CN113950176A - Magnetron anode power supply ripple mixing multi-frequency heating device and method - Google Patents
Magnetron anode power supply ripple mixing multi-frequency heating device and method Download PDFInfo
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Abstract
本发明公开了磁控管阳极电源纹波混频多频加热装置和方法,属于微波加热领域,磁控管电源连有第一阴极电源线和第二阴极电源线;第一阴极电源线和第二阴极电源线分别与磁控管的阴极两端连接;第一电容一端和中频信号发生器连接,另一端和第一阴极电源线连接;腔体上设有馈口;磁控管通过馈口向腔体内输入多个频率的微波。本发明的磁控管阳极电源纹波混频多频加热装置和方法,基于磁控管的非线性响应特性,中频信号等效为磁控管阳极电压的纹波加载到磁控管阳极电压上,并将磁控管本身激励起的谐振信号作为本地振荡信号,利用磁控管进行混频使磁控管的输出端产生多个频率的微波,对物料进行均匀加热。
The invention discloses a magnetron anode power supply ripple mixing multi-frequency heating device and method, belonging to the field of microwave heating. The magnetron power supply is connected with a first cathode power supply line and a second cathode power supply line; The two cathode power lines are respectively connected with the two ends of the cathode of the magnetron; one end of the first capacitor is connected with the intermediate frequency signal generator, and the other end is connected with the first cathode power line; the cavity is provided with a feed port; the magnetron passes through the feed port Microwaves of multiple frequencies are input into the cavity. The device and method for multi-frequency heating of the magnetron anode power ripple mixing frequency are based on the nonlinear response characteristics of the magnetron, and the intermediate frequency signal is equivalent to the ripple of the magnetron anode voltage and is loaded on the magnetron anode voltage. , and the resonance signal excited by the magnetron itself is used as the local oscillation signal, and the output end of the magnetron generates microwaves of multiple frequencies by mixing the magnetron to heat the material uniformly.
Description
技术领域technical field
本发明属于微波加热领域,具体地说涉及磁控管阳极电源纹波混频多频加热装置和方法。The invention belongs to the field of microwave heating, and in particular relates to a device and a method for heating a magnetron anode power supply ripple frequency mixing multi-frequency.
背景技术Background technique
微波作为一种新型的清洁能源广泛地应用于食品、化工、冶金和污水处理等众多领域。微波直接作用于被加热物料内部的极性分子和带电粒子,因此微波加热具有选择性加热、体加热和清洁加热等优势。然而微波在实际加热过程中普遍存在加热不均匀的问题,不均匀加热造成局部温度过高而形成“热点”,很多物质对电磁波的吸收能力与温度成正相关,“热点”区域的温度上升得更快,最终形成“热失控”现象,这很大程度制约了微波能的大规模应用。As a new type of clean energy, microwave is widely used in many fields such as food, chemical industry, metallurgy and sewage treatment. Microwave directly acts on the polar molecules and charged particles inside the heated material, so microwave heating has the advantages of selective heating, bulk heating and cleaning heating. However, in the actual heating process of microwaves, there is generally a problem of uneven heating. The uneven heating causes the local temperature to be too high to form a "hot spot". The absorption capacity of many substances to electromagnetic waves is positively correlated with the temperature, and the temperature of the "hot spot" area rises more. The phenomenon of "thermal runaway" is finally formed, which greatly restricts the large-scale application of microwave energy.
随着科技的发展和人们生活水平的提高,微波炉越来越受到消费者的重视,并慢慢成为厨房必备家用电器。由于微波加热具备加热速度快、耗能低同时还方便随时控制等优点,所以微波炉逐渐得到广泛应用。但是随着技术的不断发展,消费者对微波炉的要求也逐渐提高,尤其在对食物的加热均匀性、加热效率等方面。传统微波炉工作频率为2450MHz,仅采用单一微波源、单一频率进行加热,虽然微波炉腔体是多模谐振腔,能在腔体内激励起多个电磁模式,但激励起的模式个数毕竟有限,仍存在加热不均匀的现象。With the development of science and technology and the improvement of people's living standards, microwave ovens are increasingly valued by consumers, and have gradually become an essential household appliance in the kitchen. Because microwave heating has the advantages of fast heating speed, low energy consumption and convenient control at any time, microwave ovens have gradually been widely used. However, with the continuous development of technology, consumers' requirements for microwave ovens have gradually increased, especially in terms of heating uniformity and heating efficiency of food. The operating frequency of traditional microwave ovens is 2450MHz, and only a single microwave source and a single frequency are used for heating. Although the microwave oven cavity is a multi-mode resonant cavity, multiple electromagnetic modes can be excited in the cavity, but the number of excited modes is limited after all. There is a phenomenon of uneven heating.
在微波炉加热均匀性提升方面,学者们做了大量工作。在1989年,季天仁提出了旋转天线理念,即天线随着驱动器旋转的同时使腔体内模式场发生改变,导致场分布改变,提高加热均匀性。1995年,闫丽萍等所做工作主要是探索微波炉腔体内转盘转动对加热均匀性的影响和负载大小及面积与微波炉输出功率的关系。2001年,Sung Yi,Lie Liu用FEM,即有限元方法对规则的矩形波导和谐振腔进行了仿真分析,得出了腔体中激励的谐振频率越多,场分布就越均匀。2006年,Shinya Watanabe等人利用THE方法计算热传导与FDTD法计算电磁场,对被加热物体表面的温度分布进行了研究。2017年,Sang-Hyeon Bae和Min-GyoJeong研究了由多个2.45GHz微波源做成的可持续功率控制的微波输送带式干燥器,通过顺序控制微波源的输入功率,可以改善腔体加热均匀性。中频信号指频段由300KHz到3000KHz的频率信号,而在射频通信系统里面,调制之前的信号被称为基带信号,混频之后的被称为射频(或者高频)信号,这两级之间的就是中频信号。Scholars have done a lot of work on the improvement of microwave heating uniformity. In 1989, Ji Tianren proposed the concept of rotating antenna, that is, the mode field in the cavity changes while the antenna rotates with the driver, which leads to the change of the field distribution and improves the heating uniformity. In 1995, Yan Liping et al. mainly explored the influence of the rotation of the turntable in the microwave oven cavity on the heating uniformity and the relationship between the load size and area and the output power of the microwave oven. In 2001, Sung Yi and Lie Liu used FEM, that is, finite element method, to simulate and analyze regular rectangular waveguides and resonant cavities, and concluded that the more resonant frequencies excited in the cavity, the more uniform the field distribution. In 2006, Shinya Watanabe et al. used the THE method to calculate the heat conduction and the FDTD method to calculate the electromagnetic field, and studied the temperature distribution on the surface of the heated object. In 2017, Sang-Hyeon Bae and Min-GyoJeong studied a sustainable power-controlled microwave conveyor belt dryer made of multiple 2.45GHz microwave sources. By sequentially controlling the input power of the microwave sources, the uniform heating of the cavity can be improved. sex. The intermediate frequency signal refers to the frequency signal with the frequency band from 300KHz to 3000KHz, and in the radio frequency communication system, the signal before modulation is called the baseband signal, and the signal after mixing is called the radio frequency (or high frequency) signal. It's the IF signal.
本领域目前还没有研究过如何使单个微波源能够输出多个频率微波,对物料进行均匀加热,以改善微波加热物料不均的问题。即便是有考虑过采用多个频率的微波对物料进行加热,一般也会增加微波源的数量,这必然导致成本的增加。或者即便是单个微波源能够输出多个频率微波,也必须采用单独设置的混频器及大量辅助配件,同样导致成本的增加。本发明低成本实现单个微波源输出多个频率微波,而且输出的微波频率可控可调,保证微波加热均匀性。So far, no research has been done on how to enable a single microwave source to output microwaves of multiple frequencies to uniformly heat materials, so as to improve the problem of uneven heating of materials by microwaves. Even if it is considered to use microwaves of multiple frequencies to heat the material, the number of microwave sources will generally increase, which will inevitably lead to an increase in cost. Or even if a single microwave source can output microwaves of multiple frequencies, a separate mixer and a large number of auxiliary accessories must be used, which also leads to an increase in cost. The invention realizes that a single microwave source outputs microwaves of multiple frequencies at low cost, and the frequency of the output microwaves is controllable and adjustable, so as to ensure the uniformity of microwave heating.
发明内容SUMMARY OF THE INVENTION
本发明的目的是针对上述不足之处提供磁控管阳极电源纹波混频多频加热装置和方法,拟解决现有技术中微波加热仍存在不均匀等问题。为实现上述目的,本发明提供如下技术方案:The purpose of the present invention is to provide a magnetron anode power supply ripple mixing multi-frequency heating device and method in view of the above shortcomings, and it is intended to solve the problems of uneven microwave heating in the prior art. To achieve the above object, the present invention provides the following technical solutions:
磁控管阳极电源纹波混频多频加热装置,包括磁控管电源1、磁控管2、中频信号发生器3、第一电容41和腔体8;所述磁控管电源1连有第一阴极电源线71和第二阴极电源线72;所述第一阴极电源线71和第二阴极电源线72分别与磁控管2的阴极两端连接;所述第一电容41一端和中频信号发生器3连接,另一端和第一阴极电源线71连接;所述腔体8上设有馈口;所述磁控管2通过馈口向腔体8内输入多个频率的微波。The magnetron anode power supply ripple mixing multi-frequency heating device includes a
进一步的,所述第一电容41与第一阴极电源线71连接交点和磁控管电源1之间的第一阴极电源线71上设有第一电感51。Further, a
进一步的,所述第二阴极电源线72上设有第二电感52。Further, the second
进一步的,还包括第三电感53;所述第三电感53一端与中频信号发生器3以及第一电容41连接中频信号发生器3的一端均连接,另一端接地。Further, it also includes a
进一步的,还包括第四电容44;所述第四电容44一端与磁控管电源1和第一电感51之间的第一阴极电源线71连接,另一端接地。Further, a
进一步的,还包括第五电容45;所述第五电容45一端与磁控管电源1和第二电感52之间的第二阴极电源线72连接,另一端接地。Further, a
进一步的,还包括第一电阻61、第二电阻62和第三电阻63;所述第一电阻61和第三电感53两端并联;所述第二电阻62和第一电感51两端并联;所述第三电阻63和第二电感52两端并联。Further, it also includes a
进一步的,还包括阻抗匹配调节器;所述阻抗匹配调节器包括第二可调电容42和第三可调电容43;所述第二可调电容42一端与中频信号发生器3以及第一电容41连接中频信号发生器3的一端均连接,另一端接地;所述第三可调电容43一端与中频信号发生器3以及第一电容41连接中频信号发生器3的一端均连接,另一端接地。Further, it also includes an impedance matching regulator; the impedance matching regulator includes a second
进一步的,还包括电路板;所述第一电容41、第一电感51、第二电感52、第三电感53、第四电容44、第五电容45、第一电阻61、第二电阻62和第三电阻63集成在电路板上;所述电路板包括第一端口、第二端口、第三端口、第四端口和第五端口;所述第一端口位于第一电感51和磁控管电源1之间的第一阴极电源线71上;所述第二端口位于第二电感52和磁控管电源1之间的第二阴极电源线72上;所述第三端口位于第一电感51和磁控管2之间的第一阴极电源线71上;所述第四端口位于第二电感52和磁控管2之间的第二阴极电源线72上;所述第五端口位于中频信号发生器3和第一电容41之间,使中频信号发生器3和第一电容41连通。Further, it also includes a circuit board; the
磁控管阳极电源纹波混频多频加热方法,采用上述任一磁控管阳极电源纹波混频多频加热装置;具体步骤为:所述磁控管电源1为磁控管2供电;所述中频信号发生器3产生中频信号,中频信号通过第一电容41输入到第一阴极电源线71上,此时中频信号等效为磁控管2阳极电压的纹波加载到磁控管2阳极电压上,并将磁控管2本身激励起的谐振信号作为本地振荡信号,当中频信号作为阳极电压纹波与磁控管2的谐振信号发生作用时,磁控管2非线性响应的特性使磁控管2的输出端产生多个频率的微波,多个频率的微波通过馈口输入腔体8内,对物料9进行加热。A magnetron anode power supply ripple-mixing multi-frequency heating method adopts any one of the above-mentioned magnetron anode power supply ripple-mixing multi-frequency heating devices; the specific steps are: the
本发明的有益效果是:The beneficial effects of the present invention are:
本发明公开了磁控管阳极电源纹波混频多频加热装置和方法,磁控管电源连有第一阴极电源线和第二阴极电源线;第一阴极电源线和第二阴极电源线分别与磁控管的阴极两端连接;第一电容一端和中频信号发生器连接,另一端和第一阴极电源线连接;腔体上设有馈口;磁控管通过馈口向腔体内输入多个频率的微波。本发明的磁控管阳极电源纹波混频多频加热装置和方法,基于磁控管的非线性响应特性,中频信号等效为磁控管阳极电压的纹波加载到磁控管阳极电压上,并将磁控管本身激励起的谐振信号作为本地振荡信号,利用磁控管进行混频使磁控管的输出端产生多个频率的微波,对物料进行均匀加热。The invention discloses a magnetron anode power supply ripple mixing multi-frequency heating device and method. The magnetron power supply is connected with a first cathode power supply line and a second cathode power supply line; the first cathode power supply line and the second cathode power supply line are respectively It is connected with both ends of the cathode of the magnetron; one end of the first capacitor is connected with the intermediate frequency signal generator, and the other end is connected with the power line of the first cathode; the cavity is provided with a feeding port; microwave frequency. The device and method for multi-frequency heating of the magnetron anode power supply ripple mixing frequency of the present invention are based on the nonlinear response characteristics of the magnetron, and the intermediate frequency signal is equivalent to the ripple of the magnetron anode voltage and is loaded on the magnetron anode voltage. , and the resonance signal excited by the magnetron itself is used as the local oscillation signal, and the output end of the magnetron generates microwaves of multiple frequencies by mixing the magnetron to heat the material uniformly.
附图说明Description of drawings
图1是本发明磁控管阳极电源纹波混频多频加热装置电路原理示意图,未显示腔体;1 is a schematic diagram of the circuit principle of a magnetron anode power supply ripple mixing multi-frequency heating device of the present invention, and the cavity is not shown;
图2是磁控管的等效电路图;根据对磁控管谐振腔结构和作用的研究,磁控管的谐振腔可以等效为RLC并联谐振电路,g+jb为等效的磁控管源部分,G+jB为等效负载,R、L、C分别为等效电阻、等效电感和等效电容;Figure 2 is the equivalent circuit diagram of the magnetron; according to the research on the structure and function of the resonant cavity of the magnetron, the resonant cavity of the magnetron can be equivalent to an RLC parallel resonant circuit, and g+jb is the equivalent magnetron source part, G+jB is equivalent load, R, L, C are equivalent resistance, equivalent inductance and equivalent capacitance respectively;
图3是磁控管输出信号时域图像;对推导得到的阳极电压含有中频信号的自由振荡磁控管稳定状态下输出信号的表达式进行作图,边带包络的深度表示了加载的中频信号的幅度,边带包络的频率则与中频信号的频率有关;Figure 3 is the time-domain image of the output signal of the magnetron; the derived expression of the output signal of the free-oscillating magnetron in the steady state with the anode voltage containing the intermediate frequency signal is plotted, and the depth of the sideband envelope represents the loaded intermediate frequency The amplitude of the signal, and the frequency of the sideband envelope is related to the frequency of the IF signal;
图4是磁控管输出信号频域图像;对推导得到的表达式进行快速傅里叶变换作出的图,图像中最高强度的频率点代表了自由振荡磁控管的中心频率,中心频率两边的强度稍弱的次频率点代表了磁控管本振频率与中频信号频率混频之后得到的新频点,中心频率与次频率分量之间的频率差即中频信号的频率;Figure 4 is the frequency domain image of the output signal of the magnetron; the figure obtained by fast Fourier transform of the derived expression, the frequency point with the highest intensity in the image represents the center frequency of the free oscillating magnetron, and the frequency points on both sides of the center frequency The sub-frequency point with slightly weaker intensity represents the new frequency point obtained after the magnetron local oscillator frequency and the intermediate frequency signal frequency are mixed, and the frequency difference between the center frequency and the sub-frequency component is the frequency of the intermediate frequency signal;
图5是加载了中频信号的磁控管阳极电压波形图;原本理想阳极电压为直流电压,加载的中频信号即体现为该直流电压上的纹波分量,此处将携带信息的复杂的中频信号简化为单一频率的正弦信号;Figure 5 is a waveform diagram of the anode voltage of the magnetron loaded with an intermediate frequency signal; the ideal anode voltage is a DC voltage originally, and the loaded intermediate frequency signal is reflected as the ripple component on the DC voltage. Here, the complex intermediate frequency signal carrying information will be Simplified to a single frequency sinusoidal signal;
图6是自由振荡状态下磁控管输出信号时域图像,通过电磁仿真软件对磁控管进行建模,仿真计算得到了自由振荡稳定状态下磁控管时域输出图像,边带包络特征与图3推导得到的图像类似;Figure 6 is the time-domain image of the output signal of the magnetron in the free oscillation state. The magnetron is modeled by electromagnetic simulation software. The simulation calculation obtains the time-domain output image of the magnetron in the free oscillation stable state, and the sideband envelope characteristics Similar to the image derived from Figure 3;
图7是自由振荡状态下磁控管输出信号频域图像,通过仿真计算得到的磁控管输出频谱图,图像上的中心频率与次频率分量之间的关系特征与图4推导得到的图像类似;Figure 7 is the frequency domain image of the output signal of the magnetron in the free oscillation state. The output spectrum of the magnetron is obtained by simulation calculation. The relationship between the center frequency and the sub-frequency component on the image is similar to the image derived from Figure 4. ;
图8是未加载中频信号时磁控管输出信号频域图像,该频谱为松下生产的2M244-M1型磁控管在自由振荡状态下输出频谱;Figure 8 is the frequency domain image of the output signal of the magnetron when the intermediate frequency signal is not loaded, the spectrum is the output spectrum of the 2M244-M1 magnetron produced by Panasonic in the free oscillation state;
图9是加载2MHz中频信号时磁控管输出信号频域图像,图像上的中心频率与次频率分量之间的关系特征与图4推导得到的图像类似;Fig. 9 is the frequency domain image of the magnetron output signal when the 2MHz intermediate frequency signal is loaded, and the relationship between the center frequency and the sub-frequency component on the image is similar to the image derived from Fig. 4;
图10是加载3MHz中频信号时磁控管输出信号频域图像,图像上的中心频率与次频率分量之间的关系特征与图4推导得到的图像类似;Figure 10 is the frequency domain image of the magnetron output signal when the 3MHz intermediate frequency signal is loaded, and the relationship between the center frequency and the sub-frequency component on the image is similar to the image derived from Figure 4;
图11是加载4MHz中频信号时磁控管输出信号频域图像,图像上的中心频率与次频率分量之间的关系特征与图4推导得到的图像类似;Figure 11 is the frequency domain image of the magnetron output signal when the 4MHz intermediate frequency signal is loaded, and the relationship between the center frequency and the sub-frequency component on the image is similar to the image derived from Figure 4;
图12是对实部表达式求解可得磁控管自由振荡状态下的高频输出电压为VRF(t)的公式;Fig. 12 is the formula that the high-frequency output voltage under the free oscillation state of the magnetron can be obtained by solving the real part expression as VRF(t);
图13是对虚部表达式求解可得磁控管自由振荡状态瞬态输出频率ω(t)的公式;Fig. 13 is the formula of the transient output frequency ω(t) of the free oscillation state of the magnetron that can be obtained by solving the imaginary part expression;
图14是物料位于腔体内的示意图;Figure 14 is a schematic diagram of the material being located in the cavity;
图15是腔体设计为405×295×340mm的矩形腔体,土豆处于腔体中心点正下方50mm,初始温度293.15K,加热时间20s的加热仿真图,单频输入2.45GHz的微波,功率600W,可看出平均温度ave=313.68K,cov=0.5352;Figure 15 is a heating simulation diagram of the cavity designed as a rectangular cavity of 405×295×340mm, the potato is 50mm directly below the center point of the cavity, the initial temperature is 293.15K, and the heating time is 20s. The single-frequency input microwave is 2.45GHz and the power is 600W. , it can be seen that the average temperature ave=313.68K, cov=0.5352;
图16是腔体设计为405×295×340mm的矩形腔体,土豆处于腔体中心点正下方50mm,初始温度293.15K,加热时间20s的加热仿真图,输入三频频差4MHz(2.45GHz、2.446GHz、2.454GHz)的微波,功率200W,可看出平均温度ave=310.63K,cov=0.3738;Figure 16 is a heating simulation diagram of a rectangular cavity with a cavity design of 405×295×340mm, the potato is 50mm directly below the center point of the cavity, the initial temperature is 293.15K, and the heating time is 20s. GHz, 2.454GHz) microwave, power 200W, it can be seen that the average temperature ave=310.63K, cov=0.3738;
图17是主要的三个频率的微波其输出功率实验结果可以做到接近一致。Figure 17 shows that the experimental results of the output power of the three main frequencies of microwaves can be close to the same.
附图中:1-磁控管电源、2-磁控管、3-中频信号发生器、41-第一电容、42-第二可调电容、43-第三可调电容、44-第四电容、45-第五电容、51-第一电感、52-第二电感、53-第三电感、61-第一电阻、62-第二电阻、63-第三电阻、71-第一阴极电源线、72-第二阴极电源线、8-腔体,9-物料。In the drawings: 1-magnetron power supply, 2-magnetron, 3-intermediate frequency signal generator, 41-first capacitor, 42-second adjustable capacitor, 43-third adjustable capacitor, 44-fourth Capacitor, 45-fifth capacitor, 51-first inductor, 52-second inductor, 53-third inductor, 61-first resistor, 62-second resistor, 63-third resistor, 71-first cathode power supply Line, 72-second cathode power line, 8-cavity, 9-material.
具体实施方式Detailed ways
下面结合附图与具体实施方式,对本发明进一步详细说明,但是本发明不局限于以下实施例。The present invention will be described in further detail below with reference to the accompanying drawings and specific embodiments, but the present invention is not limited to the following examples.
实施例一:Example 1:
见附图1~11、14。磁控管阳极电源纹波混频多频加热装置,包括磁控管电源1、磁控管2、中频信号发生器3、第一电容41和腔体8;所述磁控管电源1连有第一阴极电源线71和第二阴极电源线72;所述第一阴极电源线71和第二阴极电源线72分别与磁控管2的阴极两端连接;所述第一电容41一端和中频信号发生器3连接,另一端和第一阴极电源线71连接;所述腔体8上设有馈口;所述磁控管2通过馈口向腔体8内输入多个频率的微波。See Figures 1 to 11 and 14. The magnetron anode power supply ripple mixing multi-frequency heating device includes a
单个磁控管能够输出多个频率微波的工作原理:The working principle of a single magnetron capable of outputting multiple frequencies of microwaves:
本发明充分利用磁控管作为幅度非线性响应器件的特性,结合磁控管阳极电压纹波对其输出频谱特性的影响,将磁控管作为混频器使用。所述磁控管电源1为磁控管2供电;所述中频信号发生器3产生已调制的中频信号,中频信号通过第一电容41输入到第一阴极电源线71上,此时中频信号等效为磁控管2阳极电压的纹波加载到磁控管2阳极电压上,并将磁控管2本身激励起的谐振信号作为本地振荡信号,当中频信号作为阳极电压纹波与磁控管2的谐振信号发生作用时,磁控管2非线性响应的特性使磁控管2的输出端产生多个频率的微波,这些频率是中频信号的频率与谐振信号的频率进行线性运算的结果。同时,多个频率的微波可以直接通过馈口输入腔体8内,对物料9进行均匀加热。The invention makes full use of the characteristics of the magnetron as an amplitude nonlinear response device, and uses the magnetron as a mixer in combination with the influence of the anode voltage ripple of the magnetron on its output spectrum characteristics. The
磁控管结构:磁控管具有一个圆筒状阳极,阳极叶片沿着径向安装在阳极的内壁上,螺旋灯丝作为阴极,阴极位于磁控管中心,天线安装在阳极叶片之一上,多个冷却片安置在阳极的外圆周表面上,两个磁铁分别安装在阳极顶部和底部形成磁场。磁控管电源1通过第一阴极电源线71和第二阴极电源线72为阴极供电,加热阴极灯丝使之发射出热电子,热电子在受到电场和磁场作用下,借助阳极叶片形成的若干个共振空腔,在做摆线运动的同时,把电子能转换为高频能量,即微波,微波通过天线发射出去。磁控管电源1为阴极提供3.3V电压,阳极接地,阴极和阳极之间具有4kV左右的负高压。Magnetron structure: The magnetron has a cylindrical anode, the anode blade is installed on the inner wall of the anode along the radial direction, the spiral filament is used as the cathode, the cathode is located in the center of the magnetron, the antenna is installed on one of the anode blades, and many A cooling fin is placed on the outer circumferential surface of the anode, and two magnets are installed at the top and bottom of the anode to form a magnetic field. The
所述第一阴极电源线71和第二阴极电源线72分别与磁控管2的阴极两端直接或间接连接;阴极两端可以分别通过扼流线圈连接第一阴极电源线71和第二阴极电源线72。第一电容41用来隔直流通交流,防止磁控管电源1的高压直流跑到中频信号发生器3里面去,同时保证中频信号发生器3产生的已调制中频信号,能够输入到第一阴极电源线71上。The first cathode
理论推导:Theoretical derivation:
见图2,本发明在磁控管等效RLC谐振电路模型的基础上,磁控管自由振荡稳定状态下的电路方程:Referring to Fig. 2, the present invention is based on the equivalent RLC resonant circuit model of the magnetron, and the circuit equation under the free oscillation stable state of the magnetron:
其中,in,
ω为磁控管的振荡频率,即磁控管的输出端产生的信号振荡频率;ω0为谐振腔本振频率,即磁控管本身激励起的谐振信号作为本地振荡信号的频率;Q0为谐振电路的固有品质因数;Qext为谐振电路的外部品质因数;Vdc为磁控管的阳极电压,即磁控管的阴极和阳极之间的电压,阳极接地;VRF为高频电压,即磁控管的输出端产生的信号的电压;A为中频信号的幅度;f为中频信号的频率;g+jb为等效的磁控管源部分,g为磁控管源电子电导,b为磁控管源电子电纳;G+jB为等效负载,G为负载端电子电导,B为负载端电子电纳;j为虚数单位;b0、tanα为常数;R、L、C分别为等效电阻、等效电感和等效电容;t为时间变量。J.C.Slater曾在1947年4月3日发表过名为“THE PHASING OF MAGNETRONS”的论文,有具体讲述以上理论原理,目前已属于本领域公知常识,可以直接拿来使用。ω is the oscillation frequency of the magnetron, that is, the oscillation frequency of the signal generated by the output end of the magnetron; ω 0 is the local oscillation frequency of the resonant cavity, that is, the resonant signal excited by the magnetron itself is used as the frequency of the local oscillation signal; Q 0 is the intrinsic quality factor of the resonant circuit; Q ext is the external quality factor of the resonant circuit; V dc is the anode voltage of the magnetron, that is, the voltage between the cathode and the anode of the magnetron, and the anode is grounded; V RF is the high-frequency voltage , that is, the voltage of the signal generated at the output end of the magnetron; A is the amplitude of the intermediate frequency signal; f is the frequency of the intermediate frequency signal; g+jb is the equivalent magnetron source part, g is the electron conductance of the magnetron source, b is the electronic susceptance of the magnetron source; G+jB is the equivalent load, G is the electronic conductance of the load end, B is the electronic susceptance of the load end; j is the imaginary unit; b 0 , tanα are constants; R, L, C are the equivalent resistance, equivalent inductance and equivalent capacitance, respectively; t is the time variable. JCSlater once published a paper named "THE PHASING OF MAGNETRONS" on April 3, 1947, in which the above theoretical principles are described in detail. It is now common knowledge in the field and can be used directly.
为了分析磁控管的起振过程,在其初始振荡的过程中,可以假设其电压的幅度随时间呈指数变化,将频率表示成复数,其虚部代表指数增长的关系,即:In order to analyze the start-up process of the magnetron, in the process of its initial oscillation, it can be assumed that the amplitude of its voltage changes exponentially with time, and the frequency is expressed as a complex number, and its imaginary part represents the relationship of exponential growth, namely:
ω=ω1+jω2 ω=ω 1 +jω 2
高频电压随时间变化的关系表示为因此定义则ω=ω1+jГ(t)。此时,磁控管自由振荡稳定状态下的电路方程可以改写为:The relationship of the high frequency voltage with time is expressed as So define Then ω=ω 1 +jГ(t). At this point, the circuit equation in the free oscillation steady state of the magnetron can be rewritten as:
将该方程中实部与虚部分离可得:Separating the real and imaginary parts of this equation gives:
其中 in
对实部表达式求解可得磁控管自由振荡状态下的高频输出电压为: Solving the real part expression, the high-frequency output voltage of the magnetron in the free oscillation state can be obtained as:
同理,对虚部表达式求解可得磁控管自由振荡状态瞬态输出频率为: Similarly, by solving the imaginary part expression, the transient output frequency of the free oscillation state of the magnetron can be obtained as:
其中, in,
表明磁控管稳定工作之后其频率由三部分组成:It shows that after the magnetron works stably, its frequency consists of three parts:
ω0代表谐振腔的本振频率;代表由电子束引起的频率前推效应;代表由负载引起的频率牵引效应。ω 0 represents the local oscillator frequency of the resonator; represents the frequency push effect caused by the electron beam; Represents the frequency pulling effect caused by the load.
综上所述,在将中频信号加载到磁控管阳极电压上,等效为阳极电压纹波时,自由振荡稳定状态下的磁控管输出信号表达式为:To sum up, when the intermediate frequency signal is loaded on the anode voltage of the magnetron, which is equivalent to the anode voltage ripple, the output signal of the magnetron in the free oscillation stable state is expressed as:
V(t)=VRF(t)·sin(ω(t)·t)V(t)= VRF (t)·sin(ω(t)·t)
将前文中理论推导得到的磁控管输出表达式进行快速傅里叶变换,可以得到该表达式对应的频域图。图3是磁控管输出信号时域图像;对推导得到的阳极电压含有中频信号的自由振荡磁控管稳定状态下输出信号的表达式进行作图,边带包络的深度表示了加载的中频信号的幅度,边带包络的频率则与中频信号的频率有关。图4是磁控管输出信号频域图像;对推导得到的表达式进行快速傅里叶变换作出的图,图像中最高强度的频率点代表了自由振荡磁控管的中心频率,中心频率两边的强度稍弱的次频率点代表了磁控管本振频率与中频信号频率混频之后得到的新频点,中心频率与次频率分量之间的频率差即中频信号的频率。根据磁控管输出的频域图像,在磁控管输出信号的中心频率两边出现强度稍弱的次频率分量,而中心频率与次频率分量之间的频率差即为加载在阳极电压上的中频信号的频率,意味着磁控管起到了预期的混频器的作用。Fast Fourier transform is performed on the magnetron output expression derived theoretically in the previous section, and the frequency domain diagram corresponding to the expression can be obtained. Figure 3 is the time-domain image of the output signal of the magnetron; the derived expression of the output signal of the free-oscillating magnetron in the steady state with the anode voltage containing the intermediate frequency signal is plotted, and the depth of the sideband envelope represents the loaded intermediate frequency The amplitude of the signal, and the frequency of the sideband envelope is related to the frequency of the IF signal. Figure 4 is the frequency domain image of the output signal of the magnetron; the figure obtained by fast Fourier transform of the derived expression, the frequency point with the highest intensity in the image represents the center frequency of the free oscillating magnetron, and the frequency points on both sides of the center frequency The sub-frequency point with slightly weaker intensity represents the new frequency point obtained by mixing the local oscillator frequency of the magnetron with the frequency of the intermediate frequency signal. The frequency difference between the center frequency and the sub-frequency component is the frequency of the intermediate frequency signal. According to the frequency domain image output by the magnetron, a slightly weaker sub-frequency component appears on both sides of the center frequency of the magnetron output signal, and the frequency difference between the center frequency and the sub-frequency component is the intermediate frequency loaded on the anode voltage. The frequency of the signal means that the magnetron acts as the intended mixer.
图5是加载了中频信号的磁控管阳极电压波形图;原本理想阳极电压为直流电压,加载的中频信号即体现为该直流电压上的纹波分量,此处将携带信息的复杂的中频信号简化为单一频率的正弦信号。图6是自由振荡状态下磁控管输出信号时域图像,通过电磁仿真软件对磁控管进行建模,仿真计算得到了自由振荡稳定状态下磁控管时域输出图像,边带包络特征与图3推导得到的图像类似。图7是自由振荡状态下磁控管输出信号频域图像,通过仿真计算得到的磁控管输出频谱图,图像上的中心频率与次频率分量之间的关系特征与图4推导得到的图像类似。在电磁仿真软件CST Studio Suite对阳极电压上加载了中频信号作为等效纹波的自由振荡状态磁控管进行仿真,得到的输出频谱结果同样验证了磁控管可以起到混频器的作用。Figure 5 is a waveform diagram of the anode voltage of the magnetron loaded with an intermediate frequency signal; the ideal anode voltage is a DC voltage originally, and the loaded intermediate frequency signal is reflected as the ripple component on the DC voltage. Here, the complex intermediate frequency signal carrying information will be Simplified to a single frequency sinusoidal signal. Figure 6 is the time-domain image of the output signal of the magnetron in the free oscillation state. The magnetron is modeled by electromagnetic simulation software. The simulation calculation obtains the time-domain output image of the magnetron in the free oscillation stable state, and the sideband envelope characteristics Similar to the image derived from Figure 3. Figure 7 is the frequency domain image of the output signal of the magnetron in the free oscillation state. The output spectrum of the magnetron is obtained by simulation calculation. The relationship between the center frequency and the sub-frequency component on the image is similar to the image derived from Figure 4. . In the electromagnetic simulation software CST Studio Suite, the free oscillation state magnetron with the intermediate frequency signal loaded on the anode voltage as the equivalent ripple is simulated, and the output spectrum results obtained also verify that the magnetron can function as a mixer.
在此基础上,本发明搭建测试系统对数值计算和软件仿真的结果进行验证,本系统使用的是松下生产的2M244-M1型磁控管,在未加载中频信号时,磁控管的输出频谱如附图8所示;加载不同频率的中频信号之后,磁控管输出频谱如附图9、附图10、附图11所示。图像上的中心频率与次频率分量之间的关系特征与图4推导得到的图像类似,中心频率与次频率分量之间的频率差即为加载在阳极电压上的中频信号的频率,说明中频信号等效为磁控管阳极电压的纹波加载到磁控管阳极电压上,并将磁控管本身激励起的谐振信号作为本地振荡信号,能够利用磁控管进行混频使磁控管的输出端产生主要的三个频率的微波,即中心频率以及中心频率两边出现的强度稍弱的次频率分量,所以中频信号不仅可以使磁控管的输出端产生主要的三个频率的微波,而且还可以影响频率的分布,使频率可调可控,主要的三个频率的微波可以对物料进行均匀加热。On this basis, the present invention builds a test system to verify the results of numerical calculation and software simulation. The system uses the 2M244-M1 magnetron produced by Panasonic. When the intermediate frequency signal is not loaded, the output spectrum of the magnetron is As shown in FIG. 8 ; after loading intermediate frequency signals of different frequencies, the output spectrum of the magnetron is shown in FIG. 9 , FIG. 10 , and FIG. 11 . The relationship between the center frequency and the sub-frequency component on the image is similar to the image derived from Figure 4. The frequency difference between the center frequency and the sub-frequency component is the frequency of the intermediate frequency signal loaded on the anode voltage, indicating that the intermediate frequency signal The ripple equivalent to the anode voltage of the magnetron is loaded on the anode voltage of the magnetron, and the resonance signal excited by the magnetron itself is used as the local oscillation signal, and the output of the magnetron can be mixed by using the magnetron. The main three frequencies of microwaves are generated at the end of the magnetron, that is, the center frequency and the slightly weaker sub-frequency components appearing on both sides of the center frequency, so the intermediate frequency signal can not only make the output end of the magnetron generate the main three frequencies of microwaves, but also It can affect the frequency distribution, make the frequency adjustable and controllable, and the main three frequencies of microwave can heat the material evenly.
实施例二:Embodiment 2:
见附图1~11、14。在实施例一的基础上,所述第一电容41与第一阴极电源线71连接交点和磁控管电源1之间的第一阴极电源线71上设有第一电感51。由上述结构可知,第一电感51用来隔交流通直流,防止中频信号进入磁控管电源1,同时又保障高压直流和低频直流灯丝电流能进入到磁控管。See Figures 1 to 11 and 14. On the basis of the first embodiment, the
所述第二阴极电源线72上设有第二电感52。由上述结构可知,第二电感52用来隔交流通直流,防止中频信号进入磁控管电源1,同时又保障高压直流和低频直流灯丝电流能进入到磁控管。The second
还包括第三电感53;所述第三电感53一端与中频信号发生器3以及第一电容41连接中频信号发生器3的一端均连接,另一端接地。由上述结构可知,当第一电容41失效短路时,高压就直接加在中频信号发生器3上了,所以增加第三电感53,第一电容41失效短路时高压直流就通过第三电感53接地。第三电感53起到保护中频信号发生器3的作用。It also includes a
还包括第四电容44;所述第四电容44一端与磁控管电源1和第一电感51之间的第一阴极电源线71连接,另一端接地。由上述结构可知,第四电容44防止高频信号回到磁控管电源1。It also includes a
还包括第五电容45;所述第五电容45一端与磁控管电源1和第二电感52之间的第二阴极电源线72连接,另一端接地。由上述结构可知,第五电容45防止高频信号回到磁控管电源1。It also includes a
还包括第一电阻61、第二电阻62和第三电阻63;所述第一电阻61和第三电感53两端并联;所述第二电阻62和第一电感51两端并联;所述第三电阻63和第二电感52两端并联。由上述结构可知,第一电阻61、第二电阻62和第三电阻63分别用来降低第三电感53、第一电感51、第二电感52的Q值,避免电感产生谐振。It also includes a
还包括阻抗匹配调节器;所述阻抗匹配调节器包括第二可调电容42和第三可调电容43;所述第二可调电容42一端与中频信号发生器3以及第一电容41连接中频信号发生器3的一端均连接,另一端接地;所述第三可调电容43一端与中频信号发生器3以及第一电容41连接中频信号发生器3的一端均连接,另一端接地。由上述结构可知,阻抗匹配调节器用于和电路进行阻抗匹配。It also includes an impedance matching regulator; the impedance matching regulator includes a second
还包括电路板;所述第一电容41、第一电感51、第二电感52、第三电感53、第四电容44、第五电容45、第一电阻61、第二电阻62和第三电阻63集成在电路板上;所述电路板包括第一端口、第二端口、第三端口、第四端口和第五端口;所述第一端口位于第一电感51和磁控管电源1之间的第一阴极电源线71上;所述第二端口位于第二电感52和磁控管电源1之间的第二阴极电源线72上;所述第三端口位于第一电感51和磁控管2之间的第一阴极电源线71上;所述第四端口位于第二电感52和磁控管2之间的第二阴极电源线72上;所述第五端口位于中频信号发生器3和第一电容41之间,使中频信号发生器3和第一电容41连通。由上述结构可知,将第一电容41、第一电感51、第二电感52、第三电感53、第四电容44、第五电容45、第一电阻61、第二电阻62和第三电阻63集成在电路板上,方便模块化使用,直接将中频信号发生器3、磁控管电源1、磁控管2分别和电路板对应的端口连接,结构更加简化简单。It also includes a circuit board; the
一般出现的三个主要强度的微波频率为中心频率以及中心频率两边出现的强度稍弱的次频率分量,可以通过调整调制电路的匹配后,使磁控管输出的中心频率强度与次频率分量强度相同,也就是功率一致,这将更有助于物料均匀加热。The three main intensities of microwave frequencies that generally appear are the center frequency and the slightly weaker sub-frequency components appearing on both sides of the center frequency. After adjusting the matching of the modulation circuit, the intensity of the center frequency output by the magnetron and the intensity of the sub-frequency components can be adjusted. The same, that is, the same power, which will help the material to be heated evenly.
实施例三:Embodiment three:
见附图1~11、14。磁控管阳极电源纹波混频多频加热方法,采用上述实施例任一磁控管阳极电源纹波混频多频加热装置;具体步骤为:所述磁控管电源1为磁控管2供电;所述中频信号发生器3产生中频信号,中频信号通过第一电容41输入到第一阴极电源线71上,此时中频信号等效为磁控管2阳极电压的纹波加载到磁控管2阳极电压上,并将磁控管2本身激励起的谐振信号作为本地振荡信号,当中频信号作为阳极电压纹波与磁控管2的谐振信号发生作用时,磁控管2非线性响应的特性使磁控管2的输出端产生多个频率的微波,多个频率的微波通过馈口输入腔体8内,对物料9进行加热。本发明方法充分利用磁控管作为幅度非线性响应器件的特性,结合磁控管阳极电压纹波对其输出频谱特性的影响,将磁控管作为混频器使用,无需单独设置混频器及配合大量辅助配件就能够使磁控管2的输出端产生多个频率可控可调的微波,多个频率的微波通过馈口输入腔体8内,对物料9进行均匀加热。See Figures 1 to 11 and 14. A method for heating a magnetron anode power supply ripple frequency mixing and multi-frequency, using any of the above-mentioned embodiments of the magnetron anode power supply ripple mixing and multi-frequency heating device; the specific steps are: the
实际上磁控管输出大量不同频率的微波,但主要的三个频率的微波强度较高,所以只考虑这三个频率的微波,其余低强度的频率微波可以忽略。只需要在COMSOLMultiphysics仿真软件中对磁控管输出三个不同频率微波实现改善物料加热均匀性进行验证即可:In fact, the magnetron outputs a large number of microwaves of different frequencies, but the three main frequencies of microwaves have high intensities, so only the microwaves of these three frequencies are considered, and the remaining low-intensity microwaves can be ignored. It only needs to be verified in the COMSOL Multiphysics simulation software that the magnetron outputs three different frequency microwaves to improve the heating uniformity of the material:
实验说明:因为在该软件中不能实现同时馈入频率不同的源,本发明采用在COMSOL Multiphysics中使用单一频率源馈入,将不同频率下得到的温升结果导出到MATLAB软件中进行计算,以此来模拟磁控管三频同时输出的效果。Experiment description: Because it is impossible to feed sources with different frequencies at the same time in this software, the present invention uses a single frequency source to feed in COMSOL Multiphysics, and the temperature rise results obtained at different frequencies are exported to MATLAB software for calculation. This is to simulate the effect of the three-frequency output of the magnetron at the same time.
首先腔体设计为405×295×340mm的矩形腔体,磁控管采用BJ-26矩形波导馈电,腔体内放置尺寸为50×50×50mm的土豆作为物料。仿真验证中利用频率为2.45GHz、功率为600W的单一微波源与中心频率为2.45GHz、频差2~8MHz(例如,频差2MHz即三个微波频率为2.448GHz、2.45GHz、2.452GHz),功率均为200W的三个不同频率微波分别进行馈电,再将温升数据导入到MATLAB中进行计算,模拟三频加热结果,以此种方法对比验证加热均匀性的改善效果。First, the cavity is designed as a rectangular cavity of 405×295×340mm, the magnetron is fed by a BJ-26 rectangular waveguide, and potatoes with a size of 50×50×50mm are placed in the cavity as materials. In the simulation verification, a single microwave source with a frequency of 2.45GHz and a power of 600W is used with a center frequency of 2.45GHz and a frequency difference of 2-8MHz (for example, a frequency difference of 2MHz means that the three microwave frequencies are 2.448GHz, 2.45GHz, and 2.452GHz). Three different frequency microwaves with a power of 200W were fed separately, and then the temperature rise data was imported into MATLAB for calculation, and the three-frequency heating results were simulated. This method was used to compare and verify the improvement effect of heating uniformity.
利用MTALAB软件计算出各情况下的平均温度(ave)及温度变异系数(cov),温度变异系数(cov)是原始数据标准差与原始数据平均数的比,反映数据离散程度的绝对值,cov值越小,说明加热越均匀。同时计算了土豆不同位置下的改善加热均匀性情况。Use MTALAB software to calculate the average temperature (ave) and temperature coefficient of variation (cov) in each case. The temperature coefficient of variation (cov) is the ratio of the standard deviation of the original data to the average of the original data, reflecting the absolute value of the degree of dispersion of the data, cov Smaller values indicate more uniform heating. At the same time, the improvement of heating uniformity under different positions of potatoes was calculated.
下表为土豆处于腔体中心点正下方50mm的数据:The following table shows the data when the potato is 50mm directly below the center point of the cavity:
下表为土豆处于中心点正下方80mm的数据:The following table shows the data of potatoes at 80mm directly below the center point:
将腔体设计为450×350×340mm的矩形腔体,下表为土豆处于中心点正下方80mm的数据:The cavity is designed as a rectangular cavity of 450×350×340mm. The following table shows the data of the potato being 80mm directly below the center point:
通过以上数据可以得出结论,将中频信号调制到磁控管高压电源上的调制电路,使磁控管混频产生具有指定频差的微波信号,实现三频输出的微波加热对改善加热均匀性具有良好的效果,能到达到预期目的。可以根据实验,选取最优的中频信号的频率,使物料加热均匀性最优。From the above data, it can be concluded that the modulation circuit that modulates the intermediate frequency signal to the magnetron high-voltage power supply makes the magnetron mix frequency to generate a microwave signal with a specified frequency difference, and realizes the microwave heating of the three-frequency output to improve the heating uniformity. It has good effect and can achieve the expected purpose. According to the experiment, the frequency of the optimal intermediate frequency signal can be selected to make the heating uniformity of the material optimal.
图15是腔体设计为405×295×340mm的矩形腔体,土豆处于腔体中心点正下方50mm,初始温度293.15K,加热时间20s的加热仿真图,单频输入2.45GHz的微波,功率600W,可看出平均温度ave=313.68K,cov=0.5352;Figure 15 is a heating simulation diagram of the cavity designed as a rectangular cavity of 405×295×340mm, the potato is 50mm directly below the center point of the cavity, the initial temperature is 293.15K, and the heating time is 20s. The single-frequency input microwave is 2.45GHz and the power is 600W. , it can be seen that the average temperature ave=313.68K, cov=0.5352;
图16是腔体设计为405×295×340mm的矩形腔体,土豆处于腔体中心点正下方50mm,初始温度293.15K,加热时间20s的加热仿真图,输入三频频差4MHz(2.45GHz、2.446GHz、2.454GHz)的微波,功率200W,可看出平均温度ave=310.63K,cov=0.3738;Figure 16 is a heating simulation diagram of a rectangular cavity with a cavity design of 405×295×340mm, the potato is 50mm directly below the center point of the cavity, the initial temperature is 293.15K, and the heating time is 20s. GHz, 2.454GHz) microwave, power 200W, it can be seen that the average temperature ave=310.63K, cov=0.3738;
由图15、16对比可以看出,三频加热的最高温度和平均温度没有单频加热高,但平均温度差别较小,且由体表面的温度分布可以看出三频加热对均匀性的确存在一定的改善作用。From the comparison of Figures 15 and 16, it can be seen that the maximum temperature and average temperature of triple-frequency heating are not as high as those of single-frequency heating, but the difference in average temperature is small, and it can be seen from the temperature distribution of the body surface that triple-frequency heating does exist for uniformity. certain improvement.
由图17可以看出,通过改变中频信号的功率,实验可以得到主要的三个频率的微波其输出功率做到接近一致,越接近则加热越均匀。As can be seen from Figure 17, by changing the power of the intermediate frequency signal, the experiment can obtain that the output power of the three main frequencies of microwaves is close to the same, and the closer it is, the more uniform the heating is.
以上所述仅为本发明的优选实施例,并非因此限制本发明的专利范围,凡是利用本发明说明书及附图内容所作的等效结构或等效流程变换,或直接或间接运用在其他相关的技术领域,均同理包括在本发明的专利保护范围内。The above descriptions are only preferred embodiments of the present invention, and are not intended to limit the scope of the present invention. Any equivalent structure or equivalent process transformation made by using the contents of the description and drawings of the present invention, or directly or indirectly applied to other related All technical fields are similarly included in the scope of patent protection of the present invention.
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