Method for measuring intracranial elasticity
09724068 · 2017-08-08
Assignee
Inventors
Cpc classification
A61B8/5223
HUMAN NECESSITIES
A61B8/485
HUMAN NECESSITIES
International classification
A61B8/00
HUMAN NECESSITIES
Abstract
A novel method to noninvasively measure intracranial pressure (ICP) and more generally brain elasticity is disclosed. ICP is determined using an algorithm coupled on a simulated artificial neural network (SANN) that calculates ICP based on a determination of a set of interacted ultrasound signals (IUSs) generated from multiple ultrasound pulses. The methods and systems of the present invention are capable of rapidly determining ICP without manual review of EPG waves by a technician.
Claims
1. A method of measuring elasticity of a tissue within a mammalian body, comprising the steps of: a. transmitting at least one ultrasound pulse into the body at a target to obtain a reflected signal; b. graphing the reflected signal (“s”) intensity over time (“t”) to generate an echopulsograph (“EPG”); c. identifying the points of variation of said signal over time; and d. calculating the elasticity of a tissue using said points of variation and a weighing function W; wherein said weighing function W is obtained by performing the steps of: e. determining a reference value corresponding to an initial tissue elasticity as represented by an initial set of points of variation; f. assigning an arbitrary value for said weighing function W; g. calculating an intermediate value for a current tissue elasticity from said initial set of points of variation and said arbitrary value; h. calculating a difference between said reference value and said intermediate value; i. changing said arbitrary value of function W based on said difference; and j. repeating steps g and l until said intermediate value reaches said reference value.
2. The method of claim 1, wherein the ultrasound pulse has a frequency of at least 1 MHz.
3. The method of claim 1, wherein the ultrasound pulse has a frequency of at least 5 MHz.
4. The method of claim 1, wherein the ultrasound pulse has a frequency of at least 10 MHz.
5. The method of claim 1, wherein at least 10 ultrasound pulses are transmitted into the body.
6. The method of claim 1, where the ultrasound pulse has an amplitude between 0 to 200 volts.
7. The method of claim 1, where the ultrasound pulse is received by an ultrasound receiver at a rate of 10 mega-samples/sec over 14 beats.
8. The method of claim 1, where the ultrasound pulse is received by an ultrasound receiver at a rate of 1000 mega-samples/sec over 14 beats.
9. The method of claim 1, where the ultrasound pulse is received by an ultrasound receiver at a rate of 10,000 mega-samples/sec over 14 beats.
10. The method of claim 1, where the ultrasound pulse is received by an ultrasound receiver at a rate of 100,000 mega-samples/sec over 14 beats.
11. The method of claim 1 wherein said elasticity is calculating using the formula:
Σ tan h(Σl×W+b)W+b wherein l is an input matrix of data points based on the reflected signal(s), and b is a bias constant.
12. The method of claim 1 wherein said step of calculating said elasticity is performed using a neural network.
13. The method of claim 1 further comprising performing an invasive technique on said tissue to determine said reference value.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
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DETAILED DESCRIPTION
(11) The present invention is directed to a method for non-invasively measuring ICP and more generally the elasticity of tissues within or proximate to various organs or cavities within the body. In one embodiment, ICP is determined by insonating the cranial cavity using a transcranial Doppler signal. First, the position of the anterior and posterior walls of the third ventricle are identified, and an ICP wave plot established. The ICP is then calculated from the ICP wave using a neural network. More generally, the methods and systems of the present invention may be used for measuring tissue elasticity in a variety of different tissues.
(12) In one embodiment of the invention, the methods and systems of the present invention use ultrasonic probes. Such probes may be constructed from one or more piezoelectric elements activated by electrodes, for example, from lead zirconate titanate (“PZT”), polyvinylidene diflouride (“PVDF”), PZT ceramic/polymer composite, and the like. The electrodes are connected to a voltage source, a voltage waveform is applied, and the piezoelectric elements change in size at a frequency corresponding to that of the applied voltage. When a voltage waveform is applied, the piezoelectric elements emit an ultrasonic wave into the media to which it is coupled at the frequencies contained in the excitation waveform. Conversely, when an ultrasonic wave strikes the piezoelectric element, the element produces a corresponding voltage across its electrodes. The invention may be practiced using any of numerous ultrasonic probes that are well known in the art.
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(15) Standard, commercially available components may be used in system of the present invention. The following description of specific components is only exemplary, and the system of the present invention is not limited to these components. For example, the DSP 4 may be a C2000 DSC and TMS320C20x by Texas Instruments, a Canberra's 2060 model, CEVA-X1641, CEVA-X1622, CEVA-X1620, or the CEVA-TeakLite-III. The DSP 4 is responsible for generation of electrical pulses or signals with a frequency of at least 1 MHz via the probe 1, detection of the reflected waves or echoes through the probe 1, and processing of the detected digital signals. The ranges can be changed in the firmware of the DSP 4 according to the signal studied.
(16) A measurement cycle is initiated when a start signal from the computer 6 is received by the DSP 4. In response, the DSP 4 instructs the probe 1 to generate a series of ultrasound pulses. A commercially available ultrasound probe may be used with the methods and systems of the invention (see, Advanced Transducer Services, Inc. [online], [retrieved on Jul. 30, 2008]. Retrieved from the Internet <URL: www.atsultrasound.com/>). The ultrasound probe 1 should be capable of transmitting ultrasound waves at a frequency of at least about 1 MHz, and up to about 10 MHz.
(17) Ultrasound sources and detectors may be employed in a transmission mode, or in a variety of reflection or scatter modes, including modes that examine the transference of pressure waves into shear waves, and vice versa. Ultrasound detection techniques may also be used to monitor the acoustic emission (“s”) from insonified tissue. Detection techniques involve measurement of changes in acoustic scatter such as backscatter, or changes in acoustic emission. Examples of acoustic scatter or emission data that are related to tissue properties include changes in the amplitude of acoustic signals, changes in phase of acoustic signals, changes in frequency of acoustic signals, changes in length of scattered or emitted signals relative to the interrogation signal, changes in the primary and/or other maxima and/or minima amplitudes of an acoustic signal within a cardiac and/or respiratory cycle; the ratio of the maximum and/or minimum amplitude to that of the mean or variance or distribution of subsequent oscillations within a cardiac cycle, changes in temporal or spatial variance of scattered or emitted signals at different times in the same location and/or at the same time in different locations, all possible rates of change of endogenous brain tissue displacement or relaxation, such as the velocity or acceleration of displacement, and the like. Multiple acoustic interrogation signals may be employed, at the same or different frequencies, pulse lengths, pulse repetition frequencies, intensities, and the multiple interrogation signals may be sent from the same location or multiple locations simultaneously and/or sequentially. Scatter or emission from single or multiple interrogation signals may be detected at single or at multiple frequencies, at single or multiple times, and at single or multiple locations.
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(19) During any cardiac cycle (“systole and diastole”) multiple EPG measurements can be taken;
(20) In one embodiment of the invention, at least 10 EPGs measurements are made. In another embodiment, at least 25 EPGs are made. In a third embodiment, at least 50 EPGs are made. In a fourth embodiment, at least 100 EPGs are made. The EPG signals are each digitized and displayed on a display screen as a function of intensity and time. As shown in
(21) These points represent the discrete bundles of digitized data points from the isolated portion of the EPG, which are then used to calculate ICP based on the equation:
ICP=Σ tan h(“Σ.sup.I×W+b”)W+b
where I represents the input matrix of all the data points from the selected portion of the echopulsogram 21-35, W is the weight matrix that is obtained through the training process, and b is a random bias constant assigned by the computer 6.
(22) The input matrix is a (“n by k”) mathematical matrix where n rows equals the number of samples; in one embodiment of this invention, this value is at least ten. The k columns equal the data points along the respective EPGs found between the ventricle walls. The matrix is calculated via known mathematical means.
(23) The W value, or weight matrix, is obtained through the training or correlation process, which must be done once. The method of training the SANN is described in V. D. De Viterbo and J. C. Belchior, Artificial Neural Networks Applied for Studying Metallic Complexes, Journal of Computational Chemistry, vol. 22, no. 14, 1691-1701 (“2001”). The training process is a backpropagation algorithm that consists of repeatedly presenting the input and desired output sets to the network. The weights are gradually corrected until the desired error is achieved in the network. This method is depicted in
ΔW.sup.l.sub.ji=ηδ.sub.j.sup.lout.sub.i.sup.l−1+μΔW.sub.ji.sup.l(previous) (1)
where ΔW.sup.l.sub.ji represents the correction to the weight between the jth element in the lth layer and ith element in the previous layer. The quantity out .sub.I.sup.l−1 contains the output result on the l−1 layer. The parameters η and μ are denominated the learning rate and the momentum constant, respectively. These constants determine the rate of convergence during the training procedure. Usually, these parameters are dynamically adjusted to obtain the best convergence rate. The errors introduced during the training stage are calculated as
δ.sub.i.sup.last=(y.sub.j−out.sub.j.sup.last)out.sub.j.sup.last(1−out.sub.j.sup.last) (2)
and
δ.sub.j.sup.l=(Σ.sub.k=1.sup.rδkl+1Wkjl+1)out.sub.j.sup.l(1−out.sub.j.sup.l) (3)
where y.sub.j is the output target that is compared with the output results of the out.sub.j.sup.l of the lth layer. The network error can be then calculated as
ε.sup.l=Σ.sub.j=1.sup.n(y.sub.j−out.sub.j.sup.l).sup.2 (4)
For the learning procedure the neuron behavior was calculated through the sigmoid function for the intermediary layer and a linear function in the output layer.
(24) For minimizing functions, one embodiment of the invention uses the robust method proposed by Levenberg and implemented by Marquardt (Marquardt et al. J Soc Ind Appl Math 11:431 (“1963”). It works through the dynamical adjustment of the Steepest Descent method and Newton's method. Its advantage is that it is much faster in the way of finding the minimum. According to the Levenberg-Marquardt method (LMM), the update matrix of the weights can be calculated as
W.sub.n+1=W.sub.n−(H+BI).sup.−1∇ε.sup.1(W.sub.n) (5)
where H is the Hessian matrix and β is a variable parameter, and usually it starts as β=0.01. The latter is changed during the minimization search according to the estimation of the local error, and I is the identity matrix. The most difficult task when the LMM is used can be attributed to the calculation of H, and it is approached by
H=J.sup.TJ (6)
where J is the Jacobian matrix and is given by
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where l is the relative error of all weights [eq. (4)]. This approximation for solving the Hessian matrix will avoid computation of second derivatives, which simplifies the calculations. Substituting the above approaches into eq. (5), one obtains
W.sub.n+1=W.sub.n−[J.sup.T(W.sub.n)J(W.sub.n)+β.sub.nI].sup.−1J.sup.T(W.sub.n)ε.sup.1(W.sub.n) (8)
Equation (8) will approach to the pure Gauss-Newton method if β.fwdarw.0 or to the Steepest descent method when β.fwdarw.∞.
(26) In accordance with the present invention, this means that, initially, an ICP value is calculated via the equation with a randomly assigned W value. The resulting ICP value is the test value. A reference ICP value is determined by a known invasive means of measuring ICP. Training then involves comparing that test ICP value to the reference ICP value obtained from a known invasive method. If the difference in ICP values is greater than an acceptable error, the random W value is adjusted. Upon adjusting the W value, a new test ICP value is calculated using the equation and this value is again compared to the reference ICP value. This training process of adjusting the weight value, calculating a new ICP value and comparing it to a reference point is repeated until the calculated ICP value from this process is within an acceptable range of error to the reference value. When this occurs, the W value is stored by the computer 6 and automatically correlated to that specific ICP value that was obtained as the test ICP value. In one embodiment of the invention, the algorithm to train the neural network is as follows:
(27) TABLE-US-00001 BEGIN WHILE START=ON GET SAMPLES OF DIGITALIZED ECHO FROM ADC STORE THE SAMPLES IN A FILE PLOT THE SAMPLES CHOOSE THE VALID WAVES (MANUAL PROCESS) IF WAVES ARE VALID START=OFF (MANUAL) END IF END WHILE NUMBERS OF INPUT OF THE NEURAL NETWORK=306 NUMBERS OF HIDDEN NEURONS=2 W1(2×306)=RANDOM NUMBERS W2(1×2)=RANDOM NUMBERS WHILE(ERROR>0.001) ICP_NON_INVASIVE= W2*(TANH(W1*DIGITALIZED_ECHO)) ERROR=ICP_INVASIVE − ICP_NON_INVASIVE CALCULATE THE NEW W1 AND W2 USING THE LEVENBERG MARQUARDT METHOD W1=W1+DW1 W2=W2+DW2 END WHILE END BEGIN
(28) This training process must be completed for each possible ICP value for the computer to create an index or database of weight values and corresponding ICP values. After the training, the computer 6 is able to calculate the ICP values automatically by corresponding the appropriate W value for each set of inputs and ICP value without an invasive procedure.
(29) The neural network is, therefore, an Algorithm for Correlation of Dynamic Properties of the Head (“ACDPH”) 20. It creates ICP waves using the inputted data. Each point at time (“t”) along the EPG wave is then plotted across multiple EPG waves. As can be appreciated, up to (“n”) samples can be made from a single EPG wave. A graph is then prepared for each time (“t”) showing the amplitude of the EPG wave at each time (“t”) for multiple EPG waves. For structures, such as the occipital portion of the cranium, which do not vary over the cardiac cycle, the graph showing the sampling from multiple EPG waves at time (“t”) is a straight line. The same is not true of points along the third ventricle. Graphically, this is reflected by a change in amplitude in the EPG wave during the cycle. More specifically, this change is represented as an ICP wave with a sine wave pattern, reflecting the expansion and contraction of the wall over the cardiac cycle. The ADCPH 20 obtains the upper and lower boundaries of the inputted points and correlates that data with the value of patients' ICPs obtained from an invasive device through training. After training, the ADCPH is able to calculate the ICP of the patient automatically without using an invasive method. In one embodiment of the invention, the algorithm to obtain the ICP values is as follows:
(30) TABLE-US-00002 BEGIN WHILE START=ON LOAD TRAINED NEURAL NETWORK W1 AND W2 GET SAMPLES OF DIGITALIZED ECHO FROM ADC STORE THE SAMPLES IN A FILE PLOT THE SAMPLES CHOOSE THE VALID WAVES (MANUAL PROCESS) IF WAVES ARE VALID (MANUAL PROCESS) ICP_NON_INVASIVE= W2*(TANH(W1*DIGITIZED_ECHO)) END IF END WHILE END BEGIN
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(32) In contrast to the '743 patent, the present invention provides a more accurate ICP measurement because it takes into account the changes over time in the third ventricle. The '743 patent relies on a point in time at which the flow of blood through the brain tissue is primarily exiting the brain. Moreover, after generating an EPG from an Echo EG signal and an ECG, the prior art patent relies on the operator to select the portion of the EPG that corresponds to the ICP value. In the present invention, the computer program identifies the relevant portion of the graph, the third ventricle. Last, the '743 patent calculates ICP based on an equation, ICP=ρ(“t/T”)*[t/T]−β, that relies on four different equations to define p(“t/T”).
(33) The scope of the present invention is not limited by what has been specifically shown and described hereinabove. Numerous references, including patents and various publications, are cited and discussed in the description of this invention. The citation and discussion of such references is provided merely to clarify the description of the present invention and is not an admission that any reference is prior art to the invention described herein. All references cited and discussed in this specification are incorporated herein by reference in their entirety. Variations, modifications and other implementations of what is described herein will occur to those of ordinary skill in the art without departing from the spirit and scope of the invention. While certain embodiments of the present invention have been shown and described, it will be obvious to those skilled in the art that changes and modifications may be made without departing from the spirit and scope of the invention. The matter set forth in the foregoing description and accompanying drawings is offered by way of illustration only and not as a limitation. The actual scope of the invention is intended to be defined in the following claims.