CN113190792A - Ethylene cracking furnace operation state monitoring method based on neighbor local abnormal factors - Google Patents

Ethylene cracking furnace operation state monitoring method based on neighbor local abnormal factors Download PDF

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CN113190792A
CN113190792A CN202110440247.5A CN202110440247A CN113190792A CN 113190792 A CN113190792 A CN 113190792A CN 202110440247 A CN202110440247 A CN 202110440247A CN 113190792 A CN113190792 A CN 113190792A
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ethylene cracking
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虞飞宇
林世颢
陈杨
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College of Science and Technology of Ningbo University
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Abstract

The invention discloses an ethylene cracking furnace running state monitoring method based on a neighbor local abnormal factor, which realizes real-time characteristic analysis on sampled data of an ethylene cracking furnace on the premise of considering unsteady state running and time-varying characteristics of the ethylene cracking furnace, thereby effectively monitoring the running state of the ethylene cracking furnace. The method solves the problem of unsteady state change of the sampled data of the ethylene cracking furnace by a technical means of constructing the local abnormal factor of the neighbor in real time, maximizes the difference between the online new sampled data and the reference data set of the neighbor in real time, and judges whether the new sampled data reflects the abnormality of the ethylene cracking furnace. In addition, the method of the invention realizes the real-time update of the monitoring model of the running state of the ethylene cracking furnace by introducing the normal latest sample data into the normal data matrix in real time and deleting the oldest sample data.

Description

Ethylene cracking furnace operation state monitoring method based on neighbor local abnormal factors
Technical Field
The invention relates to a method for monitoring the running state of a chemical process, in particular to a method for monitoring the running state of an ethylene cracking furnace based on a neighbor local abnormal factor.
Background
The ethylene cracking furnace is used for processing cracking gas and is of the types of double radiation chambers, single radiation chambers and millisecond furnaces. The ethylene cracking furnace is the core equipment of an ethylene production device, and mainly has the functions of processing various raw materials such as natural gas, refinery gas, crude oil, naphtha and the like into cracking gas, providing the cracking gas for other ethylene devices, and finally processing the cracking gas into ethylene, propylene and various byproducts. The production capacity and the technical height of the ethylene cracking furnace directly determine the production scale, the yield and the product quality of the whole set of ethylene equipment, so that the ethylene cracking furnace plays a leading role in the ethylene production equipment and even the whole set of petrochemical production.
Therefore, the operation of the ethylene cracking furnace in the expected state (namely, the normal state) plays an important role in the whole ethylene production process, and the real-time monitoring of the operation state of the ethylene cracking furnace is essential. However, conventional monitoring of the operating conditions of ethylene cracking furnaces is accomplished by monitoring changes in one or a few key technical parameters. The monitoring of the change of the key variable according to the univariate thought can only monitor whether a single technical parameter is within an allowable change range in real time, and cannot monitor the running state of the ethylene cracking furnace in real time from the perspective of the whole system.
In addition, in the actual operation of the ethylene cracking furnace, the state of the ethylene cracking furnace is influenced by the fluctuation of the factors such as raw material feeding, steam feeding and the like, so that the operation of the ethylene cracking furnace is unstable. The data collected under this condition are all non-steady state sample data. The traditional data-driven approach assumes a gaussian distribution, which is not true in sample data for ethylene cracking furnaces. Therefore, data-driven monitoring of the operating conditions of ethylene cracking furnaces is known to be a relatively difficult problem. Fortunately, due to the promotion of industrial big data at the present stage, a plurality of measuring instruments and computer-aided systems are installed on the ethylene cracking furnace object, and the sample data can be measured in real time at short intervals. The method lays a full data foundation for implementing data-driven monitoring of the operation state of the ethylene cracking furnace.
In the case of sufficient sampled data volume of the ethylene cracking furnace, the unsteady nature of the process operation causes the gaussian distribution assumption to remain false. However, considering that the abnormal operation state of the ethylene cracking furnace is unknown, and any number of abnormalities or any variable of abnormalities may indicate that the operation state of the ethylene cracking furnace is abnormal. Therefore, the characteristic analysis of the sample data of the ethylene cracking furnace should be carried out on line in real time. In addition, the unsteady state characteristic of the sampled data is further considered, the historical sample data of the ethylene cracking furnace cannot be taken as a whole, and the sample data under the normal operation state of the ethylene cracking furnace can be updated in real time.
Disclosure of Invention
The invention aims to solve the main technical problems that: on the premise of considering the unsteady state operation and the time-varying characteristic of the ethylene cracking furnace, how to perform real-time characteristic analysis on the sampled data of the ethylene cracking furnace is carried out, so that the operation state of the ethylene cracking furnace is effectively monitored. Specifically, the method constructs a near-neighbor local abnormal factor for online sampling data of the ethylene cracking furnace in real time, and monitors whether the running state of the ethylene cracking furnace is abnormal or not by judging whether the abnormal factor is over-limit or not. And then, the sample data in the normal operation state is updated to the reference data set in real time, so that the self-adaptive updating characteristic of the model is ensured.
The technical scheme adopted by the method for solving the problems is as follows: a method for monitoring the running state of an ethylene cracking furnace based on a neighbor local abnormal factor comprises the following steps.
Step (1): obtaining sample data x of n sampling moments of an ethylene cracking furnace in a normal operation state1,x2,…,xnAnd composing it into a data matrix X ═ X of dimension n × m1,x2,…,xn]T(ii) a Wherein, the sample data x of the ith sampling timei∈R33×1The 33 measurement data in the process sequentially comprise the feeding pressure of 6 furnace tube radiation chambers, the feeding flow of 6 furnace tubes, the dilution steam flow of 6 furnace tubes, the discharging temperature of 6 furnace tubes, the cross temperature of 6 furnace tubes, the average discharging temperature of 1 ethylene cracking furnace, the furnace wall gas flow of 1 ethylene cracking furnace and the bottom gas flow of 1 ethylene cracking furnace, i belongs to {1, 2, …, n }, R } in turn33×1A real number vector of 33 × 1 dimensions is represented, R represents a real number set, and the upper symbol T represents a matrix or a transpose of a vector.
Step (2): according to the formula
Figure BSA0000240431340000021
For column vectors z in the data matrix X, respectively1,z2,…,z33Performing normalization to obtain normalized data matrix
Figure BSA0000240431340000022
Wherein z iskAnd
Figure BSA0000240431340000023
respectively represent X and
Figure BSA0000240431340000024
column vector of the kth column, k ∈ {1, 2, …, 33}, μkAnd deltakRespectively representing column vectors zkMean and standard deviation of all elements in (a).
And (3): determining the normal upper limit value Q of the adjacent local abnormal factor according to the following steps (3.1) to (3.6)lim
Step (3.1): the initialization i is 1.
Step (3.2): is provided with
Figure BSA0000240431340000025
Then, X is addediThe row vector of the ith row in the matrix is deleted, thereby obtaining a matrix X consisting of n-1 row vectorsi∈R(n-1)×33(ii) a Wherein R is(n-1)×33A real number matrix representing (n-1) × 33 dimensions.
Step (3.3): calculating XiMiddle row vector and row vector yiDistance between, then XiIs in with yiThe N row vectors with the minimum distance between them form a neighbor reference matrix
Figure BSA0000240431340000026
Wherein R isN×33Representing a matrix of real numbers of Nx 33 dimensions, yiTo represent
Figure BSA0000240431340000027
The row vector of the ith row.
Step (3.4): solving generalized eigenvalue problem
Figure BSA0000240431340000028
Medium maximum eigenvalue lambdaiCorresponding feature vector alphaiThen according to the formula
Figure BSA0000240431340000029
Updating the feature vector alphai
Step (3.5): according to the formula
Figure BSA00002404313400000210
Calculating a nearest neighbor local anomaly factor QiThen, judging whether the condition i is less than n; if yes, setting i to i +1, and then returning to the step (3.2); if not, obtaining Q1,Q2,…,Qn
Step (3.6): will Q1,Q2,…,QnThe maximum value in (1) is recorded as the normal upper limit value Q of the nearest local abnormality factorlim
And (4): at the latest sampling time t, sample data x of the ethylene cracking furnace is collectedt∈R1×33According to the formula
Figure BSA00002404313400000211
For xtEach element in the data is normalized to obtain normalized online data vector
Figure BSA00002404313400000212
Wherein x ist(k) And
Figure BSA00002404313400000213
respectively represent xtAnd
Figure BSA00002404313400000214
the kth element in (1).
And (5): computing
Figure BSA00002404313400000215
Middle row vector and number of linesData vector
Figure BSA00002404313400000216
The distance between the two
Figure BSA00002404313400000217
Neutralization of
Figure BSA00002404313400000218
The N row vectors with the minimum distance between them form a neighbor reference matrix
Figure BSA00002404313400000219
And (6): solving generalized eigenvalue problem
Figure BSA00002404313400000220
Medium maximum eigenvalue lambdatCorresponding feature vector ptThen according to the formula
Figure BSA00002404313400000221
Updating feature vector pt
And (7): according to the formula
Figure BSA00002404313400000222
Calculating the nearest neighbor local anomaly factor Q of the latest sampling time ttThen, whether or not the condition Q is satisfied is judgedt≤Qlim(ii) a If yes, executing step (8); if not, executing step (10).
And (8): according to the formula shown below
Figure BSA0000240431340000031
Row vector y of middle and last n-1 rows2,y3,…,ynAnd
Figure BSA0000240431340000032
after merging into a matrix Y, step (9) is performed.
Figure BSA0000240431340000033
In the above formula, y2,y3,…,ynRespectively represent
Figure BSA0000240431340000034
Line 2 to line n vectors.
And (9): according to the formula
Figure BSA0000240431340000035
Respectively to column vectors in matrix Y
Figure BSA0000240431340000036
Performing normalization to obtain normalized matrix
Figure BSA0000240431340000037
According to the formula
Figure BSA0000240431340000038
And
Figure BSA0000240431340000039
the mean values mu are updated separately1,μ2,…,μ33And standard deviation delta1,δ2,…,δ33Then, set up
Figure BSA00002404313400000310
And returning to the step (4) to continue to monitor the running state of the ethylene cracking furnace at the latest sampling moment; wherein the content of the first and second substances,
Figure BSA00002404313400000311
and η k represent Y and
Figure BSA00002404313400000312
the column vector of the k-th column,
Figure BSA00002404313400000313
and
Figure BSA00002404313400000314
respectively represent column vectors
Figure BSA00002404313400000315
Mean and standard deviation of all elements in (a).
Step (10): returning to the step (4) to continue to monitor the running state of the ethylene cracking furnace at the latest sampling moment until the adjacent local abnormal factors of the continuous 6 latest sampling moments are obtained, and judging whether the 6 adjacent local abnormal factors are all larger than Qlim(ii) a If yes, triggering an abnormal alarm; if not, the operation state of the ethylene cracking furnace is normal, and the step (8) is executed.
In the above implementation steps, step (3.4) and step (6) both involve the problem of generalized eigenvalues with similar calculations. The generalized eigenvalue problem solving is actually a key core process for implementing the construction of the nearest neighbor local anomaly factor. Taking step (3.4) as an example, the so-called neighbor local feature factor is intended to pass through a feature vector αiTo quantize the row vector yiWith respect to neighbor reference matrix
Figure BSA00002404313400000316
Degree of abnormality of (d).
Simply put, it is the neighbor reference matrix
Figure BSA00002404313400000317
Alpha warpiThe range of change is minimized after projective transformation, and the line vector y is simultaneously enablediAlpha warpiThe projective transformation is as maximum as possible. By taking the basic idea of discriminant analysis algorithm as a reference, an objective function can be constructed as follows:
Figure BSA00002404313400000318
without loss of generality, the denominator in the objective function can be set
Figure BSA00002404313400000319
Thus, the above equation can be equivalently transformed into a maximization problem with constraints as shown below:
Figure BSA00002404313400000320
the solution of equation (c) above can use the classical lambertian multiplier method, i.e. construct the lambertian function L as shown below.
Figure BSA00002404313400000321
Then, solve L relative to alphaiAnd set equal to 0, the following equation is obtained:
Figure BSA00002404313400000322
and then converting into a generalized eigenvalue problem in step (3.4):
Figure BSA00002404313400000323
if the two sides of the equation of the generalized eigenvalue problem are multiplied by the left side
Figure BSA00002404313400000324
Then can obtain
Figure BSA00002404313400000325
Thus, λiEqual to the maximum target in the above formula (c), i.e. the generalized eigenvalue problem
Figure BSA0000240431340000041
The largest eigenvalue needs to be calculated.
By carrying out the steps described above, the advantages of the method of the invention are presented below.
The method solves the problem of unsteady state change of the sampled data of the ethylene cracking furnace by a technical means of constructing a neighbor local abnormal factor, maximizes the difference between the online new sampled data and a neighbor reference data set in real time, and judges whether the new sampled data reflects the abnormality of the ethylene cracking furnace. In addition, the method of the invention realizes the real-time update of the monitoring model of the running state of the ethylene cracking furnace by introducing the normal latest sample data into the normal data matrix in real time and deleting the oldest sample data.
Drawings
FIG. 1 is a schematic flow chart of the method of the present invention.
FIG. 2 is a schematic view of an ethylene cracking furnace.
Detailed Description
The present invention will be described in detail below with reference to the accompanying drawings and specific embodiments.
As shown in figure 1, the invention discloses an ethylene cracking furnace operation state monitoring method based on a neighbor local abnormal factor. The following describes a specific embodiment of the method of the present invention in conjunction with a specific application example.
The ethylene cracking furnace shown in fig. 2 is a tap device for producing ethylene in a certain chemical industry in China, and the device comprises 6 furnace tubes, wherein 5 variables which can be measured by each furnace tube specifically comprise: feed pressure, feed flow, dilution steam flow, exit temperature, and crossover temperature of the radiant chamber. Thus, there were 30 measured variables for 6 tubes. In addition, three measurable variables are provided, specifically furnace wall gas flow of the ethylene cracking furnace, bottom gas flow of the ethylene cracking furnace and average discharging temperature of the ethylene cracking furnace. In summary, in this embodiment, 33 measurement data can be acquired at each sampling time, and a 33 × 1 dimensional sample data is formed.
Step (1): acquiring sample data x of n sampling moments of an ethylene cracking furnace in a normal operation state1,x2,…,xnAnd recording it as a data matrix X ═ X in n × m dimensions1,x2,…,xn]T
Step (2): according to the formula
Figure BSA0000240431340000042
For column vectors z in the data matrix X, respectively1,z2,…,z33Performing normalization to obtain normalized data matrix
Figure BSA0000240431340000043
And (3): determining the normal upper limit value Q of the adjacent local abnormal factor according to the steps (3.1) to (3.6)lim
And (4): at the latest sampling time t, sample data x of the ethylene cracking furnace is collectedt∈R1×33According to the formula
Figure BSA0000240431340000044
For xtEach element in the data is normalized to obtain normalized online data vector
Figure BSA0000240431340000045
Wherein x ist(k) And
Figure BSA0000240431340000046
respectively represent xtAnd
Figure BSA0000240431340000047
the kth element in (1).
And (5): computing
Figure BSA0000240431340000048
Middle row vector and on-line data vector
Figure BSA0000240431340000049
The distance between the two
Figure BSA00002404313400000410
Neutralization of
Figure BSA00002404313400000411
The N row vectors with the minimum distance between them form a neighbor reference matrix
Figure BSA00002404313400000412
In step (5), calculating
Figure BSA00002404313400000413
Middle ith row vector yiAnd online data vector
Figure BSA00002404313400000414
The specific embodiments of the distance between are:
Figure BSA0000240431340000051
and (6): solving generalized eigenvalue problem
Figure BSA0000240431340000052
Medium maximum eigenvalue lambdatCorresponding feature vector ptThen according to the formula
Figure BSA0000240431340000053
Updating feature vector pt
And (7): according to the formula
Figure BSA0000240431340000054
Calculating the nearest neighbor local anomaly factor Q of the latest sampling time ttThen, whether or not the condition Q is satisfied is judgedt≤Qlim(ii) a If yes, executing step (8); if not, executing step (10).
And (8): according to the formula
Figure BSA0000240431340000055
Row vector y of middle and last n-1 rows2,y3,…,ynAnd
Figure BSA0000240431340000056
are combined into a matrix Y1Then, step (9) is performed.
And (9): according to the formula
Figure BSA0000240431340000057
Are respectively aligned with matrix Y1Column vector of
Figure BSA0000240431340000058
Performing normalization to obtain normalized matrix
Figure BSA0000240431340000059
According to the formula
Figure BSA00002404313400000510
And
Figure BSA00002404313400000511
the mean values mu are updated separatelykAnd standard deviation deltakThen, set up
Figure BSA00002404313400000512
And returning to the step (4) to continue to monitor the running state of the ethylene cracking furnace at the latest sampling moment.
Step (10): returning to the step (4) to continue to monitor the running state of the ethylene cracking furnace at the latest sampling moment until the adjacent local abnormal factors of the continuous 6 latest sampling moments are obtained, and judging whether the 6 adjacent local abnormal factors are all larger than Qlim(ii) a If yes, triggering an abnormal alarm; if not, the operation state of the ethylene cracking furnace is normal, and the step (8) is executed.

Claims (1)

1. A method for monitoring the running state of an ethylene cracking furnace based on neighbor local abnormal factors is characterized by comprising the following steps:
step (1): acquiring sample data x of n sampling moments of an ethylene cracking furnace in a normal operation state1,x2,…,xnAnd composing it into a data matrix X ═ X in n × m dimensions1,x2,…,xn]T(ii) a Wherein, the sample data x of the ith sampling timei∈R33×1The 33 measurement data specifically comprise the feeding pressure of 6 furnace tube radiation chambers, the feeding flow of 6 furnace tubes, the dilution steam flow of 6 furnace tubes, the discharging temperature of 6 furnace tubes, the crossing temperature of 6 furnace tubes, the average discharging temperature of 1 ethylene cracking furnace, the furnace wall gas flow of 1 ethylene cracking furnace and the bottom gas flow of 1 ethylene cracking furnace, i belongs to {1, 2, …, n }, R } of33×1Representing a real number vector of 33 x 1 dimensions, R representing a real number set, and the upper label T representing a matrix or a transpose of a vector;
step (2): according to the formula
Figure FSA0000240431330000011
For column vectors z in the data matrix X, respectively1,z2,…,z33Performing normalization to obtain normalized data matrix
Figure FSA0000240431330000012
Wherein z iskAnd
Figure FSA0000240431330000013
respectively represent X and
Figure FSA0000240431330000014
column vector of the kth column, k ∈ {1, 2, …, 33}, μkAnd deltakRespectively representing column vectors zkMean and standard deviation of all elements in (a);
and (3): determining the normal upper limit value Q of the adjacent local abnormal factor according to the following steps (3.1) to (3.6)lim
Step (3.1): initializing i to 1;
step (3.2): is provided with
Figure FSA0000240431330000015
Then, X is addediThe row vector of the ith row in the matrix is deleted, thereby obtaining a matrix X consisting of n-1 row vectorsi∈R(n-1)×33(ii) a Wherein R is(n-1)×33Is represented by (n)-1) x 33 dimensional real matrix;
step (3.3): calculating XiMiddle row vector and row vector yiDistance between, then XiIs in with yiThe N row vectors with the minimum distance between them form a neighbor reference matrix
Figure FSA0000240431330000016
Wherein R isN×33Representing a matrix of real numbers of Nx 33 dimensions, yiTo represent
Figure FSA0000240431330000017
A row vector of the ith row;
step (3.4): solving generalized eigenvalue problem
Figure FSA0000240431330000018
Medium maximum eigenvalue lambdaiCorresponding feature vector alphaiThen according to the formula
Figure FSA0000240431330000019
Updating the feature vector alphai
Step (3.5): according to the formula
Figure FSA00002404313300000110
Calculating a nearest neighbor local anomaly factor QiThen, judging whether the condition i is less than n; if yes, setting i to i +1, and then returning to the step (3.2); if not, obtaining Q1,Q2,…,Qn
Step (3.6): will Q1,Q2,…,QnThe maximum value in (1) is recorded as the normal upper limit value Q of the nearest local abnormality factorlim
And (4): at the latest sampling time t, sample data x of the ethylene cracking furnace is collectedt∈R1×33According to the formula
Figure FSA00002404313300000111
For xtEach ofCarrying out standardization processing on each element to obtain an online data vector after standardization processing
Figure FSA00002404313300000112
Wherein x ist(k) And
Figure FSA00002404313300000113
respectively represent xtAnd
Figure FSA00002404313300000114
the kth element in (1);
and (5): computing
Figure FSA00002404313300000115
Middle row vector and on-line data vector
Figure FSA00002404313300000116
The distance between the two
Figure FSA00002404313300000117
Neutralization of
Figure FSA00002404313300000118
The N row vectors with the minimum distance between them form a neighbor reference matrix
Figure FSA00002404313300000119
And (6): solving generalized eigenvalue problem
Figure FSA00002404313300000120
Medium maximum eigenvalue lambdatCorresponding feature vector ptThen according to the formula
Figure FSA00002404313300000121
Updating feature vector pt
And (7): according to the formula
Figure FSA00002404313300000122
Calculating the nearest neighbor local anomaly factor Q of the latest sampling time ttThen, whether or not the condition Q is satisfied is judgedt≤Qlim(ii) a If yes, executing step (8); if not, executing the step (10);
and (8): according to the formula shown below
Figure FSA0000240431330000021
Row vector y of middle and last n-1 rows2,y3,…,ynAnd
Figure FSA0000240431330000022
after the matrix Y is combined, the step (9) is executed;
Figure FSA0000240431330000023
in the above formula, y2,y3,…,ynRespectively represent
Figure FSA0000240431330000024
Line 2 to line n vectors;
and (9): according to the formula
Figure FSA0000240431330000025
Are respectively aligned with matrix Y1Column vector of
Figure FSA0000240431330000026
Performing normalization to obtain normalized matrix
Figure FSA0000240431330000027
According to the formula
Figure FSA0000240431330000028
And
Figure FSA0000240431330000029
the mean values mu are updated separately1,μ2,…,μ33And standard deviation delta1,δ2,…,δ33Then, set up
Figure FSA00002404313300000210
And returning to the step (4) to continue to monitor the running state of the ethylene cracking furnace at the latest sampling moment; wherein the content of the first and second substances,
Figure FSA00002404313300000211
and ηkRespectively represent Y and
Figure FSA00002404313300000212
the column vector of the k-th column,
Figure FSA00002404313300000213
and
Figure FSA00002404313300000214
respectively represent column vectors
Figure FSA00002404313300000215
Mean and standard deviation of all elements in (a);
step (10): returning to the step (4) to continue to monitor the running state of the ethylene cracking furnace at the latest sampling moment until the adjacent local abnormal factors of the continuous 6 latest sampling moments are obtained, and judging whether the 6 adjacent local abnormal factors are all larger than Qlim(ii) a If yes, triggering an abnormal alarm; if not, the operation state of the ethylene cracking furnace is normal, and the step (8) is executed.
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