mechanical manifestation of human hemodynamics j.kříž, p.Šeba department of physics,university...

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Mechanical manifestation Mechanical manifestation of human of human hemodynamics hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles University 15. konference českých a slovenských fyziků 7.9.2005 arXiv: physics/0507135

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Page 1: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Mechanical manifestationMechanical manifestation of human of human

hemodynamicshemodynamics

J.Kříž, P.ŠebaDepartment of physics,University Hradec Kralove

andK.Martiník

Faculty of Medicine, Charles University

15. konference českých a slovenských fyziků

7.9.2005

arXiv: physics/0507135

Page 2: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Force plate

Measured are the three force and three moment components , i.e. a six dimensional multivariate time series

Page 3: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Typical data

Page 4: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Force plate

Measured are the three force and three moment components , i.e. a six dimensional multivariate time series

only five independent channelsMF

Usual choice: three force components + point of application of the force: COP

,z

y

F

Mx .

z

x

F

My

Page 5: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Typical data: COP (120 s)

Page 6: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Our equipment

Page 7: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Measurements

Using the force plate and a special bed we measured the force plate output and the ECG signal on 17 healthy adult males. In three cases we measured also the heart sounds. In such a way we obtained a 7 or 8 dimensional time series. The used sampling rate was 1000 Hz.

Page 8: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Typical data: COP (10 s)

Page 9: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

For a reclining subject the motion of the internal masses withinthe body has a crucial effect. Measured ground reaction forces contain

information on the blood mass transient flow at each heartbeat and on the movement of the heart itself. (There are also other sources of the internal mass motion that cannot be suppressed, like the stomach activity etc, but they are much slower and do not display a periodic-likepattern.)

Starting point of the cardiac cycle: the R wave of the ECG signal. Length of the cycle: 1000 ms

Page 10: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Multivariate signal: processprocess multidimensional time-parameterized curve.

Measured channel: projection of the curve to a given axis

Changing the position of an electrode within EEG measurement changes the measured voltage. The measured process remains unchanged.

Characterizing the curve: geometrical invariants:

c: [a,b] n … Cn([a,b]) – mapping, such that

examples of geometrical invariants: length of a curve

Curvatures

].,[,0)(' battc

dttclb

a )('

Page 11: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Frenet frameA Frenet frame is a moving reference frame of n orthonormal vectors e_i(t) which are used to describe a curve locally at each point γ(t).

The main message of the differential geometry: it is more natural to describe local properties of the curve in terms of a local reference system than using a global one like the euclidean coordinates.

Page 12: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Assume that are linearly independent

The Frenet Frame is the family of orthonormal vectors called Frenet vectors. They are constructed from the derivates of c(t) using the Gram-Schmidt orthogonalization algorithm with

                   

                                                                         

                             

The real valued functions are called generalized curvatures and are defined as

)(,),(''),(' )1( tctctc n ].,[ bat

]},[|)(),(),({ 21 batttt n eee

).()()()(

,1,2 ),()(),()()( ,)(

)()(

,)('

)(')(

121

1

1

)()(

1

tttt

nktttctctt

tt

tc

tct

nn

i

k

ii

kkk

k

kk

eeee

eeee

ee

e

1,,1 ),( njtj

.)('

)(),(')(

1

tc

ttt

jj

j

ee

Page 13: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Special cases2 – dimensional curve

3 – dimensional curve

)('

)('

)('

1)(,

)('

)('

)('

1)(

1

22

2

11 tc

tc

tct

tc

tc

tct ee

31221

1)('

)(')('')(')('')()(

tc

tctctctctt

…curvature

…tangent, normal

binormal normal, tangent, )()()( 321 ttt eee

31)('

)('')(')()(

tc

tctctt

22)('')('

)('''),('')(')()(

tctc

tctctctt

…curvature

…torsion

Page 14: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Frenet-Serret FormulasRelation between the local reference frame and its changes

Main theorem of curve theory

.,,,1)('

).,(2,,10)(1,,1

),(,,,

121

1121

n

j

jnn

ctc

cn

batnjtnj

Cba

curvatures has and

that so , curve ldimensiona- tions)transforma Eucleidian to (up unique is

there Then and for withand for

continuous- with some on defined functions Given j

Curvatures are invariant under reparametrization and Eucleidian transformations!Therefore they are geometric properties of the curve.

Page 15: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

The 5 curvatures were evaluated at each cycle and the mean over cycles was taken. The measurement lasted 8 minutes

Page 16: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

The results are reproducible

Page 17: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

What does it mean?

Are the curvature peaks linked to some physiological events?

Page 18: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles
Page 19: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles
Page 20: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

On branching places of large arteries the pulse wave is scattered andthe subsequent elastic recoil contribute to the force changes measured by the plate. A similar recoil is expected also when the artery changes its direction (like for instance in the aortal arc).

Page 21: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Pressure wave oscillations

Page 22: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Pathology: abdominal aneurism

Page 23: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles
Page 24: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

volunteer

pacient

Page 25: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Scattering of the pressure wave on the artery branchings / bendings leads to forces and moments measured by the force plate.

Pressure wave velocity :

Depends on the elasticity of the arterial wall and on the arterial pressure.

Page 26: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles
Page 27: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Pulse wave velocity on large arteries is not directly accessible.

Page 28: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Timing and consistency

Pulse wave velocity: c=L/T; L=0.7 m

Page 29: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

Magnetic resonace measurements

Page 30: Mechanical manifestation of human hemodynamics J.Kříž, P.Šeba Department of physics,University Hradec Kralove and K.Martiník Faculty of Medicine, Charles

What is it good for?Measuring the pressure wave velocity in large arteries

Observing pathological reflections (recoils)

Testing the effect of medicaments on the aortal wall properties

etc. and all this fully noninvasively. Cooperation of the patient is not needed