Image transmission and control method based on dynamic EQ compensation and nuclear radiation resistance

Abstract

The invention discloses an image transmission and control method and device based on dynamic EQ compensation and nuclear radiation resistance, and belongs to the field of data transmission. According to the method, the first loss coefficient used for finely quantifying the influence of environmental nuclear radiation on the transmission performance of the unshielded twisted pair is calculated, the second loss coefficient used for quantifying the comprehensive influence of all environmental factors and signal frequencies on the transmission performance of the unshielded twisted pair is calculated, and the two coefficients are fused. Then, on the basis of the signal frequency of the target video signal and the fused loss coefficient, a cable attenuation coefficient of the unshielded twisted pair is calculated according to a preset composite attenuation model, and an amplitude attenuation factor of the unshielded twisted pair is calculated according to a preset cable transmission function; and performing equalization compensation on the target video signal transmitted by the unshielded twisted pair. The technical effects of dynamically adapting to a complex nuclear radiation environment, dynamically and accurately compensating signal attenuation and remarkably improving the transmission quality and stability of unshielded twisted-pair video signals are achieved.

Description

Technical Field

[0001] The present application relates to the technical field of data transmission, and in particular to a method, device and storage medium for image transmission and control based on dynamic EQ compensation and nuclear radiation resistance. Background Art

[0002] With the rapid development of information technology, video signal transmission plays a vital role in numerous fields, such as security surveillance, video conferencing, and distance education. Unshielded twisted pair (UTP), as a low-cost, easy-to-install, and easy-to-maintain transmission medium, is widely used in video signal transmission. However, in practical applications, UTP still faces some technical challenges in video signal transmission.

[0003] First of all, signal attenuation is a major problem faced when transmitting video signals over unshielded twisted pair cables. Due to the loss of the conductors and the medium itself, the video signal will gradually weaken during transmission. This attenuation will lead to a decline in signal quality, manifested as blurred images, loss of details, and in severe cases, it may even cause the signal to be unable to be correctly received and decoded. The degree of signal attenuation is affected by many factors, including transmission distance, signal frequency, and the quality of the cable itself. In order to address the problem of signal attenuation, the industry has developed some equalization compensation solutions. For example, the patent application with publication number CN103139526A and invention name "System and method for cable equalization" receives the video signal transmitted on the cable through an equalizer, provides compensation for the frequency attenuation that occurs during transmission on the cable, and outputs the compensated video signal. For example, the patent application with publication number CN101667412A and invention name "Signal compensation device, signal compensation method and multi-computer switching system" solves the problems of ghosting and overexcitation caused by distance in signal transmission by using a combination of a de-differentializing unit, a detection unit, a control unit, a filter and an equalizer in the signal compensation device, thereby achieving accurate compensation of the video signal and maintaining picture clarity.

[0004] It's important to note that nuclear radiation interference is also a significant factor affecting the quality of video signal transmission over unshielded twisted-pair cables. Common types of nuclear radiation include alpha, beta, gamma, neutrons, and X-rays. These radiations can couple onto unshielded twisted-pair cables, interfering with video signals and causing degradation, noise, distortion, and other issues. The intensity and type of nuclear radiation interference depend on environmental factors, making signal transmission quality uncertain and volatile. However, existing equalization and compensation solutions often fail to fully account for the impact of nuclear radiation interference and lack dynamic compensation mechanisms for this interference.

[0005] The existing equalization compensation scheme for unshielded twisted-pair video signal transmission lacks a dynamic compensation mechanism for nuclear radiation interference, and a corresponding technical solution is urgently needed. Summary of the Invention

[0006] The embodiments of the present disclosure provide a method and device for image transmission and control based on dynamic EQ compensation and nuclear radiation resistance, so as to at least solve the technical problem in the prior art that the equalization compensation scheme for unshielded twisted pair video signal transmission lacks a dynamic compensation mechanism for nuclear radiation interference.

[0007] According to one aspect of an embodiment of the present disclosure, a method for image transmission and control based on dynamic EQ compensation and nuclear radiation resistance is provided, comprising: collecting intensity values ​​of various types of nuclear radiation in an environment in which an unshielded twisted pair is located, and determining a first conductor loss coefficient and a first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of various types of nuclear radiation; transmitting a target video signal to which a first test pulse signal is added through the unshielded twisted pair, and determining a second conductor loss coefficient and a second dielectric loss coefficient of the unshielded twisted pair based on the loss of the first test pulse signal in the transmitted target video signal; fusing the first conductor loss coefficient with the second conductor loss coefficient to obtain a third conductor loss coefficient; fusing the first dielectric loss coefficient with the second dielectric loss coefficient to obtain a third dielectric loss coefficient; determining a cable attenuation coefficient of the unshielded twisted pair according to a preset composite attenuation model based on the signal frequency of the target video signal, the third conductor loss coefficient and the third dielectric loss coefficient; and calculating an amplitude attenuation factor of the unshielded twisted pair according to a preset cable transmission function based on the cable attenuation coefficient, and performing equalization compensation on the target video signal after transmission through the unshielded twisted pair based on the amplitude attenuation factor.

[0008] According to another aspect of an embodiment of the present disclosure, a storage medium is further provided, the storage medium including a stored program, wherein when the program is run, a processor executes any one of the above methods.

[0009] According to another aspect of the embodiment of the present disclosure, there is also provided an image transmission and control device based on dynamic EQ compensation and nuclear radiation resistance, comprising: a first determination module for collecting intensity values ​​of various types of nuclear radiation in the environment in which the unshielded twisted pair is located, and determining a first conductor loss coefficient and a first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of various types of nuclear radiation; a second determination module for transmitting a target video signal to which a first test pulse signal is added through the unshielded twisted pair, and determining a second conductor loss coefficient and a second dielectric loss coefficient of the unshielded twisted pair according to the loss of the first test pulse signal in the target video signal after transmission; a fusion module for combining the first conductor loss coefficient and the second dielectric loss coefficient The first dielectric loss coefficient is merged with the second dielectric loss coefficient to obtain a third conductor loss coefficient; the first dielectric loss coefficient is merged with the second dielectric loss coefficient to obtain a third dielectric loss coefficient; a third determination module is used to determine the cable attenuation coefficient of the unshielded twisted pair according to a preset composite attenuation model based on the signal frequency of the target video signal, the third conductor loss coefficient and the third dielectric loss coefficient; and a balanced compensation module is used to calculate the amplitude attenuation factor of the unshielded twisted pair according to a preset cable transmission function based on the cable attenuation coefficient, and perform balanced compensation on the target video signal after transmission through the unshielded twisted pair based on the amplitude attenuation factor.

[0010] According to another aspect of the embodiment of the present disclosure, there is also provided an image transmission and control device based on dynamic EQ compensation and nuclear radiation resistance, comprising: a processor; and a memory connected to the processor, for providing the processor with instructions for processing the following processing steps: collecting intensity values ​​of various types of nuclear radiation in the environment in which the unshielded twisted pair is located, and determining the first conductor loss coefficient and the first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of the various types of nuclear radiation; transmitting a target video signal to which a first test pulse signal is added through the unshielded twisted pair, and determining the second conductor loss coefficient and the second dielectric loss coefficient of the unshielded twisted pair according to the loss of the first test pulse signal in the target video signal after transmission. dielectric loss coefficient; fusing the first conductor loss coefficient with the second conductor loss coefficient to obtain a third conductor loss coefficient; fusing the first dielectric loss coefficient with the second dielectric loss coefficient to obtain a third dielectric loss coefficient; based on the signal frequency of the target video signal, the third conductor loss coefficient and the third dielectric loss coefficient, determining the cable attenuation coefficient of the unshielded twisted pair according to a preset composite attenuation model; and based on the cable attenuation coefficient, calculating the amplitude attenuation factor of the unshielded twisted pair according to a preset cable transmission function, and performing equalization compensation on the target video signal after transmission through the unshielded twisted pair based on the amplitude attenuation factor.

[0011] This application first collects the intensity values ​​of various types of nuclear radiation in the environment of an unshielded twisted pair cable and dynamically calculates the first conductor loss coefficient and first dielectric loss coefficient of the unshielded twisted pair cable based on the nuclear radiation intensity values. This is used to precisely quantify the impact of environmental nuclear radiation on the transmission performance of the unshielded twisted pair cable. Next, a target video signal with a first test pulse signal added is transmitted through the unshielded twisted pair cable. Based on the loss of the first test pulse signal in the transmitted target video signal, the second conductor loss coefficient and second dielectric loss coefficient of the unshielded twisted pair cable are determined to quantify the combined impact of signal frequency and all environmental factors on the transmission performance of the unshielded twisted pair cable. Secondly, the first loss coefficient (including the first conductor loss coefficient and the first dielectric loss coefficient), which precisely quantifies the impact of environmental nuclear radiation, is combined with the second loss coefficient (including the second conductor loss coefficient and the second dielectric loss coefficient), which comprehensively reflects the impact of environmental factors and signal frequency. This results in a composite loss coefficient (including the third conductor loss coefficient and the third dielectric loss coefficient) that can dynamically adapt to complex electromagnetic environments and is used for subsequent calculation of the cable attenuation coefficient. Secondly, based on the signal frequency of the target video signal, the third conductor loss coefficient, and the third dielectric loss coefficient, the cable attenuation coefficient of the unshielded twisted pair is calculated according to a preset composite attenuation model, which is used for subsequent calculation of the signal attenuation loss value. Finally, based on the cable attenuation coefficient, the amplitude attenuation factor of the unshielded twisted pair is calculated according to a preset cable transmission function. Based on this amplitude attenuation factor, the target video signal after transmission through the unshielded twisted pair is equalized and compensated to restore the original quality of the target video signal. This achieves the technical effects of dynamically adapting to complex nuclear radiation environments, dynamically and accurately compensating for signal attenuation, and significantly improving the quality and stability of unshielded twisted pair video signal transmission. This solves the technical problem that the existing equalization compensation scheme for unshielded twisted pair video signal transmission lacks a dynamic compensation mechanism for nuclear radiation interference. BRIEF DESCRIPTION OF THE DRAWINGS

[0012] The drawings described herein are used to provide a further understanding of the present disclosure and constitute a part of this application. The illustrative embodiments of the present disclosure and their descriptions are used to explain the present disclosure and do not constitute an improper limitation of the present disclosure. In the drawings: Figure 1 is a hardware structure block diagram of a computing device for implementing the method according to embodiment 1 of the present disclosure; Figure 2 is a flow chart of the image transmission and control method based on dynamic EQ compensation and nuclear radiation resistance according to Example 1 of the present application; Figure 3 is a schematic diagram of an image transmission and control device based on dynamic EQ compensation and nuclear radiation resistance according to Example 2 of the present application; Figure 4This is a schematic diagram of the image transmission and control device based on dynamic EQ compensation and nuclear radiation resistance according to Example 3 of the present application. DETAILED DESCRIPTION

[0013] In order to enable those skilled in the art to better understand the technical solutions of the present disclosure, the technical solutions in the embodiments of the present disclosure will be clearly and completely described below in conjunction with the drawings in the embodiments of the present disclosure. Obviously, the described embodiments are only part of the embodiments of the present disclosure, not all of the embodiments. Based on the embodiments of the present disclosure, all other embodiments obtained by ordinary technicians in this field without making creative efforts should fall within the scope of protection of the present disclosure.

[0014] It should be noted that the terms "first", "second", etc. in the specification and claims of the present disclosure and the above-mentioned drawings are used to distinguish similar objects and are not necessarily used to describe a specific order or sequence. It should be understood that the numbers used in this way can be interchanged where appropriate, so that the embodiments of the present disclosure described herein can be implemented in an order other than those illustrated or described herein. In addition, the terms "including" and "having" and any variations thereof are intended to cover non-exclusive inclusions, for example, a process, method, system, product or device that includes a series of steps or units is not necessarily limited to those steps or units clearly listed, but may include other steps or units that are not clearly listed or inherent to these processes, methods, products or devices.

[0015] Example 1 According to this embodiment, a method embodiment of an image transmission and control method based on dynamic EQ compensation and nuclear radiation resistance is provided. It should be noted that the steps shown in the flowchart of the accompanying drawings can be executed in a computer system such as a set of computer executable instructions, and although a logical order is shown in the flowchart, in some cases, the steps shown or described can be executed in an order different from that shown here.

[0016] The method embodiment provided in this embodiment can be executed in a server or similar computing device. Figure 1 The hardware structure block diagram of a computing device for implementing a method for image transmission and control based on dynamic EQ compensation and nuclear radiation resistance is shown. Figure 1As shown, a computing device may include one or more processors (the processor may include, but is not limited to, a microprocessor (MCU) or a programmable logic device (FPGA) or other processing device), a memory for storing data, a transmission device for communication functions, and an input / output interface. The memory, transmission device, and input / output interface are connected to the processor via a bus. In addition, it may also include: a display, a keyboard, and a cursor control device connected to the input / output interface. Those skilled in the art will understand that Figure 1 The structure shown is only for illustration and does not limit the structure of the above electronic device. Figure 1 More or fewer components than shown, or with Figure 1 Different configurations shown.

[0017] It should be noted that the one or more processors and / or other data processing circuits described above may generally be referred to herein as "data processing circuitry." The data processing circuitry may be embodied in whole or in part as software, hardware, firmware, or any other combination thereof. Furthermore, the data processing circuitry may be a single, independent processing module, or may be fully or partially integrated into any of the other components of the computing device. As discussed in the embodiments of the present disclosure, the data processing circuitry functions as a processor control (e.g., selection of a variable resistor terminal path connected to an interface).

[0018] The memory can be used to store software programs and modules for application software, such as the program instructions / data storage device corresponding to the dynamic EQ compensation and radiation-resistant image transmission and control method described in the embodiments of the present disclosure. The processor executes the software programs and modules stored in the memory to perform various functional applications and data processing, thereby implementing the dynamic EQ compensation and radiation-resistant image transmission and control method described in the application. The memory can include high-speed random access memory (RAM) and non-volatile memory, such as one or more magnetic storage devices, flash memory, or other non-volatile solid-state memory. In some embodiments, the memory can further include memory remotely located from the processor, which can be connected to the computing device via a network. Examples of such networks include, but are not limited to, the Internet, corporate intranets, local area networks, mobile communication networks, and combinations thereof.

[0019] The transmission device is used to receive or send data via a network. Specific examples of the aforementioned network may include a wireless network provided by a communications provider of the computing device. In one embodiment, the transmission device includes a network interface controller (NIC), which can be connected to other network devices via a base station to enable communication with the Internet. In another embodiment, the transmission device may be a radio frequency (RF) module, which is used to communicate with the Internet wirelessly.

[0020] The display may be, for example, a touch screen liquid crystal display (LCD) that enables a user to interact with a user interface of the computing device.

[0021] It should be noted that, in some optional embodiments, the above Figure 1 The computing device shown may include hardware elements (including circuits), software elements (including computer code stored on a computer-readable medium), or a combination of both hardware and software elements. Figure 1 This is merely one example of a particular embodiment and is intended to illustrate the types of components that may be present in the computing device described above.

[0022] In the above operating environment, according to the first aspect of this embodiment, a method for image transmission and control based on dynamic EQ compensation and nuclear radiation resistance is provided. Figure 2 A schematic diagram showing the process of the method is shown in FIG. Figure 2 As shown, the method includes: S202: collecting intensity values ​​of various types of nuclear radiation in an environment where the unshielded twisted pair is located, and determining a first conductor loss coefficient and a first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of the various types of nuclear radiation; S204: Transmitting the target video signal to which the first test pulse signal is added through the unshielded twisted pair cable, and determining a second conductor loss coefficient and a second dielectric loss coefficient of the unshielded twisted pair cable based on a loss condition of the first test pulse signal in the transmitted target video signal; S206: Merging the first conductor loss coefficient and the second conductor loss coefficient to obtain a third conductor loss coefficient; and merging the first dielectric loss coefficient and the second dielectric loss coefficient to obtain a third dielectric loss coefficient. S208: Determine a cable attenuation coefficient of the unshielded twisted pair according to a preset composite attenuation model based on the signal frequency of the target video signal, the third conductor loss coefficient, and the third dielectric loss coefficient; and S210: Based on the cable attenuation coefficient, calculate the amplitude attenuation factor of the unshielded twisted pair according to a preset cable transmission function, and perform equalization compensation on the target video signal transmitted through the unshielded twisted pair based on the amplitude attenuation factor.

[0023] Specifically, nuclear radiation intensity sensors can be pre-placed around unshielded twisted-pair cables to ensure comprehensive coverage and accurate capture of all types of nuclear radiation affecting the cables. When video signals need to be transmitted via unshielded twisted-pair cables, sensors can be used to monitor the transmission environment in real time to obtain information on the intensity of various types of nuclear radiation present in the environment. Subsequently, based on this collected nuclear radiation intensity data, a series of calculations and analyses are performed to determine the conductor and dielectric loss characteristics of the unshielded twisted-pair cables under the influence of nuclear radiation. This yields a first conductor loss coefficient and a first dielectric loss coefficient that can precisely quantify the loss of the unshielded twisted-pair cables in a specific nuclear radiation environment, providing basic data for subsequent steps.

[0024] The first test pulse signal is then superimposed on the target video signal. After transmission through the unshielded twisted pair cable, the amplitude attenuation of each frequency component in the first test pulse signal is analyzed at the receiving end using a Fourier transform. By analyzing the amplitude attenuation of each frequency component, the second conductor loss coefficient and second dielectric loss coefficient of the unshielded twisted pair cable in actual transmission scenarios can be calculated. This quantifies the combined impact of signal frequency and all environmental factors on the transmission performance of the unshielded twisted pair cable, providing dynamic data support for cable performance evaluation.

[0025] Next, considering the frequency characteristics of the target video signal to be transmitted, combined with the loss coefficient obtained through fusion processing, the cable attenuation coefficient of the unshielded twisted pair is determined through a preset composite attenuation model to establish a direct connection between signal frequency and line loss, providing a key parameter for quantifying the attenuation degree of the video signal during transmission. The expression of the composite attenuation model is:

[0026] Where, is the cable attenuation coefficient of the unshielded twisted pair, k1 is the third conductor loss coefficient of the unshielded twisted pair, k2 is the third dielectric loss coefficient of the unshielded twisted pair, and f is the signal frequency of the target video signal to be transmitted.

[0027] Finally, based on the determined cable attenuation coefficient, the amplitude attenuation factor of the unshielded twisted pair cable is calculated using the existing cable transfer function. Subsequently, equalization compensation is performed on the target video signal after transmission over the unshielded twisted pair cable at the receiving end. This compensation mechanism eliminates signal attenuation during transmission, ensuring that the video signal is restored to near-original quality at the receiving end, achieving clear and stable video signal transmission. The cable transfer function is:

[0028] Where, Amplitude attenuation factor of unshielded twisted pair, is the cable attenuation coefficient of the unshielded twisted pair cable, and L is the length of the unshielded twisted pair cable.

[0029] As mentioned in the background, nuclear radiation interference is also a significant factor affecting the quality of video signal transmission over unshielded twisted-pair cables. Common types of nuclear radiation include alpha, beta, gamma, neutrons, and X-rays. These radiations can couple onto unshielded twisted-pair cables, interfering with video signals and causing degradation of signal quality, noise, distortion, and other issues. The intensity and type of nuclear radiation interference depend on environmental factors, making signal transmission quality uncertain and volatile. However, existing equalization and compensation schemes often fail to fully account for the impact of nuclear radiation interference and lack dynamic compensation mechanisms for this interference.

[0030] In light of this, this application first collects the intensity values ​​of various types of nuclear radiation in the environment of an unshielded twisted pair cable and dynamically calculates the first conductor loss coefficient and first dielectric loss coefficient of the unshielded twisted pair cable based on the nuclear radiation intensity values. This is used to precisely quantify the impact of environmental nuclear radiation on the transmission performance of the unshielded twisted pair cable. Next, a target video signal with a first test pulse signal added is transmitted through the unshielded twisted pair cable. Based on the loss of the first test pulse signal in the transmitted target video signal, the second conductor loss coefficient and second dielectric loss coefficient of the unshielded twisted pair cable are determined to quantify the combined impact of signal frequency and all environmental factors on the transmission performance of the unshielded twisted pair cable. Secondly, the first loss coefficient (including the first conductor loss coefficient and the first dielectric loss coefficient), which precisely quantifies the impact of environmental nuclear radiation, is combined with the second loss coefficient (including the second conductor loss coefficient and the second dielectric loss coefficient), which comprehensively reflects the influence of environmental factors and signal frequency. This results in a composite loss coefficient (including the third conductor loss coefficient and the third dielectric loss coefficient) that can dynamically adapt to complex electromagnetic environments and is used for subsequent calculation of the cable attenuation coefficient. Secondly, based on the signal frequency of the target video signal, the third conductor loss coefficient, and the third dielectric loss coefficient, the cable attenuation coefficient of the unshielded twisted pair is calculated according to a preset composite attenuation model, which is used for subsequent calculation of the signal attenuation loss value. Finally, based on the cable attenuation coefficient, the amplitude attenuation factor of the unshielded twisted pair is calculated according to a preset cable transmission function. Based on this amplitude attenuation factor, the target video signal after transmission through the unshielded twisted pair is equalized and compensated to restore the original quality of the target video signal. This achieves the technical effects of dynamically adapting to complex nuclear radiation environments, dynamically and accurately compensating for signal attenuation, and significantly improving the quality and stability of unshielded twisted pair video signal transmission. This solves the technical problem that the existing equalization compensation scheme for unshielded twisted pair video signal transmission lacks a dynamic compensation mechanism for nuclear radiation interference.

[0031] Optionally, the operation of determining the first conductor loss coefficient and the first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of various types of nuclear radiation includes: calculating the first conductor loss coefficient of the unshielded twisted pair based on the intensity values ​​of various types of nuclear radiation using a first formula; wherein the first formula is:

[0032] Among them, k 11 is the first conductor loss coefficient of the unshielded twisted pair; x0 is the initial conductor loss coefficient of the unshielded twisted pair in a non-nuclear radiation environment; I i is the intensity value of the i-th type of nuclear radiation; x i is a constant term of the intensity value of the i-th type of nuclear radiation, and the constant term is a preset value; n is the number of types of nuclear radiation in the environment where the unshielded twisted pair is located; Based on the intensity values ​​of various types of nuclear radiation, a first dielectric loss coefficient of the unshielded twisted pair is calculated using a second formula; wherein the second formula is:

[0033] Among them, k 21 is the first dielectric loss coefficient of the unshielded twisted pair; y0 is the initial dielectric loss coefficient of the unshielded twisted pair in a non-nuclear radiation environment; I i is the intensity value of the i-th type of nuclear radiation; y i is a constant term of the intensity value of the i-th type of nuclear radiation, and the constant term is a preset value; n is the number of types of nuclear radiation in the environment where the unshielded twisted pair is located.

[0034] Specifically, in practical applications, unshielded twisted-pair cables are often exposed to complex nuclear radiation environments. Considering the impact of these radiation sources can more accurately assess the transmission performance of unshielded twisted-pair cables in actual use. Therefore, after collecting the radiation intensity value, a preset mathematical model (including the first and second formulas described above) is used to convert the radiation intensity value into the conductor loss coefficient and dielectric loss coefficient of the unshielded twisted-pair cable. By incorporating the radiation intensity value and related constant terms, this preset mathematical model can more accurately calculate the first conductor loss coefficient and first dielectric loss coefficient of the unshielded twisted-pair cable in a specific nuclear radiation environment.

[0035] The first conductor loss factor k 11 It represents the conductor loss coefficient of unshielded twisted pair cables in a specific nuclear radiation environment. It is a comprehensive indicator that reflects the signal attenuation caused by various factors (including nuclear radiation) when transmitting signals in unshielded twisted pair cables. Therefore, in the first formula, the initial conductor loss coefficient x0 of unshielded twisted pair cables in a nuclear radiation-free environment is used as the reference value. This is the inherent conductor loss of unshielded twisted pair cables in an ideal environment without any nuclear radiation interference. In the first formula, the different effects of different types of nuclear radiation on unshielded twisted pair cables are also considered, and a specific constant term x is set for each type of nuclear radiation. i .

[0036] k 21 represents the dielectric loss coefficient of the unshielded twisted pair in a specific nuclear radiation environment. In the second formula, the initial dielectric loss coefficient y0 of the unshielded twisted pair in a non-nuclear radiation environment is used as the reference value. This reference value is the inherent dielectric loss of the unshielded twisted pair in an ideal environment without any nuclear radiation interference. In the second formula, the different effects of different types of nuclear radiation on the unshielded twisted pair are also considered, and a specific constant term y is set for each type of nuclear radiation. i .

[0037] Therefore, by introducing the nuclear radiation intensity value and related constant terms, the conductor loss and dielectric loss of unshielded twisted pair cables in a specific nuclear radiation environment can be calculated more accurately, which helps to formulate a more reasonable signal transmission compensation strategy and improve the reliability and stability of signal transmission.

[0038] Optionally, the constants in the first formula and the second formula are determined by the following steps: in a non-nuclear radiation test environment, transmitting a second test pulse signal of different frequencies through the unshielded twisted pair, and performing a loss analysis on the second test pulse signal after transmission, and determining the initial conductor loss coefficient and the initial dielectric loss coefficient of the unshielded twisted pair according to the results of the loss analysis; in a nuclear radiation test environment, transmitting a second test pulse signal of different frequencies through the unshielded twisted pair, and performing a loss analysis on the second test pulse signal after transmission, and determining multiple groups of loss coefficients of the unshielded twisted pair according to the results of the loss analysis; wherein each group of loss coefficients includes a test conductor loss coefficient and a test dielectric loss coefficient; collecting the test intensity values ​​of various types of nuclear radiation in the nuclear radiation test environment, setting the constants in the first formula and the second formula as unknown quantities, substituting the test intensity values ​​of various types of nuclear radiation, the multiple groups of loss coefficients, the initial conductor loss coefficient and the initial dielectric loss coefficient into the first formula and the second formula, and solving the constants in the first formula and the second formula.

[0039] Specifically, in a non-nuclear radiation test environment (e.g., in a shielded room), second test pulse signals (f1, f2, ..., fn) of different frequencies are transmitted through an unshielded twisted pair cable. The ends of the unshielded twisted pair cable (length L) are connected to Port 1 and Port 2 of a vector network analyzer (VNA). The vector network analyzer sends a frequency sweep signal (e.g., 1 MHz step) and records the frequency at each frequency point f i Insertion loss S 21 (f i ). Then, calculate each frequency point f by the following formula i Cable attenuation coefficient of unshielded twisted pair cable :

[0040] Next, each frequency point f i Cable attenuation coefficient of unshielded twisted pair cable Substituting the composite attenuation model, we obtain the overdetermined equations:

[0041] The above overdetermined equations are solved using the least squares method to ultimately obtain k1 and k2 under a non-nuclear radiation test environment. Thus, k1 under a non-nuclear radiation test environment is determined as the initial conductor loss coefficient x0 of the unshielded twisted pair cable, and k2 under a non-nuclear radiation test environment is determined as the initial dielectric loss coefficient y0 of the unshielded twisted pair cable.

[0042] Through the above steps, the initial conductor loss coefficient x0 and the initial dielectric loss coefficient y0 of the unshielded twisted pair cable in a non-nuclear radiation environment can be accurately measured.

[0043] Next, multiple types of nuclear radiation sources were introduced into the shielded room, and then the intensity value of each type of nuclear radiation source was accurately measured using a spectrum analyzer and an electromagnetic field probe. (Unit: dBμV / m) and record its frequency band characteristics. Then, send a second test pulse signal with multiple frequency groups (covering the target frequency band, such as 1MHz-150MHz), with each frequency group corresponding to a test point. For example, send pulse signals with frequencies of 10MHz, 50MHz, and 100MHz, and repeat the test three times at each frequency point to reduce random errors. Use a vector network analyzer (VNA) to measure the insertion loss (S 21 parameters), and each frequency point f i Cable attenuation coefficient of unshielded twisted pair cable After that, each frequency point f i Cable attenuation coefficient of unshielded twisted pair cable Substituting the composite attenuation model into the corresponding set of equations, we solved them using the least squares method to obtain k1 and k2 under the nuclear radiation test environment. Repeating the above method for multiple rounds of experiments yielded k1 and k2 under multiple sets of nuclear radiation test environments.

[0044] Assume that the constants in the first formula are unknown quantities, and take k1 in the nuclear radiation test environment as the first conductor loss coefficient k of the unshielded twisted pair cable. 11 , the initial conductor loss coefficient x0 and k1 under multiple groups of nuclear radiation test environments obtained above are respectively substituted into the first formula to obtain the corresponding overdetermined equations and solve them to obtain the specific values ​​of the constants in the first formula.

[0045] Similarly, set the constants in the second formula as unknown quantities, and treat k2 in the nuclear radiation test environment as the first dielectric loss coefficient k of the unshielded twisted pair cable. 21 , the initial dielectric loss coefficient y0 and k2 under multiple groups of nuclear radiation test environments obtained above are respectively substituted into the first formula to obtain the corresponding overdetermined equations and solve them to obtain the specific values ​​of the constants in the second formula.

[0046] In this way, the constants in the first and second formulas can be accurately determined.

[0047] Optionally, the operation of fusing the first conductor loss coefficient and the second conductor loss coefficient to obtain a third conductor loss coefficient includes: fusing the first conductor loss coefficient and the second conductor loss coefficient using a third formula to obtain the third conductor loss coefficient; wherein the third formula is:

[0048] Wherein, k1 is the loss coefficient of the third conductor of the unshielded twisted pair; k 11 k is the first conductor loss factor of the unshielded twisted pair; 12 is the loss factor of the second conductor of the unshielded twisted pair; and is the weight coefficient, + =1; The first dielectric loss coefficient and the second dielectric loss coefficient are combined using a fourth formula to obtain a third dielectric loss coefficient; wherein the fourth formula is:

[0049] Wherein, k2 is the third dielectric loss coefficient of the unshielded twisted pair cable; k 21 k is the first dielectric loss coefficient of the unshielded twisted pair; 22 is the second dielectric loss coefficient of the unshielded twisted pair; and is the weight coefficient, + =1.

[0050] In the embodiment of the present invention, the weight coefficient is determined by the following steps: 、 、 and : (1) Prepare M test samples. The mth test sample includes the frequencies that need to be transmitted in a nuclear radiation test environment. , ,…, The test pulse signal, the intensity value of each type of nuclear radiation source in the nuclear radiation test environment , ,…, ( is the number of types of nuclear radiation sources), and each frequency point The actual cable attenuation coefficient of unshielded twisted pair cable ; (2) Intensity value of each type of nuclear radiation source , ,…, In the nuclear radiation test environment, the test pulse signals of different frequencies ( , ,…, ) is transmitted through an unshielded twisted pair cable. The ends of the unshielded twisted pair cable (length L) are connected to Port 1 and Port 2 of the vector network analyzer (VNA). The vector network analyzer sends a sweep frequency signal (for example, 1 MHz step) and records each frequency point. Insertion loss Then, calculate each frequency point through the corresponding formula Test cable attenuation coefficient of unshielded twisted pair cable ; (3) The frequency points of the mth test sample Test cable attenuation coefficient of unshielded twisted pair cable Substitute the composite attenuation model into the composite attenuation model to obtain the following expression:

[0051] (4) Calculate the loss value of all test samples using the following formula:

[0052] (5) Using the gradient descent algorithm, update the parameters of the composite attenuation model according to the calculated loss value 、 、 and , iterative optimization until the loss value converges to the minimum value or reaches the preset number of iterations / accuracy threshold.

[0053] Optionally, the target video signal with the first test pulse signal added thereto is transmitted through the unshielded twisted pair, and the second conductor loss coefficient and the second dielectric loss coefficient of the unshielded twisted pair are determined based on the loss of the first test pulse signal in the target video signal after transmission, including: generating a first test pulse signal containing multiple different frequency components, and adding the first test pulse signal to the target video signal to be transmitted; transmitting the target video signal with the first test pulse signal added thereto through the unshielded twisted pair; performing a fast Fourier transform on the first test pulse signal before and after transmission to obtain amplitude information of the first test pulse signal on each frequency component before and after transmission; comparing the amplitude changes of each frequency component in the first test pulse signal before and after transmission, and determining the cable attenuation coefficient when the unshielded twisted pair transmits the corresponding frequency component based on the amplitude changes; substituting the cable attenuation coefficient when the unshielded twisted pair transmits each frequency component and the frequency value of each frequency component into the following equation to solve the second conductor loss coefficient and the second dielectric loss coefficient:

[0054] Where, is the cable attenuation coefficient when the unshielded twisted pair transmits the i-th frequency component; is the frequency value of the i-th frequency component; k 12 k is the loss factor of the second conductor; 22 is the second dielectric loss coefficient.

[0055] Specifically, a first test pulse signal (such as a swept frequency signal or a comb spectrum signal) is generated, containing multiple frequency components. This signal covers the critical frequency band of the video signal (e.g., 0-6 MHz) to comprehensively evaluate the cable's transmission characteristics for different frequency components. A signal synthesizer then embeds the test pulses into the target video signal using a low-amplitude, high-frequency modulation scheme. For example, the test pulses can be inserted between the horizontal sync pulses of the video signal, taking advantage of the absence of valid image information during this period to avoid visible interference with the video content.

[0056] Next, an unshielded twisted pair (UTP) cable is connected to a signal generator and a receiving device. The target video signal, supplemented with the first test pulse signal, is transmitted over the cable. At the transmitting end, a Fourier transform is performed on the original first test pulse signal, recording the initial amplitude of each frequency component to establish a spectral baseline. At the receiving end, a Fourier transform is performed on the transmitted first test pulse signal to extract the residual amplitude of each frequency component. By comparing the spectra before and after transmission, the loss of each frequency component can be quantified.

[0057] For each frequency component , calculate the amplitude attenuation :

[0058] Where, Indicates frequency components Energy attenuation due to cable loss during transmission (unit: dB); Indicates frequency components The residual amplitude of Indicates frequency components The remaining initial amplitude.

[0059] Converting amplitude attenuation to cable attenuation coefficient in the linear domain :

[0060] Where, Reflects the frequency components of unshielded twisted pair The total loss (including conductor, dielectric and nuclear radiation coupling loss).

[0061] Next, each frequency component Cable attenuation coefficient of unshielded twisted pair cable Introducing the composite attenuation model , get the corresponding overdetermined equations, solve to get the second conductor loss coefficient k 12 and the second dielectric loss coefficient k 22 .

[0062] In this way, the loss factor k of the second conductor of an unshielded twisted pair can be accurately determined. 12 and the second dielectric loss coefficient k 22 .

[0063] In addition, reference Figure 1 As shown, according to a second aspect of this embodiment, a storage medium is provided, wherein the storage medium includes a stored program, wherein when the program is run, a processor executes any one of the above methods.

[0064] It should be noted that for the aforementioned method embodiments, for simplicity of description, they are all expressed as a series of action combinations. However, those skilled in the art should be aware that the present invention is not limited by the order of the actions described, because according to the present invention, certain steps can be performed in other orders or simultaneously. Secondly, those skilled in the art should also be aware that the embodiments described in this specification are all preferred embodiments, and the actions and modules involved are not necessarily required by the present invention.

[0065] Through the description of the above embodiments, those skilled in the art will clearly understand that the methods according to the above embodiments can be implemented using software plus the necessary general-purpose hardware platform. Of course, hardware can also be used, but in many cases the former is a more preferred embodiment. Based on this understanding, the technical solution of the present invention, or the portion that contributes to the prior art, can be embodied in the form of a software product. This computer software product is stored in a storage medium (such as ROM / RAM, magnetic disk, or optical disk) and includes a number of instructions for enabling a terminal device (which can be a mobile phone, computer, server, or network device, etc.) to execute the methods described in various embodiments of the present invention.

[0066] Example 2 Figure 3 The image transmission and control device based on dynamic EQ compensation and nuclear radiation resistance according to this embodiment is shown, which corresponds to the method according to embodiment 1. Figure 3 As shown, the device includes: a first determination module 310, which is used to collect intensity values ​​of various types of nuclear radiation in the environment where the unshielded twisted pair is located, and determine the first conductor loss coefficient and the first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of the various types of nuclear radiation; a second determination module 320, which is used to transmit the target video signal with the first test pulse signal added through the unshielded twisted pair, and determine the second conductor loss coefficient and the second dielectric loss coefficient of the unshielded twisted pair according to the loss of the first test pulse signal in the target video signal after transmission; a fusion module 330, which is used to fuse the first conductor loss coefficient with the second conductor loss coefficient , obtaining a third conductor loss coefficient; fusing the first dielectric loss coefficient with the second dielectric loss coefficient to obtain a third dielectric loss coefficient; a third determination module 340, used to determine the cable attenuation coefficient of the unshielded twisted pair according to a preset composite attenuation model based on the signal frequency of the target video signal, the third conductor loss coefficient and the third dielectric loss coefficient; and an equalization compensation module 350, used to calculate the amplitude attenuation factor of the unshielded twisted pair according to a preset cable transmission function based on the cable attenuation coefficient, and perform equalization compensation on the target video signal after transmission through the unshielded twisted pair based on the amplitude attenuation factor.

[0067] Optionally, the first determining module 310 is specifically configured to calculate a first conductor loss coefficient of the unshielded twisted pair cable using a first formula based on intensity values ​​of various types of nuclear radiation; wherein the first formula is:

[0068] Among them, k 11is the first conductor loss coefficient of the unshielded twisted pair; x0 is the initial conductor loss coefficient of the unshielded twisted pair in a non-nuclear radiation environment; I i is the intensity value of the i-th type of nuclear radiation; x i is a constant term of the intensity value of the i-th type of nuclear radiation, and the constant term is a preset value; n is the number of types of nuclear radiation in the environment where the unshielded twisted pair is located; Based on the intensity values ​​of various types of nuclear radiation, a first dielectric loss coefficient of the unshielded twisted pair is calculated using a second formula; wherein the second formula is:

[0069] Among them, k 21 is the first dielectric loss coefficient of the unshielded twisted pair; y0 is the initial dielectric loss coefficient of the unshielded twisted pair in a non-nuclear radiation environment; I i is the intensity value of the i-th type of nuclear radiation; y i is a constant term of the intensity value of the i-th type of nuclear radiation, and the constant term is a preset value; n is the number of types of nuclear radiation in the environment where the unshielded twisted pair is located.

[0070] Optionally, the device also includes a fourth determination module, which is used to determine the constants in the first formula and the second formula through the following steps: in a non-nuclear radiation test environment, transmitting a second test pulse signal of different frequencies through the unshielded twisted pair, and performing a loss analysis on the second test pulse signal after transmission, and determining the initial conductor loss coefficient and the initial dielectric loss coefficient of the unshielded twisted pair according to the results of the loss analysis; in a nuclear radiation test environment, transmitting a second test pulse signal of different frequencies through the unshielded twisted pair, and performing a loss analysis on the second test pulse signal after transmission, and determining multiple groups of loss coefficients of the unshielded twisted pair according to the results of the loss analysis; wherein each group of loss coefficients includes a test conductor loss coefficient and a test dielectric loss coefficient; collecting the test intensity values ​​of various types of nuclear radiation in the nuclear radiation test environment, setting the constants in the first formula and the second formula as unknown quantities, and substituting the test intensity values ​​of various types of nuclear radiation, the multiple groups of loss coefficients, the initial conductor loss coefficient and the initial dielectric loss coefficient into the first formula and the second formula to solve the constants in the first formula and the second formula.

[0071] Optionally, the operation of fusing the first conductor loss coefficient and the second conductor loss coefficient to obtain a third conductor loss coefficient includes: fusing the first conductor loss coefficient and the second conductor loss coefficient using a third formula to obtain the third conductor loss coefficient; wherein the third formula is:

[0072] Wherein, k1 is the loss coefficient of the third conductor of the unshielded twisted pair; k 11 k is the first conductor loss factor of the unshielded twisted pair; 12 is the loss factor of the second conductor of the unshielded twisted pair; and is the weight coefficient, + =1; The first dielectric loss coefficient and the second dielectric loss coefficient are combined using a fourth formula to obtain a third dielectric loss coefficient; wherein the fourth formula is:

[0073] Wherein, k2 is the third dielectric loss coefficient of the unshielded twisted pair cable; k 21 k is the first dielectric loss coefficient of the unshielded twisted pair; 22 is the second dielectric loss coefficient of the unshielded twisted pair; and is the weight coefficient, + =1.

[0074] Optionally, the second determination module 320 is specifically used to: generate a first test pulse signal containing multiple different frequency components, and add the first test pulse signal to the target video signal to be transmitted; transmit the target video signal with the first test pulse signal added through the unshielded twisted pair; perform fast Fourier transform on the first test pulse signal before and after transmission to obtain amplitude information of the first test pulse signal on each frequency component before and after transmission; compare the amplitude changes of each frequency component in the first test pulse signal before and after transmission, and determine the cable attenuation coefficient when the unshielded twisted pair transmits the corresponding frequency component based on the amplitude changes; substitute the cable attenuation coefficient when the unshielded twisted pair transmits each frequency component and the frequency value of each frequency component into the following equation to solve the second conductor loss coefficient and the second dielectric loss coefficient:

[0075] Where, is the cable attenuation coefficient when the unshielded twisted pair transmits the i-th frequency component; is the frequency value of the i-th frequency component; k 12 k is the loss factor of the second conductor; 22 is the second dielectric loss coefficient.

[0076] Therefore, according to this embodiment, the intensity values ​​of various types of nuclear radiation in the environment of the unshielded twisted pair are first collected. Based on these radiation intensity values, the first conductor loss coefficient and the first dielectric loss coefficient of the unshielded twisted pair are dynamically calculated to precisely quantify the impact of environmental nuclear radiation on the transmission performance of the unshielded twisted pair. Next, a target video signal with a first test pulse signal added is transmitted through the unshielded twisted pair. Based on the loss of the first test pulse signal in the transmitted target video signal, the second conductor loss coefficient and the second dielectric loss coefficient of the unshielded twisted pair are determined to quantify the combined impact of signal frequency and all environmental factors on the transmission performance of the unshielded twisted pair. Next, the first loss coefficient (including the first conductor loss coefficient and the first dielectric loss coefficient), which precisely quantifies the impact of environmental nuclear radiation, is combined with the second loss coefficient (including the second conductor loss coefficient and the second dielectric loss coefficient), which comprehensively reflects the impact of environmental factors and signal frequency. This results in a composite loss coefficient (including the third conductor loss coefficient and the third dielectric loss coefficient) that can dynamically adapt to complex electromagnetic environments and is used for subsequent calculation of the cable attenuation coefficient. Secondly, based on the signal frequency of the target video signal, the third conductor loss coefficient, and the third dielectric loss coefficient, the cable attenuation coefficient of the unshielded twisted pair is calculated according to a preset composite attenuation model, which is used for subsequent calculation of the signal attenuation loss value. Finally, based on the cable attenuation coefficient, the amplitude attenuation factor of the unshielded twisted pair is calculated according to a preset cable transmission function. Based on this amplitude attenuation factor, the target video signal after transmission through the unshielded twisted pair is equalized and compensated to restore the original quality of the target video signal. This achieves the technical effects of dynamically adapting to complex nuclear radiation environments, dynamically and accurately compensating for signal attenuation, and significantly improving the quality and stability of unshielded twisted pair video signal transmission. This solves the technical problem that the existing equalization compensation scheme for unshielded twisted pair video signal transmission lacks a dynamic compensation mechanism for nuclear radiation interference.

[0077] Example 3 Figure 4 The image transmission and control device based on dynamic EQ compensation and nuclear radiation resistance according to this embodiment is shown, which corresponds to the method according to embodiment 1. Figure 4As shown, the device includes: a processor 410; and a memory 420, connected to the processor 410, for providing the processor 410 with instructions for processing the following processing steps: collecting intensity values ​​of various types of nuclear radiation in the environment where the unshielded twisted pair is located, and determining a first conductor loss coefficient and a first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of the various types of nuclear radiation; transmitting a target video signal with a first test pulse signal added through the unshielded twisted pair, and determining a second conductor loss coefficient and a second dielectric loss coefficient of the unshielded twisted pair according to the loss of the first test pulse signal in the transmitted target video signal; and The loss coefficient is merged with the second conductor loss coefficient to obtain a third conductor loss coefficient; the first dielectric loss coefficient is merged with the second dielectric loss coefficient to obtain a third dielectric loss coefficient; based on the signal frequency of the target video signal, the third conductor loss coefficient and the third dielectric loss coefficient, the cable attenuation coefficient of the unshielded twisted pair is determined according to a preset composite attenuation model; and based on the cable attenuation coefficient, the amplitude attenuation factor of the unshielded twisted pair is calculated according to a preset cable transmission function, and based on the amplitude attenuation factor, the target video signal after transmission through the unshielded twisted pair is balanced and compensated.

[0078] Optionally, the operation of determining the first conductor loss coefficient and the first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of various types of nuclear radiation includes: calculating the first conductor loss coefficient of the unshielded twisted pair based on the intensity values ​​of various types of nuclear radiation using a first formula; wherein the first formula is:

[0079] Among them, k 11 is the first conductor loss coefficient of the unshielded twisted pair; x0 is the initial conductor loss coefficient of the unshielded twisted pair in a non-nuclear radiation environment; I i is the intensity value of the i-th type of nuclear radiation; x i is a constant term of the intensity value of the i-th type of nuclear radiation, and the constant term is a preset value; n is the number of types of nuclear radiation in the environment where the unshielded twisted pair is located; Based on the intensity values ​​of various types of nuclear radiation, a first dielectric loss coefficient of the unshielded twisted pair is calculated using a second formula; wherein the second formula is:

[0080] Among them, k 21 is the first dielectric loss coefficient of the unshielded twisted pair; y0 is the initial dielectric loss coefficient of the unshielded twisted pair in a non-nuclear radiation environment; I i is the intensity value of the i-th type of nuclear radiation; y iis a constant term of the intensity value of the i-th type of nuclear radiation, and the constant term is a preset value; n is the number of types of nuclear radiation in the environment where the unshielded twisted pair is located.

[0081] Optionally, the constants in the first formula and the second formula are determined by the following steps: in a non-nuclear radiation test environment, transmitting a second test pulse signal of different frequencies through the unshielded twisted pair, and performing a loss analysis on the second test pulse signal after transmission, and determining the initial conductor loss coefficient and the initial dielectric loss coefficient of the unshielded twisted pair according to the results of the loss analysis; in a nuclear radiation test environment, transmitting a second test pulse signal of different frequencies through the unshielded twisted pair, and performing a loss analysis on the second test pulse signal after transmission, and determining multiple groups of loss coefficients of the unshielded twisted pair according to the results of the loss analysis; wherein each group of loss coefficients includes a test conductor loss coefficient and a test dielectric loss coefficient; collecting the test intensity values ​​of various types of nuclear radiation in the nuclear radiation test environment, setting the constants in the first formula and the second formula as unknown quantities, substituting the test intensity values ​​of various types of nuclear radiation, the multiple groups of loss coefficients, the initial conductor loss coefficient and the initial dielectric loss coefficient into the first formula and the second formula, and solving the constants in the first formula and the second formula.

[0082] Optionally, the operation of fusing the first conductor loss coefficient and the second conductor loss coefficient to obtain a third conductor loss coefficient includes: fusing the first conductor loss coefficient and the second conductor loss coefficient using a third formula to obtain the third conductor loss coefficient; wherein the third formula is:

[0083] Wherein, k1 is the loss coefficient of the third conductor of the unshielded twisted pair; k 11 k is the first conductor loss factor of the unshielded twisted pair; 12 is the loss factor of the second conductor of the unshielded twisted pair; and is the weight coefficient, + =1; The first dielectric loss coefficient and the second dielectric loss coefficient are combined using a fourth formula to obtain a third dielectric loss coefficient; wherein the fourth formula is:

[0084] Wherein, k2 is the third dielectric loss coefficient of the unshielded twisted pair cable; k 21 k is the first dielectric loss coefficient of the unshielded twisted pair; 22 is the second dielectric loss coefficient of the unshielded twisted pair; and is the weight coefficient, + =1.

[0085] Optionally, the target video signal with the first test pulse signal added thereto is transmitted through the unshielded twisted pair, and the second conductor loss coefficient and the second dielectric loss coefficient of the unshielded twisted pair are determined based on the loss of the first test pulse signal in the target video signal after transmission, including: generating a first test pulse signal containing multiple different frequency components, and adding the first test pulse signal to the target video signal to be transmitted; transmitting the target video signal with the first test pulse signal added thereto through the unshielded twisted pair; performing a fast Fourier transform on the first test pulse signal before and after transmission to obtain amplitude information of the first test pulse signal on each frequency component before and after transmission; comparing the amplitude changes of each frequency component in the first test pulse signal before and after transmission, and determining the cable attenuation coefficient when the unshielded twisted pair transmits the corresponding frequency component based on the amplitude changes; substituting the cable attenuation coefficient when the unshielded twisted pair transmits each frequency component and the frequency value of each frequency component into the following equation to solve the second conductor loss coefficient and the second dielectric loss coefficient:

[0086] Where, is the cable attenuation coefficient when the unshielded twisted pair transmits the i-th frequency component; is the frequency value of the i-th frequency component; k 12 k is the loss factor of the second conductor; 22 is the second dielectric loss coefficient.

[0087] Therefore, according to this embodiment, the intensity values ​​of various types of nuclear radiation in the environment of the unshielded twisted pair are first collected. Based on these radiation intensity values, the first conductor loss coefficient and the first dielectric loss coefficient of the unshielded twisted pair are dynamically calculated to precisely quantify the impact of environmental nuclear radiation on the transmission performance of the unshielded twisted pair. Next, a target video signal with a first test pulse signal added is transmitted through the unshielded twisted pair. Based on the loss of the first test pulse signal in the transmitted target video signal, the second conductor loss coefficient and the second dielectric loss coefficient of the unshielded twisted pair are determined to quantify the combined impact of signal frequency and all environmental factors on the transmission performance of the unshielded twisted pair. Next, the first loss coefficient (including the first conductor loss coefficient and the first dielectric loss coefficient), which precisely quantifies the impact of environmental nuclear radiation, is combined with the second loss coefficient (including the second conductor loss coefficient and the second dielectric loss coefficient), which comprehensively reflects the impact of environmental factors and signal frequency. This results in a composite loss coefficient (including the third conductor loss coefficient and the third dielectric loss coefficient) that can dynamically adapt to complex electromagnetic environments and is used for subsequent calculation of the cable attenuation coefficient. Secondly, based on the signal frequency of the target video signal, the third conductor loss coefficient, and the third dielectric loss coefficient, the cable attenuation coefficient of the unshielded twisted pair is calculated according to a preset composite attenuation model, which is used for subsequent calculation of the signal attenuation loss value. Finally, based on the cable attenuation coefficient, the amplitude attenuation factor of the unshielded twisted pair is calculated according to a preset cable transmission function. Based on this amplitude attenuation factor, the target video signal after transmission through the unshielded twisted pair is equalized and compensated to restore the original quality of the target video signal. This achieves the technical effects of dynamically adapting to complex nuclear radiation environments, dynamically and accurately compensating for signal attenuation, and significantly improving the quality and stability of unshielded twisted pair video signal transmission. This solves the technical problem that the existing equalization compensation scheme for unshielded twisted pair video signal transmission lacks a dynamic compensation mechanism for nuclear radiation interference.

[0088] The serial numbers of the above embodiments of the present invention are for description only and do not represent the advantages or disadvantages of the embodiments.

[0089] In the above embodiments of the present invention, the description of each embodiment has its own focus. For parts that are not described in detail in a certain embodiment, reference can be made to the relevant descriptions of other embodiments.

[0090] In the several embodiments provided in this application, it should be understood that the disclosed technical content can be implemented in other ways. Among them, the device embodiments described above are only schematic. For example, the division of the units is only a logical function division. In actual implementation, there may be other division methods, such as multiple units or components can be combined or integrated into another system, or some features can be ignored or not executed. Another point is that the mutual coupling or direct coupling or communication connection shown or discussed can be through some interfaces, indirect coupling or communication connection of units or modules, which can be electrical or other forms.

[0091] The units described as separate components may or may not be physically separate, and the components shown as units may or may not be physical units, that is, they may be located in one place or distributed across multiple network units. Some or all of these units may be selected to achieve the purpose of this embodiment according to actual needs.

[0092] In addition, the functional units in the various embodiments of the present invention may be integrated into a single processing unit, each unit may exist physically separately, or two or more units may be integrated into a single unit. The aforementioned integrated units may be implemented in the form of hardware or software functional units.

[0093] If the integrated unit is implemented as a software functional unit and sold or used as an independent product, it can be stored in a computer-readable storage medium. Based on this understanding, the technical solution of the present invention, or the portion that contributes to the prior art, or all or part of the technical solution, can be embodied in the form of a software product. This computer software product is stored in a storage medium and includes several instructions for causing a computer device (which can be a personal computer, server, or network device, etc.) to execute all or part of the steps of the method described in each embodiment of the present invention. The aforementioned storage medium includes various media that can store program code, such as a USB flash drive, read-only memory (ROM), random access memory (RAM), a mobile hard drive, a magnetic disk, or an optical disk.

[0094] The above is only a preferred embodiment of the present invention. It should be pointed out that for ordinary technicians in this technical field, several improvements and modifications can be made without departing from the principles of the present invention. These improvements and modifications should also be regarded as within the scope of protection of the present invention.

Claims

1. A method for image transmission and control based on dynamic EQ compensation and nuclear radiation resistance, characterized in that: include: Collecting intensity values ​​of various types of nuclear radiation in an environment where the unshielded twisted pair is located, and determining a first conductor loss coefficient and a first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of the various types of nuclear radiation; Transmitting a target video signal to which a first test pulse signal is added through the unshielded twisted pair cable, and determining a second conductor loss coefficient and a second dielectric loss coefficient of the unshielded twisted pair cable based on a loss condition of the first test pulse signal in the transmitted target video signal; The first conductor loss coefficient and the second conductor loss coefficient are combined to obtain a third conductor loss coefficient; the first dielectric loss coefficient and the second dielectric loss coefficient are combined to obtain a third dielectric loss coefficient; Determining the cable attenuation coefficient of the unshielded twisted pair according to a preset composite attenuation model based on the signal frequency of the target video signal, the third conductor loss coefficient, and the third dielectric loss coefficient; as well as Based on the cable attenuation coefficient, an amplitude attenuation factor of the unshielded twisted pair is calculated according to a preset cable transmission function, and based on the amplitude attenuation factor, equalization compensation is performed on the target video signal after transmission through the unshielded twisted pair.

2. The method according to claim 1, characterized in that The operation of determining the first conductor loss coefficient and the first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of various types of nuclear radiation includes: Based on the intensity values ​​of various types of nuclear radiation, the first conductor loss coefficient of the unshielded twisted pair is calculated using a first formula; wherein the first formula is: ， Among them, k 11 is the first conductor loss coefficient of the unshielded twisted pair; x0 is the initial conductor loss coefficient of the unshielded twisted pair in a non-nuclear radiation environment; I i is the intensity value of the i-th type of nuclear radiation; x i is a constant term of the intensity value of the i-th type of nuclear radiation, and the constant term is a preset value; n is the number of types of nuclear radiation in the environment where the unshielded twisted pair is located; Based on the intensity values ​​of various types of nuclear radiation, a first dielectric loss coefficient of the unshielded twisted pair is calculated using a second formula; wherein the second formula is: ， Among them, k 21 is the first dielectric loss coefficient of the unshielded twisted pair; y0 is the initial dielectric loss coefficient of the unshielded twisted pair in a non-nuclear radiation environment; I i is the intensity value of the i-th type of nuclear radiation; y i is a constant term of the intensity value of the i-th type of nuclear radiation, and the constant term is a preset value; n is the number of types of nuclear radiation in the environment where the unshielded twisted pair is located.

3. The method according to claim 2, characterized in that The constants in the first formula and the second formula are determined by the following steps: In a non-nuclear radiation test environment, transmitting a second test pulse signal of a different frequency through the unshielded twisted pair cable, performing a loss analysis on the transmitted second test pulse signal, and determining an initial conductor loss coefficient and an initial dielectric loss coefficient of the unshielded twisted pair cable based on the results of the loss analysis; In a nuclear radiation test environment, transmitting second test pulse signals of different frequencies through the unshielded twisted pair cable, performing loss analysis on the transmitted second test pulse signals, and determining multiple groups of loss coefficients of the unshielded twisted pair cable based on the results of the loss analysis; wherein each group of loss coefficients includes a test conductor loss coefficient and a test dielectric loss coefficient; Collect the test intensity values ​​of various types of nuclear radiation in the nuclear radiation test environment, set the constants in the first formula and the second formula as unknown quantities, substitute the test intensity values ​​of various types of nuclear radiation, the multiple groups of loss coefficients, the initial conductor loss coefficient and the initial dielectric loss coefficient into the first formula and the second formula, and solve the constants in the first formula and the second formula.

4. The method according to claim 3, characterized in that The operation of fusing the first conductor loss coefficient and the second conductor loss coefficient to obtain a third conductor loss coefficient includes: The first conductor loss coefficient and the second conductor loss coefficient are combined using a third formula to obtain a third conductor loss coefficient; wherein the third formula is: ， Wherein, k1 is the loss coefficient of the third conductor of the unshielded twisted pair; k 11 k is the first conductor loss factor of the unshielded twisted pair; 12 is the loss factor of the second conductor of the unshielded twisted pair; and is the weight coefficient, + =1; The first dielectric loss coefficient and the second dielectric loss coefficient are combined using a fourth formula to obtain a third dielectric loss coefficient; wherein the fourth formula is: ， Wherein, k2 is the third dielectric loss coefficient of the unshielded twisted pair cable; k 21 k is the first dielectric loss coefficient of the unshielded twisted pair; 22 is the second dielectric loss coefficient of the unshielded twisted pair; and is the weight coefficient, + =1.

5. The method according to claim 1, characterized in that The operation of transmitting the target video signal to which the first test pulse signal is added through the unshielded twisted pair cable and determining the second conductor loss coefficient and the second dielectric loss coefficient of the unshielded twisted pair cable according to the loss of the first test pulse signal in the transmitted target video signal includes: generating a first test pulse signal including a plurality of different frequency components, and adding the first test pulse signal to a target video signal to be transmitted; transmitting the target video signal added with the first test pulse signal through the unshielded twisted pair cable; Performing a fast Fourier transform on the first test pulse signal before and after transmission to obtain amplitude information of the first test pulse signal at each frequency component before and after transmission; Comparing the amplitude changes of the various frequency components in the first test pulse signal before and after transmission, and determining the cable attenuation coefficient when the unshielded twisted pair transmits the corresponding frequency component based on the amplitude changes; Substitute the cable attenuation coefficient when the unshielded twisted pair transmits each frequency component and the frequency value of each frequency component into the following equation to solve the second conductor loss coefficient and the second dielectric loss coefficient: ， Where, is the cable attenuation coefficient when the unshielded twisted pair transmits the i-th frequency component; is the frequency value of the i-th frequency component; k 12 k is the loss factor of the second conductor; 22 is the second dielectric loss coefficient.

6. A storage medium, characterized in that The storage medium includes a stored program, wherein when the program is run, the processor executes the method according to any one of claims 1 to 5.

7. An image transmission and control device based on dynamic EQ compensation and nuclear radiation resistance, characterized in that: include: a first determination module, configured to collect intensity values ​​of various types of nuclear radiation in an environment where an unshielded twisted pair is located, and determine a first conductor loss coefficient and a first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of the various types of nuclear radiation; a second determining module, configured to transmit the target video signal to which the first test pulse signal is added through the unshielded twisted pair cable, and determine a second conductor loss coefficient and a second dielectric loss coefficient of the unshielded twisted pair cable based on a loss condition of the first test pulse signal in the transmitted target video signal; a fusion module, configured to fuse the first conductor loss coefficient with the second conductor loss coefficient to obtain a third conductor loss coefficient; and fuse the first dielectric loss coefficient with the second dielectric loss coefficient to obtain a third dielectric loss coefficient; a third determining module, configured to determine the cable attenuation coefficient of the unshielded twisted pair cable according to a preset composite attenuation model based on the signal frequency of the target video signal, the third conductor loss coefficient, and the third dielectric loss coefficient; as well as The equalization compensation module is used to calculate the amplitude attenuation factor of the unshielded twisted pair based on the cable attenuation coefficient and a preset cable transmission function, and perform equalization compensation on the target video signal after transmission through the unshielded twisted pair based on the amplitude attenuation factor.

8. The device according to claim 7, characterized in that The first determining module is specifically configured to: Based on the intensity values ​​of various types of nuclear radiation, the first conductor loss coefficient of the unshielded twisted pair is calculated using a first formula; wherein the first formula is: ， Among them, k 11 is the first conductor loss coefficient of the unshielded twisted pair; x0 is the initial conductor loss coefficient of the unshielded twisted pair in a non-nuclear radiation environment; I i is the intensity value of the i-th type of nuclear radiation; x i is a constant term of the intensity value of the i-th type of nuclear radiation, and the constant term is a preset value; n is the number of types of nuclear radiation in the environment where the unshielded twisted pair is located; Based on the intensity values ​​of various types of nuclear radiation, a first dielectric loss coefficient of the unshielded twisted pair is calculated using a second formula; wherein the second formula is: ， Among them, k 21 is the first dielectric loss coefficient of the unshielded twisted pair; y0 is the initial dielectric loss coefficient of the unshielded twisted pair in a non-nuclear radiation environment; I i is the intensity value of the i-th type of nuclear radiation; x i is a constant term of the intensity value of the i-th type of nuclear radiation, and the constant term is a preset value; n is the number of types of nuclear radiation in the environment where the unshielded twisted pair is located.

9. The device according to claim 8, characterized in that The system further includes a fourth determining module, configured to determine various constants in the first formula and the second formula by the following steps: In a non-nuclear radiation test environment, transmitting a second test pulse signal of a different frequency through the unshielded twisted pair cable, performing a loss analysis on the transmitted second test pulse signal, and determining an initial conductor loss coefficient and an initial dielectric loss coefficient of the unshielded twisted pair cable based on the results of the loss analysis; In a nuclear radiation test environment, transmitting second test pulse signals of different frequencies through the unshielded twisted pair cable, performing loss analysis on the transmitted second test pulse signals, and determining multiple groups of loss coefficients of the unshielded twisted pair cable based on the results of the loss analysis; wherein each group of loss coefficients includes a test conductor loss coefficient and a test dielectric loss coefficient; Collect the test intensity values ​​of various types of nuclear radiation in the nuclear radiation test environment, set the constants in the first formula and the second formula as unknown quantities, substitute the test intensity values ​​of various types of nuclear radiation, the multiple groups of loss coefficients, the initial conductor loss coefficient and the initial dielectric loss coefficient into the first formula and the second formula, and solve the constants in the first formula and the second formula.

10. An image transmission and control device based on dynamic EQ compensation and nuclear radiation resistance, characterized in that: include: processor; as well as A memory, connected to the processor, configured to provide the processor with instructions for processing the following steps: Collecting intensity values ​​of various types of nuclear radiation in an environment where the unshielded twisted pair is located, and determining a first conductor loss coefficient and a first dielectric loss coefficient of the unshielded twisted pair based on the intensity values ​​of the various types of nuclear radiation; Transmitting a target video signal to which a first test pulse signal is added through the unshielded twisted pair cable, and determining a second conductor loss coefficient and a second dielectric loss coefficient of the unshielded twisted pair cable based on a loss condition of the first test pulse signal in the transmitted target video signal; The first conductor loss coefficient and the second conductor loss coefficient are combined to obtain a third conductor loss coefficient; the first dielectric loss coefficient and the second dielectric loss coefficient are combined to obtain a third dielectric loss coefficient; Determining the cable attenuation coefficient of the unshielded twisted pair according to a preset composite attenuation model based on the signal frequency of the target video signal, the third conductor loss coefficient, and the third dielectric loss coefficient; as well as Based on the cable attenuation coefficient, an amplitude attenuation factor of the unshielded twisted pair is calculated according to a preset cable transmission function, and based on the amplitude attenuation factor, equalization compensation is performed on the target video signal after transmission through the unshielded twisted pair.

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