is given in Tesla (T)
γ is the so-called gyro-magnetic ratio γ是所谓的陀螺磁比
ω0=γB0 ω0=γB0
The equation states that the precession frequency becomes 等式说明进动频率变为
higher when the magnetic field strength increases. 当磁场强度增加时。
The exact relationship is determined by the gyro-magnetic 确切的关系由陀螺磁比γ决定。
ratio γ.
Y Y
X X
S S
longitudinal magnetization longitudinal magnetization
Z The z-axis runs in the direction of Z Z轴沿磁场线方向运行。
the magnetic field lines.
WeAs cannot
this magnetization
measure thisismagnetic
in direction along
force, as it/ 我们不能测量这个磁力,因为它是同一方向
islongitudinal to the external
the same direction, parallelmagnetic fields, it
to the external ,平行于外部磁场。
is also called
magnetic field.longitudinal magnetization.
Z Z
It is actually this new magnetic vector 它实际上是这个新的磁向量,可能被
that may be used to get a signal. 用来得到一个信号。
Y Y
We cannot measure this magnetic force, as it 我们不能测量这个磁力,因为它是同一方向
is the same direction, parallel to the external ,平行于外部磁场。
magnetic field.
RF Coil RF Coil
Z Z Z Z
RF pulse RF pulse
X X X 其中一些被提升到更高的能量
Some of them are lifted to a
higher level of energy, pointing 水平,在图中指向下方。
downward in the illustration.
Z Z
In effect the magnetization along RF pulse 实际上,沿着z轴的磁化强度会 RF pulse
the z-axis decrease, as the 降低,因为指向下方的质子会"
protons which point down 中和"相同数量的指向上方的质
“neutralize” the same number of 子。
protons pointing up.
Y Y
X
X X
X
also causes the protons to precess in step, in phase. 也导致质子在步进,在相中进动。
Z Z Z Z
RF pulse RF pulse
X X X X
a new transversal magnetization,which 一种新的横向磁化强度,它随进动质
moves around with the precessing 子移动。
protons.
Secondary Magnetic 二次磁性
Resonance Imaging ResonanceImaging
Magnets
Volume coils 体积块线圈
Surface coils 曲面线圈
Volume coils 体积线圈
Volume coils are used in all MR units. 体积线圈用于所有MR单元。
These volume coils should be closed to the size of the subject. 这些卷线圈应关闭到对象的大小。
It also receives the signal when larger parts of the body are 当身体较大的部分成像时,它也接收信号。
imaged.
Surface coils 曲面线圈
Surface coils are placed directly on the area of interest, and have 曲面线圈直接放置在感兴趣的区域上,并具有与要检查的零件
different shapes corresponding to the part to be examined. 对应的不同形状。
They are receiver coils only, most of the received signal coming 它们只是接收器线圈,大部分接收到的信号来自附近的组织
from tissues near by; deeper structure cannot be examined ;这些线圈不能检查更深的结构。
with these coils.
As with the head coils, the RF pulse is transmitted by the body 与头部线圈一样,在这些情况下,射频脉冲由身体线圈传递
coil in these cases. 。
a general overview of MRI. 核磁共振成像的概况。
Longit. Longit.
T1-curve T1-curve
magn. magn.
MZ=M0・(1-e-t/T1) MZ=M0・(1-e-t/T1)
time time
The time that it takes for the longitudinal 纵向磁化强度恢复所需的时间,要回到其原
magnetization to recover, to go back to its 值,用纵向松弛时间来描述,也称为T1。
original value, is described by the longitudinal
relaxation time, also called T1.
This actually is not the exact time it takes , 这实际上不是它所花费的确切时间,而是一
but a time constant, describing how fast this 个时间常数,描述这个过程有多快。
process goes.
Y Y Y Y Y Y
X X X X X X
Transversal relaxation time (T2)
If oneZplots transversal magnetization vs. 如果在RF脉冲关闭后绘制横向磁化强度与
time after the RF pulse is switched off, one 时间的关系图,则得到一条曲线,如所示
gets a curve as illustrated, which called a ,称为T2曲线。
T2-curve. Y
X
Transv. Transv.
magn magn
T2-curve T2-curve
MXY=M0・e-t/T2 MXY=M0・e-t/T2
Time Time
How long is a relaxation time? 放松时间有多长?
T2 value T2 value
T2 is the time when transversal magnetization T2是横向磁化强度降至原值37%的时间。
decreased to 37% of the original value.
Approximate
ApproximateTT12relaxation
relaxationtimes
times at
ataafield
field 一个场的近似T2松弛时间
strength
strengthof
of1.0T
1.0Tfor
forvarious
varioustissues
tissues 各种组织的1.0T强度
Tissue T1 (ms) T2 (ms) Tissue T1 (ms) T2 (ms)
Fat 180 90 Fat 180 90
Liver 270 50 270 50
Renal cortex 360 70 肾皮质 360 70
White matter 390 90 白质属 390 90
Spleen 480 80 480 80
灰色物质(graymat
Gray matter 520 100 ter) 520 100
Muscle 600 40 600 40
Renal medulla 680 140 肾髓质 680 140
Blood 800 180 血脑嵴液 800 180
Cerebrospinal fluid 2000 300 2000 300
Water 2500 2500 2500 2500
a general overview of MRI. 核磁共振成像的概况。
X X X X
Y Y
X X
FID signal (free induction decay) FID信号(freeinductiondecay)
Y Y
X X
FID (free induction decay) 自由感应衰变(FID)
Signal 信号强
intensity 度
TE/2 TE TE/2 TE
signal signal
Longit. relax. Longit. relax.
TR TE time TR TE time
When
With awe only wait a very short
in TTE, inthen 当我们只等待一个很短的TE时,由于T2的差异而
A long TR long
and TR,
adifferences
short TE 1 longitudinal 长T 导致的信号强度的差异还没有时间发音。
differences
magnetizationin signal intensity
time are dueimportant
not very to differences
any in
T 2 have
more, asnot
all yet hadhave
tissues timeregained
to become pronounced.
their full
Thelongitudinal magnetization.
T1- and T2-curves for two different tissues are depicted 描
signal signal
TR time TR time
TE TE
The resulting picture is thus neither T1-nor T2- 由此得到的图片既不是T1-norT2加权,但大
weighted, but mostly determined by the 多由组织的质子密度决定。
proton density of the tissues.
signal signal
TR TE time TR TE time
Thus the resulting picture is T2-weighted. 因此,得到的图片是T2-weighted的。
TR time TR time
TE TE
When TE is short, differences in T2 cannot really 当TE短时,T2中的差异不能真正表现出来,因此得
manifest themselves, so the resulting picture is still T1- 到的画面仍然是T1加权。
weighted.
10 10
40 40
100 100
T1-weighted image T1-weighted image
T2-weighted image 250 T2-weighted image 250
500 500
TR (short) TR (short)
25 50 100 200 400 1000 2000 3000 (ms) 25 50 100 200 400 1000 2000 3000 (ms)
a general overview of MRI. 核磁共振成像的概况。