BASELINE RESTORATION METHODS AND APPARATUSES AND MEDICAL DETECTING EQUIPMENTS THEREOF

Abstract

This disclosure relates to baseline restoration methods and apparatuses and medical detecting equipment thereof. The baseline restoration method comprises: determining whether there is a high-amplitude baseline in an input signal by previous k output signals (Y1, . . . , Yk) of a filter, where k is a natural number and k≧1; setting the previous m output signals (Y1, . . . , Ym) of the filter as Y′ when there is a high-amplitude baseline in the input signal, where Y′ is a desired output signal of the filter; and using a current input signal X0, the previous n input signals (X1, . . . , Xn), and the previous m output signals (Y1, . . . , Ym) of said filter to obtain a current output signal Y0 of said filter.

Description

TECHNICAL FIELD

This disclosure relates generally to medical electronics, particularly to baseline restoration methods and apparatuses and medical detecting equipment thereof.

BACKGROUND

Due to polarization voltage, zero drift and other factors, a baseline of a signal acquired would exceed a dynamic range of the signal during signal collection. When displayed, the signal with a high-amplitude baseline might not be displayed within a display area, or only part of the signal could be displayed within the display area.

In order to observe the complete signal, the baseline should be restored. Because the baseline is a low-frequency signal, a baseline restoration method provided by prior art uses a high-pass filter to remove the baseline. The frequency of the baseline is generally low, so the cut-off frequency of the high-pass filter should be very low. However, the lower the cut-off frequency of the high-pass filter, the longer the time required for the baseline to restore to zero, which leads to the baseline spending a very long time to restore to zero and the requirement for use could not be met. As shown in FIG. 1, assuming that the amplitude of the baseline is 1, the time required for the baseline to restore to zero by a high-pass filter would be more than 20 seconds.

SUMMARY

Disclosed here are embodiments of baseline restoration methods and apparatuses and medical detecting equipment thereof.

In one aspect, a baseline restoration apparatus comprises a filter, a high-amplitude baseline detector and a baseline restoration module.

The high-amplitude baseline detector detects whether there is a high-amplitude baseline in an input signal by the previous k output signals (Y₁, . . . , Y_k) of said filter, where k is a natural number and k≧1.

Said baseline restoration module sets previous m output signals (Y₁, . . . , Y_m) of said filter as Y′ when there is a high-amplitude baseline in the input signal, where Y′ is a desired output signal of said filter.

Said filter uses a current input signal X₀, the previous n input signals (X₁, . . . , X_n), and the previous m output signals (Y₁, . . . , Y_m) to obtain a current output signal Y₀ of said filter.

In another aspect, a baseline restoration method comprises:

determining whether there is a high-amplitude baseline in an input signal by the previous k output signals (Y₁, . . . , Y_k) of the filter, where k is a natural number and k≧1;

setting the previous m output signals (Y₁, . . . , Y_m) of the filter as Y′ when there is a high-amplitude baseline in the input signal, wherein Y′ is a desired output signal of the filter; and

using a current input signal X₀, the previous n input signals (X₁, . . . , X_n), and the previous m output signals (Y₁, . . . , Y_m) of said filter to obtain a current output signal Y₀ of said filter.

In another aspect, a medical detecting equipment comprises a baseline restoration apparatus described above.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows an output signal of a high-pass filter used for baseline restoration in a prior art;

FIG. 2 shows a schematic diagram of a baseline restoration apparatus according to an embodiment.

FIG. 3 shows a specific schematic diagram of the baseline restoration apparatus shown in FIG. 2.

FIG. 4 shows a flow chart of a baseline restoration method according to one embodiment.

DETAILED DESCRIPTION

As shown in FIG. 2, in one embodiment, a baseline restoration apparatus 100 comprises a filter 110, a high-amplitude baseline detector 120 and a baseline restoration module 130. An output port of the filter 110 may be connected to the high-amplitude baseline detector 120, the high-amplitude baseline detector 120 may be connected to the baseline restoration module 130, and the baseline restoration module 130 may be connected to the filter 110.

The high-amplitude baseline detector 120 may detect whether there is a high-amplitude baseline in an input signal by previous k output signals (Y₁, . . . , Y_k) of the filter, where k is a natural number and k≧1.

When the high-amplitude baseline detector 120 determines there is a high-amplitude baseline in the input signal, the previous m output signals (Y₁, . . . , Y_m) of the filter may be set to equal to Y′ respectively by the baseline restoration module 130, that is, making Y₁=Y′, Y₂=Y′, . . . , Y_m=Y′, where Y′ is a desired output signal of the filter 110. When the high-amplitude baseline detector 120 determines there is no high-amplitude baseline in the input signal, the baseline restoration 130 does not do anything.

The filter 110 may use a current input signal X₀, the previous n input signals (X₁, . . . , X_n), and the previous m output signals (Y₁, . . . , Y_m) of the filter to obtain a current output Y₀ of the filter.

In this embodiment, when the high-amplitude baseline is detected, the previous m outputs (Y₁, . . . , Y_m) of the filter may be set to equal to the desired output signal Y′ respectively. Thus the intermediate process, in which the output signal of the filter drops from the current output signal to the desired output signal, could be skipped, and the time required for the baseline to restore to zero could be decreased. In the meantime, the baseline restoration apparatus has nothing to do with the cut-off frequency of the filter, so it could guarantee that the filter band would not be distorted.

FIG. 3 shows the specific schematic diagram of the baseline restoration apparatus shown in FIG. 2. In this embodiment, the filter 110 may be a high-pass filter, and the cut-off frequency of the filter 110 may be relatively low.

The filter 110 may comprise an input magnification part and an output magnification part. The input magnification part may comprise an input magnification branch and n input delay and magnification branches, and the output magnification branch may comprise an output branch and m output magnification branches.

For the input magnification part, in the input magnification branch, an input end 111 may be connected to an input end of an amplifier a₀, and an output end of the amplifier a₀ may be connected to a first input end of an adder e₀; in the first input delay and magnification branch, the input end 111 may be connected to an input end of a delayer c₁, a first output end of the delayer c₁ may be connected to an input end of an amplifier a₁, an output end of the amplifier a₁ may be connected to a first input end of an adder e₁, and an output end of the adder e₁ may be connected to a second input end of the adder e₀. In the second input delay and magnification branch, a second output end of the delayer c₁ may be connected to an input end of a delayer c₂, a first output end of the delayer c₂ may be connected to an input end of an adder a₂, an output end of the amplifier a₂ may be connected to a first input end of an adder e₂, and an output end of the adder e₂ may be connected to a second input end of the adder e₁; in turn, in the nth input delay and magnification branch, a second output end of a delayer c_n-1 may be connected to an input end of a delayer c_n, an output end of the delayer c_n may be connected to an input end of an adder a_n, and an output end of the amplifier a_n may be connected to a second input end of the adder e_n-1.

The input magnification part may be connected to the output magnification part by connecting an output end of the adder e₀ to a first input end of an adder f₀.

For the output magnification part, in the output branch, an output end 113 may be connected to the output end of the adder f₀; in the first output magnification branch, the output end 113 may be connected to an input end of a delayer d₁, a first output end of the delayer d₁ may be connected to an input end of an amplifier b₁, an output end of the amplifier b₁ may be connected to a first input end of an adder f₁, and an output end of the adder f₁ may be connected to the second input end of the adder f₀. In the second output magnification branch, the second output end of the delayer d₁ may be connected to an input end of a delayer d₂, the first input end of the delayer d₂ may be connected to the input end of an amplifier b₂, the output end of the amplifier b₂ may be connected to the first input end of an adder f₂, and the output end of the adder f₂ may be connected to the second input end of the adder f₁. In the mth output magnification branch, the second output end of a delayer d_m-1 may be connected to the input end of a delayer d_m, the output signal of the delayer d_m may be connected to the input end of an amplifier b_m, and the output end of the amplifier b_m may be connected to the second input end of the adder b_m-1.

In the first embodiment, the high-amplitude detector 120 may detect whether all the previous k output signals (Y₁, . . . , Y_k) of the filter are greater than a high-amplitude threshold. When all the previous k output signals (Y₁, . . . , Y_k) of the filter are greater than the high-amplitude threshold, the high-amplitude detector 120 may determine there is a high-amplitude baseline in the input signal. When not all the previous k output signals (Y₁, . . . , Y_k) of the filter are greater than the high-amplitude threshold, the high-amplitude detector 120 may determine there is no high-amplitude baseline in the input signal.

It could be understood that the high-amplitude threshold may be related to the input signal of the filter 110. The greater the amplitude of the input signal is, the greater the high-amplitude threshold may be; the less the amplitude of the input signal is, the less the high-amplitude threshold may be.

In the second embodiment, the high-amplitude detector 120 may detect whether the output energy of the filter 110 calculated using the previous k output signals (Y₁, . . . , Y_k) of the filter is greater than an energy threshold. When the output energy of the filter 110 is greater than the energy threshold, the high-amplitude detector 120 may determine there is a high-amplitude baseline in the input signal. When the output energy of the filter 110 is less than or equal to the energy threshold, the high-amplitude detector 120 may determine there is no high-amplitude baseline in the input signal.

It could be understood that the energy threshold may be related to the amplitude of the input signal of the filter 110. The greater the amplitude of the input signal is, the greater the energy threshold may be; the less the amplitude of the input signal is, the less the energy threshold may be.

When the high-amplitude baseline detector 120 determines there is a high-amplitude baseline in the input signal, the previous m output signals 110 (Y₁, . . . , Y_m) of the filter may be set as Y′ respectively by the baseline restoration module 130, that is, making Y₁=Y′, Y₂=Y′, . . . , Y_m=Y′, where Y′ is the desired output signal of the filter 110.

The filter 110 may use the current input signal X₀, the previous n input signals (X₁, . . . , X_n), and the previous m output signals (Y₁, . . . , Y_m) of the filter 110 to obtain the current output signal Y₀ of the filter.

For the input magnification part, the current input signal X₀ may be input into the amplifier a₀ and the delayer c₁ of the first input delay and magnification branch through the input end 111. The input signal X₁ stored in the delayer c₁ may be inputted into the amplifier a₁ to obtain the magnified signal a₁X₁, . . . . The value of the input signal X_n outputted by the delayer c_n of the nth input delay and magnification branch may be inputted into the amplifier a_n to obtain an amplified signal a_nX_n.

The amplified signal a_nX_n and a_n-1X_n-1 may be inputted into and summed by the adder e_n-1, and the output signal of the adder e_n-1 and the amplified signal a_n-2X_n-2 may be inputted into and summed by the adder e_n-2, . . . . In turn, the output signal of the adder e₁ and the amplified signal a₀X₀ may be inputted into and summed by the adder e₀, and the output signal of the adder e₀ may be the first sum value S_x=a₀X₀+a₁X₁+ . . . +a_nX_n.

For the output magnification part, the current output signal Y₀ may be inputted into the delayer d₁ of the first output magnification branch, the output signal Y₁ of the delayer d₁ may be inputted into the amplifier b₁ to obtain the magnified output signal b₁Y₁, and the output signal Y₁ may be inputted into the delayer d₂ of the second output magnification branch. The output signal Y_m-1 may be inputted into the delayer d_m of the mth delay and magnification branch, and the output signal Y_m stored in the delayer d_m may be inputted into the magnification b_m to obtain the magnified output signal b_mY_m.

The amplified output signal b_mY_m and b_m-1Y_m-1 may be inputted into and summed by the adder f_m-1, the output signal of the adder f_m-1 and the magnified output signal b_m-2Y_m-2 may be inputted into and summed by the adder f_m-2, . . . , and the output signal of the adder f₂ and the magnified output signal b₁Y₁ may be inputted into and summed by the adder f₁ to obtain the second sum value S_y=b₁Y₁+ . . . +b_mY_m.

The first sum value S_x outputted by the adder e₀ and the second sum value S_y outputted by the adder f₁ may be inputted into and summed by the adder f₀ to obtain the current output signal Y₀=(a₀X₀+a₁X₁+ . . . +a_nX_n) (b₁Y₁+ . . . +b_mY_m), where Y₁=Y′, Y₂=Y′, . . . , Y_m=Y.

It could be understood that the structure of the filter 110 described above is just one embodiment of the present disclosure, and the filter 110 could be realized by other structures in other embodiments.

In addition, when the high-amplitude baseline detector 120 determines there is a high-amplitude baseline in the input signal, the baseline restoration module 130 may make Y₁=Y₁′, Y₂=Y₂′, . . . , Y_m=Y_m′, where Y₁′, Y₂′, . . . , and Y_m′ cannot be exactly the same. The output signal of the filter could decline rapidly when the difference among Y₁′, Y₂′ . . . , and Y_m′ is within a certain error range. The error range may be related to the amplitude of the input signal. The bigger the amplitude of the input signal, the bigger the error range allowed; the smaller the amplitude of the input signal, the smaller the error range allowed.

FIG. 4 shows a flow chart of a baseline restoration method in an embodiment. The baseline restoration method could include the following steps:

Step 410: detect whether there is a high-amplitude baseline in an input signal by previous k outputs (Y₁, . . . , Y_k) of the filter, where k is a natural number and k≧1. The filter could be a high-pass filter, and the cut-off frequency of the high-pass filter may be low.

Step 420: when there is a high-amplitude baseline in the input signal, set the previous m output signals (Y₁, . . . , Y_m) of the filter as Y′ respectively, that is, making Y₁=Y′, Y₂=Y′, . . . , Y_m=Y′, where Y′ is the desired output signal of the filter.

Step 430: use a current input signal X₀, previous n input signals (X₁, . . . , X_n), and previous m output signals (Y₁, . . . , Y_m) of the filter to obtain a current output Y₀ of the filter.

Step 410 could include the following steps: (1) detect whether all the previous k output signals (Y₁, . . . , Y_k) of the filter are greater than the high-amplitude threshold; (2) when all the previous k output signals of the filter are greater than the high-amplitude threshold, determine whether there is a high-amplitude baseline in the input signal; (3) when not all the previous k output signals of the filter are greater than the high-amplitude threshold, determine whether there is no high-amplitude baseline in the input signal.

In another embodiment, step 410 could include detecting whether the output energy of the filter calculated using the previous k output signals (Y₁, . . . , Y_k) of the filter is greater than an energy threshold. When the output energy of the filter is greater than the energy threshold, there is a high-amplitude baseline in the input signal; when the output energy of the filter is less than or equal to the energy threshold, there is not a high-amplitude baseline in the input signal.

Step 430 could include the following steps: (1) magnify the current input signal X₀ and the previous n input signals (X₁, X_n) by magnification factors (a₀, a₁, . . . , a_n) respectively, (2) sum all magnified input signals to obtain a first sum value S_x, where n is a natural number and n≧1; (3) magnify the previous m output signals (Y₁, . . . , Y_m) of the filter by magnification factors (b₁, . . . , b_m) respectively, (4) sum all magnified output signals to obtain a second sum value S_y, where m is a natural number and m≧1; and (5) sum the first sum value S_x and the second sum value S_y to obtain a current output signal Y₀=(a₀X₀+a₁X₁+ . . . +a_nX_n)+(b₁Y₁+ . . . +b_mY_m).

In this embodiment, the filter could be a high-pass filter.

This embodiment may be similar to the previous embodiments, the details of which could be understood to refer to FIGS. 2 and 3 and the related description above.

In one embodiment, a medical detecting equipment could comprise a baseline restoration apparatus described above, the details of which could be understood to refer to FIGS. 2 and 3 and the related description above.

In the above embodiments, when a high-amplitude baseline is detected, the previous m output signals (Y₁, . . . , Y_m) of the filter are set as Y′ respectively. Thus the intermediate process in which the value of the filter's output drops from the current output signal to the desired output signal could be skipped, and the time required for the baseline to restore to zero could be decreased. In the meantime, the baseline restoration apparatus has nothing to do with the cut-off frequency of the filter, so it could guarantee that the filter band would not be distorted.

This disclosure has been made with reference to various exemplary embodiments. However, those skilled in the art will recognize that changes and modifications may be made to the exemplary embodiments without departing from the scope of the present disclosure. While the principles of this disclosure have been shown in various embodiments, many modifications of structure, arrangements, proportions, elements, materials, and components may be adapted for a specific environment and/or operating requirements without departing from the principles and scope of this disclosure. These and other changes or modifications are intended to be included within the scope of the present disclosure.

One of ordinary skill in the art will appreciate that all or parts of steps of the method could be executed by relative hardware under direction of a computer program, and the computer program could be stored in computer-readable storage media, which could be a magnetic disk, a light disk, a Read-Only Memory, a Random Access Memory, and so on.

The foregoing specification has been described with reference to various embodiments. However, one of ordinary skill in the art will appreciate that various modifications and changes can be made without departing from the scope of the present disclosure. Accordingly, this disclosure is to be regarded in an illustrative rather than a restrictive sense, and all such modifications are intended to be included within the scope thereof. Likewise, benefits, other advantages, and solutions to problems have been described above with regard to various embodiments. However, benefits, advantages, solutions to problems, and any element(s) that may cause any benefit, advantage, or solution to occur or become more pronounced are not to be construed as a critical, a required, or an essential feature or element. The scope of the present invention should, therefore, be determined by the following claims.

Claims

1. A baseline restoration apparatus, comprising: a filter;a high-amplitude baseline detector configured to detect whether there is a high-amplitude baseline in an input signal by previous k output signals (Y1, . . . , Yk) of said filter, wherein k is a natural number and k≧1; anda baseline restoration module configured to set previous m output signals (Y1, . . . , Ym) of said filter as Y′ when there is a high-amplitude baseline in the input signal, wherein Y′ is a desired output signal of said filter, whereinsaid filter uses a current input signal X0, the previous n input signals (X1, . . . , Xn), and the previous m output signals (Y1, . . . , Ym) to obtain a current output signal Y0 of said filter.

2. The baseline restoration apparatus of claim 1, wherein said high-amplitude detector determines there is a high-amplitude baseline in the input signal when the previous k output signals (Y1, . . . , Yk) of the filter are all greater than a high-amplitude threshold, and determines there is no high-amplitude baseline in the input signal when not all the previous k output signals (Y1, . . . , Yk) are greater than a high-amplitude threshold.

3. The baseline restoration apparatus of claim 1, wherein said high-amplitude detector determines there is a high-amplitude baseline in the input signal when an output energy of said filter calculated using the previous output signals (Y1, . . . , Yk) is greater than an energy threshold, and determines there is no high-amplitude baseline in the input signal when the output energy of said filter is less than or equal to the energy threshold.

4. The baseline restoration apparatus of claim 1, wherein said filter magnifies the current input signal X0 and the previous n input signals (X1, . . . , Xn) by magnification factors (a0, a1, . . . , an) respectively and sums the magnified input signals to obtain a first sum value Sx, magnifies the previous m output signals (Y1, . . . , Ym) by magnification factors (b1, . . . , bm) respectively and sums the magnified output signals to obtain a second sum value Sy, and adds the first sum value Sx and the second sum value Sy to obtain the current output signal of the filter Y0=(a0X0+a1X1+ . . . +anXn) (b1Y1+ . . . +bmYm), wherein n is a natural number and n≧1, and m is a natural number and m≧1.

5. The baseline restoration apparatus of claim 1, wherein said filter is a high-pass filter.

6. A baseline restoration method, comprising: determining that there is a high-amplitude baseline in an input signal by previous k output signals (Y1, . . . , Yk) of a filter, wherein k is a natural number and k≧1;setting previous m output signals (Y1, . . . , Ym) of said filter as Y′ when there is a high-amplitude baseline in the input signal, wherein Y′ is a desired output signal of the filter; andusing a current input signal X0, the previous n input signals (X1, . . . , Xn), and the previous m output signals (Y1, . . . , Ym) of said filter to obtain a current output signal Y0 of said filter.

7. The method of claim 6, wherein determining that there is a high-amplitude baseline in an input signal by previous k output signals (Y1, . . . , Yk) of said filter comprises: determining whether the previous k output signals (Y1, . . . , Yk) of said filter are all greater than a high-amplitude threshold; anddetermining whether there is a high-amplitude baseline in the input signal when all of the previous k outputs of said filter are greater than the high-amplitude threshold, and there is no high-amplitude baseline in the input signal when not all of the previous k output signals of said filter are greater than the high-amplitude threshold.

8. The method of claim 6, wherein determining whether there is a high-amplitude baseline in an input signal by the previous k output signals (Y1, . . . , Yk) of said filter comprises: determining whether an output energy of said filter calculated using the previous k output signal (Y1, . . . , Yk) of said filter is greater than an energy threshold; anddetermining whether there is a high-amplitude baseline in the input signal when the output energy of said filter is greater than the energy threshold, and there is no high-amplitude baseline in the input signal when the output energy of said filter is less than or equal to the energy threshold.

9. The method of claim 6, wherein using the current input signal X0, the previous n input signals (X1, . . . , Xn), and the previous m output signals (Y1, . . . , Ym) of said filter to obtain the current output signal Y0 of said filter comprises: magnifying the current input signal X0 and the previous n input signals (X1, . . . , Xn) by magnification factors (a0, a1, . . . , an) respectively, wherein n is a natural number and n≧1;summing the magnified input signals to obtain a first sum value Sx;magnifying the previous m output signals (Y1, . . . , Ym) of said filter by magnification factors (b1, . . . , bm) respectively;summing the magnified output signals to obtain a second sum value Sy; andsumming the first sum value Sx and the second sum value Sy to obtain the current output signal Y0=(a0X0+a1X1+ . . . +anXn)+(b1Y1+ . . . +bmYm) of said filter, wherein m is a natural number and m≧1.

10. The method of claim 6, wherein said filter is a high-pass filter.

11. A medical detecting equipment, wherein said equipment comprises the baseline restoration apparatus of claim 1.