CN107273563B - Equivalent calculation method for parasitic capacitance of PCB winding of planar transformer - Google Patents

Equivalent calculation method for parasitic capacitance of PCB winding of planar transformer Download PDF

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CN107273563B
CN107273563B CN201710270652.0A CN201710270652A CN107273563B CN 107273563 B CN107273563 B CN 107273563B CN 201710270652 A CN201710270652 A CN 201710270652A CN 107273563 B CN107273563 B CN 107273563B
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CN107273563A (en
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钱钦松
张乐
刘琦
孙伟锋
陆生礼
时龙兴
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    • G06COMPUTING; CALCULATING OR COUNTING
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    • H01F27/34Special means for preventing or reducing unwanted electric or magnetic effects, e.g. no-load losses, reactive currents, harmonics, oscillations, leakage fields
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    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
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    • H01F27/2804Printed windings
    • H01F2027/2809Printed windings on stacked layers
    • HELECTRICITY
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    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/28Coils; Windings; Conductive connections
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Abstract

本发明公开了一种平面变压器PCB绕组寄生电容等效计算方法,通过对平面变压器PCB绕组的建模和分析,模拟PCB绕组寄生电容的分布情况,通过计算存在寄生电容的各相邻两层之间寄生电容存储能量的大小并进行叠加,利用能量和寄生电容之间的关系以及能量守恒定律,对PCB绕组整体的寄生电容进行计算,然后将其等效为三个部分的电容的计算,即原边绕组同名端与副边绕组同名端之间的电容C1、原边绕组同名端与副边绕组异名端之间的电容C2以及原边绕组异名端与副边绕组同名端之间的电容C3

Figure 201710270652

The invention discloses an equivalent calculation method for the parasitic capacitance of the PCB winding of a planar transformer. By modeling and analyzing the PCB winding of the planar transformer, the distribution of the parasitic capacitance of the PCB winding is simulated. The parasitic capacitance stores the energy and superimposes them. Using the relationship between energy and parasitic capacitance and the law of energy conservation, the parasitic capacitance of the PCB winding as a whole is calculated, and then it is equivalent to the calculation of the capacitance of the three parts, namely Capacitance C 1 between the same-named end of the primary winding and the same-named end of the secondary winding, capacitance C2 between the same - named end of the primary winding and the same-named end of the secondary winding, and the difference between the same-named end of the primary winding and the same-named end of the secondary winding capacitor C3 between.

Figure 201710270652

Description

一种平面变压器PCB绕组寄生电容等效计算方法An Equivalent Calculation Method for Parasitic Capacitance of PCB Windings of Planar Transformers

技术领域technical field

本发明涉及PCB型平面变压器,尤其是一种平面变压器PCB绕组寄生电容等效计算方法,可应用于平面变压器寄生参数分析以及电磁兼容领域中EMI传导模型的建立。The invention relates to a PCB-type planar transformer, in particular to an equivalent calculation method for the parasitic capacitance of the PCB winding of the planar transformer, which can be applied to the analysis of the parasitic parameters of the planar transformer and the establishment of an EMI conduction model in the field of electromagnetic compatibility.

背景技术Background technique

平面变压器具有高度低、体积小、一致性好、便于批量生产、漏感小、散热性好、电磁兼容性能好等优点,是目前应用较为广泛的新型变压器。平面变压器有多种,其中PCB平面变压器由于其成本低廉、结构稳固、制作方便等优点而得到最为广泛的应用。其结构比较简单,将各层绕组的过孔焊接即可。平面变压器的寄生电容是开关电源设计中的一个不可回避的实际问题,往往会使开关电源的工作状态偏离设计结果,甚至严重影响电源的技术指标。从而在开关电源的设计过程中必须考虑到这些寄生电容的影响。因此,采用何种方法来计算平面变压器PCB绕组寄生电容的大小就显得尤为重要。Planar transformers have the advantages of low height, small size, good consistency, easy mass production, small leakage inductance, good heat dissipation, and good electromagnetic compatibility. They are new types of transformers that are widely used. There are many kinds of planar transformers. Among them, PCB planar transformers are the most widely used due to their advantages of low cost, stable structure, and convenient production. Its structure is relatively simple, and the via holes of each layer of windings can be welded. The parasitic capacitance of the planar transformer is an unavoidable practical problem in the design of switching power supplies, which often makes the working state of the switching power supply deviate from the design results, and even seriously affects the technical indicators of the power supply. Therefore, the influence of these parasitic capacitances must be considered in the design process of the switching power supply. Therefore, it is very important to use which method to calculate the parasitic capacitance of the PCB winding of the planar transformer.

平面变压器按设计制作工艺的不同,可分为印刷电路(PCB)型,厚膜型、薄膜型、亚微米型4种。其中PCB型平面变压器主要由平面磁芯、PCB绕组和绝缘层三部分组成。平面变压器要求磁芯、绕组是平面结构,所以应该采用多层PCB绕组,一般在八层到十层,多的接近二十层。在PCB型平面变压器中,PCB绕组是做在印制电路板上的圆形扁平传导导线或是直接用铜泊,各层绕组间距小并且存在较大的正对面积,使得寄生电容不可避免的存在。可以认为PCB型平面变压器的寄生电容主要存在于PCB绕组之间。该寄生电容会使开关电源的工作状态偏离设计结果,甚至严重影响电源的技术指标。寄生电容的影响不可消除,但我们可以进行估算,从而在开关电源的设计过程中考虑到这些寄生电容的影响。Planar transformers can be divided into four types: printed circuit (PCB) type, thick-film type, thin-film type, and sub-micron type according to different design and manufacturing processes. Among them, the PCB-type planar transformer is mainly composed of three parts: a planar magnetic core, a PCB winding and an insulating layer. Planar transformers require the magnetic core and winding to be of a planar structure, so multi-layer PCB windings should be used, generally eight to ten layers, and more than twenty layers. In the PCB-type planar transformer, the PCB windings are round flat conductive wires made on the printed circuit board or directly made of copper. exist. It can be considered that the parasitic capacitance of the PCB-type planar transformer mainly exists between the PCB windings. The parasitic capacitance will make the working state of the switching power supply deviate from the design results, and even seriously affect the technical indicators of the power supply. The effects of parasitic capacitance cannot be eliminated, but we can estimate to account for these parasitic capacitance effects in the design of switching power supplies.

平面变压器PCB绕组分为两部分,原边绕组(P)和副边绕组(S)。原边绕组采用串联方式来增加匝数;为了增加绕组的载流能力,副边绕组一般采用并联结构。平面变压器原边绕组一般都是单匝形式或者都是多匝形式,并且采用串联形式;副边侧绕组都为单匝形式,并且采用并联结构。PCB型平面变压器的绕组结构存在多种方式,可以分为简单结构、三明治结构和交错结构。三种绕组形式虽然结构不同,都不可避免地会产生寄生电容。简单结构寄生电容较小;交错结构寄生电容很大;三明治结构的寄生电容大小介于二者之间。在计算寄生电容的大小时,非相邻两层绕组电容相比于相邻两层绕组间电容小得多,可以忽略不计;单层绕组自身虽然也存在电容,但一般平面变压器各层绕组很薄,可以忽略不计;副边绕组采用并联结构,当相邻两层绕组都为副边绕组时,不存在电势差,可以认为其寄生电容为零。The planar transformer PCB winding is divided into two parts, the primary winding (P) and the secondary winding (S). The primary winding is connected in series to increase the number of turns; in order to increase the current carrying capacity of the winding, the secondary winding generally adopts a parallel structure. The primary windings of planar transformers are generally single-turn or multi-turn, and are in series; the secondary windings are single-turn and parallel. There are many ways of winding structure of PCB type planar transformer, which can be divided into simple structure, sandwich structure and staggered structure. Although the three types of windings have different structures, parasitic capacitance will inevitably occur. The parasitic capacitance of the simple structure is small; the parasitic capacitance of the staggered structure is large; the parasitic capacitance of the sandwich structure is between the two. When calculating the size of the parasitic capacitance, the capacitance of the non-adjacent two-layer windings is much smaller than the capacitance between the adjacent two-layer windings and can be ignored; although the single-layer winding itself also has capacitance, the windings of each layer of the general planar transformer are very small. Thin, can be ignored; the secondary winding adopts a parallel structure, when the two adjacent layers of windings are both secondary windings, there is no potential difference, and the parasitic capacitance can be considered to be zero.

任何金属件之间都有电容存在,现有平面变压器PCB绕组寄生电容计算方法是,将每层绕组视作一个等势面,即绕组上没有压降,利用静态电容公式C=Q/U来计算绕组之间的电容大小。但在变压器中,同一绕组线匝之间、不同绕组之间、绕组对屏蔽层之间、沿着某一线长度之间的电位是变化的,这样形成的电容不同于静电容,称为分布电容。因此不能用计算静电容的方法直接计算分布电容。本发明提出一种更加精确的、适应性强的平面变压器PCB绕组寄生电容计算方法来解决现有难题。There is capacitance between any metal parts. The existing method for calculating the parasitic capacitance of PCB windings of planar transformers is to treat each layer of windings as an equipotential surface, that is, there is no voltage drop on the windings, and use the static capacitance formula C=Q/U to calculate. Calculate the size of the capacitance between the windings. However, in the transformer, the potential between turns of the same winding, between different windings, between the windings to the shielding layer, and between the lengths of a line varies, so the capacitance formed in this way is different from the electrostatic capacitance, which is called distributed capacitance. Therefore, the distributed capacitance cannot be directly calculated by the method of calculating the electrostatic capacitance. The present invention proposes a more accurate and highly adaptable method for calculating the parasitic capacitance of the PCB winding of a planar transformer to solve the existing problems.

发明内容SUMMARY OF THE INVENTION

本发明针对现有平面变压器寄生电容计算方法的不适用性,提供一种平面变压器PCB绕组寄生电容等效计算方法,该方法计算快速、准确,适应性强,具有较高实际应用价值。Aiming at the inapplicability of the existing plane transformer parasitic capacitance calculation method, the invention provides an equivalent calculation method for the parasitic capacitance of the PCB winding of the plane transformer, which is fast, accurate, adaptable and has high practical application value.

本发明的目的是由以下技术方案来实现的:一种平面变压器PCB绕组寄生电容等效计算方法,所述平面变压器包括平面磁芯、PCB绕组和绝缘层,PCB绕组为多层结构,每一层上设置一个绕组,原边绕组与副边绕组设置在不同层上,原边绕组采用单匝或多匝其中之一,副边绕组采用单匝圆环形,多匝采用螺旋形,不同层上的原边绕组以串联方式连接,不同层上的副边绕组以并联方式连接,在相邻两层同为原边绕组及相邻两层分别为原边绕组和副边绕组的情况下,此时的相邻两层之间存在不可忽略的寄生电容;The object of the present invention is achieved by the following technical solutions: an equivalent calculation method for the parasitic capacitance of the PCB winding of a planar transformer, the planar transformer includes a planar magnetic core, a PCB winding and an insulating layer, and the PCB winding is a multi-layer structure, and each A winding is arranged on the layer, the primary winding and the secondary winding are arranged on different layers, the primary winding adopts one of single-turn or multi-turn, the secondary winding adopts a single-turn circular ring, and the multi-turn adopts a spiral shape. The primary windings are connected in series, and the secondary windings on different layers are connected in parallel. When two adjacent layers are both primary windings and two adjacent layers are primary windings and secondary windings, respectively, At this time, there is a non-negligible parasitic capacitance between two adjacent layers;

其特征在于:通过对平面变压器PCB绕组的建模和分析,模拟PCB绕组寄生电容的分布情况,通过计算存在寄生电容的各相邻两层之间寄生电容存储能量的大小并进行叠加,利用能量和寄生电容之间的关系以及能量守恒定律,对PCB绕组整体的寄生电容进行计算,然后将其等效为三个部分的电容,即原边绕组同名端与副边绕组同名端之间的电容C1、原边绕组同名端与副边绕组异名端之间的电容C2以及原边绕组异名端与副边绕组同名端之间的电容C3;包括以下步骤:It is characterized in that: through the modeling and analysis of the PCB winding of the planar transformer, the distribution of the parasitic capacitance of the PCB winding is simulated, and the energy stored in the parasitic capacitance between the two adjacent layers where the parasitic capacitance exists is calculated and superimposed, and the energy is utilized. The relationship between the parasitic capacitance and the energy conservation law, the parasitic capacitance of the PCB winding as a whole is calculated, and then it is equivalent to the capacitance of three parts, that is, the capacitance between the same-named end of the primary winding and the same-named end of the secondary winding C1 . Capacitor C2 between the same - named end of the primary winding and the synonymous end of the secondary winding, and capacitance C3 between the synonymous end of the primary winding and the same - named end of the secondary winding; including the following steps:

(1)单层绕组电势计算(1) Calculation of single-layer winding potential

1)单层单匝原边侧绕组电势表示1) Single-layer single-turn primary side winding potential representation

假设原边绕组电流按顺时针方向流动,且绕组电压沿着电流方向均匀下降,以极心到电流流入点的射线为极径建立极坐标系,取绕组上的一段圆弧作为微元dθ,微元dθ位置极坐标的角度参数为θ,该微元电压表示为:Assuming that the primary winding current flows in a clockwise direction, and the winding voltage drops uniformly along the current direction, a polar coordinate system is established with the ray from the pole center to the current inflow point as the pole diameter, and a segment of the arc on the winding is taken as the micro-element dθ, The angle parameter of the polar coordinate of the position of the micro-element dθ is θ, and the voltage of the micro-element is expressed as:

Figure GDA0002562175680000021
Figure GDA0002562175680000021

V1P是单匝原边侧绕组电流流入点电压,V2P是单匝原边侧绕组电流流出点电压;V 1P is the current inflow point voltage of single-turn primary side winding, V 2P is the current outflow point voltage of single-turn primary side winding;

2)单层单匝副边侧绕组电势表示2) Representation of single-layer single-turn secondary winding potential

原边电流与副边电流进入位置互为镜像且电流流动方向相反,副边侧绕组上微元dθ电压表示为:The primary side current and the secondary side current entry position are mirror images of each other and the current flows in opposite directions. The micro-element dθ voltage on the secondary side winding is expressed as:

Figure GDA0002562175680000031
Figure GDA0002562175680000031

V1S是单匝副边侧绕组电流流入点电压,V2S是单匝副边侧绕组电流流出点电压;V 1S is the current inflow point voltage of the single-turn secondary side winding, V 2S is the current outflow point voltage of the single-turn secondary side winding;

3)单层多匝原边侧绕组电势表示3) Single-layer multi-turn primary side winding potential representation

当原边侧绕组为多匝情况时,与原边单匝绕组不同,线圈本身是一段螺旋线,每匝螺旋线之间也会有寄生电容存在,但平面变压器各层绕组的厚度小到能够忽略螺旋线间的寄生电容,应用阿基米德螺旋方程进行拟合绕组形状,阿基米德螺旋方程表示为:When the primary side winding is multi-turn, different from the primary side single-turn winding, the coil itself is a helix, and there will also be parasitic capacitance between each turn of the helix, but the thickness of each layer of the planar transformer is small enough to Ignoring the parasitic capacitance between the spirals, the Archimedes spiral equation is used to fit the winding shape. The Archimedes spiral equation is expressed as:

r*=h·θx (3)r*=h·θ x (3)

r*表示极径,h是常数表示螺线比,r* represents the polar diameter, h is a constant representing the helical ratio,

以极心到电流流入点的射线为极径建立极坐标系,取多匝线圈上的一段长度dL作为微元,θx表示微元dL沿螺旋线到极心绕过的角度参数;该微元电压表示为:The polar coordinate system is established with the ray from the pole center to the current inflow point as the pole diameter, and a length dL on the multi-turn coil is taken as the micro-element, and θ x represents the angle parameter of the micro-element dL along the spiral line to the pole center; the micro-element The element voltage is expressed as:

Figure GDA0002562175680000032
Figure GDA0002562175680000032

A表示从电流流入点到极心的直线距离,θ1表示从电流流入点沿螺旋线到极心绕过的角度,大小为:A represents the straight-line distance from the current inflow point to the pole center, θ 1 represents the angle from the current inflow point along the spiral line to the pole center, and the magnitude is:

Figure GDA0002562175680000033
Figure GDA0002562175680000033

L表示电流流入点到电流流出点的长度,大小为:L represents the length from the current inflow point to the current outflow point, and its size is:

Figure GDA0002562175680000034
Figure GDA0002562175680000034

(r*)'表示对r*求一阶导数,B表示从电流流出点到极心的直线距离,θ2表示从电流流出点沿螺旋线到极心绕过的角度,大小为:(r*)' represents the first derivative with respect to r*, B represents the straight-line distance from the current outflow point to the pole center, θ 2 represents the angle from the current outflow point along the spiral line to the pole center, the size is:

Figure GDA0002562175680000035
Figure GDA0002562175680000035

(2)相邻两层绕组电容能量计算(2) Calculation of capacitance energy of adjacent two-layer windings

1)相邻两层单匝原边绕组与单匝原边绕组电容能量计算1) Calculation of capacitance energy between two adjacent layers of single-turn primary winding and single-turn primary winding

相邻两层单匝绕组都是原边绕组,此时二者电流方向相同,电容微元表示为:The two adjacent layers of single-turn windings are both primary windings. At this time, the current direction of the two layers is the same, and the capacitance element is expressed as:

Figure GDA0002562175680000041
Figure GDA0002562175680000041

R为绕组外径,r为绕组内径,ε为板间介电常数,d为两层绕组之间的垂直距离;R is the outer diameter of the winding, r is the inner diameter of the winding, ε is the dielectric constant between the plates, and d is the vertical distance between the two layers of windings;

电容C与能量W的关系表示为:The relationship between capacitance C and energy W is expressed as:

Figure GDA0002562175680000042
Figure GDA0002562175680000042

U1,U2分别表示电容上下极板的电势大小;U 1 , U 2 respectively represent the electric potential of the upper and lower plates of the capacitor;

由式(1)、(8)、(9),相邻两层单匝原边绕组与单匝原边绕组电容能量表示为From equations (1), (8) and (9), the capacitance energy of two adjacent layers of single-turn primary winding and single-turn primary winding is expressed as

Figure GDA0002562175680000043
Figure GDA0002562175680000043

2)相邻两层单匝原边绕组与单匝副边绕组电容能量计算2) Capacitance energy calculation of two adjacent layers of single-turn primary winding and single-turn secondary winding

相邻两层绕组一层是单匝原边绕组,另一层是单匝副边绕组,此时二者电流方向相反,由式(2)、(8)、(9),相邻两层单匝原边绕组与单匝副边绕组电容能量表示为:Two adjacent layers of windings: One layer is a single-turn primary winding, and the other layer is a single-turn secondary winding. At this time, the current directions of the two are opposite. The single-turn primary winding and single-turn secondary winding capacitance energy is expressed as:

Figure GDA0002562175680000044
Figure GDA0002562175680000044

3)相邻两层多匝原边绕组与多匝原边绕组电容能量计算3) Calculation of capacitance energy between two adjacent layers of multi-turn primary winding and multi-turn primary winding

相邻两层多匝绕组都是原边绕组,此时二者电流方向相同,电容微元表示为:The two adjacent layers of multi-turn windings are all primary windings. At this time, the two current directions are the same, and the capacitance element is expressed as:

Figure GDA0002562175680000045
Figure GDA0002562175680000045

w表示多匝线圈绕组每匝的宽度,w represents the width of each turn of the multi-turn coil winding,

由式(1)、(9)、(12),相邻两层多匝原边绕组与多匝原边绕组电容能量表示为:From equations (1), (9) and (12), the capacitance energy of two adjacent layers of multi-turn primary windings and multi-turn primary windings is expressed as:

Figure GDA0002562175680000046
Figure GDA0002562175680000046

其中,n表示单层多匝线圈总匝数,匝数从电流流入点开始计算,每转过2π计一匝,不足一匝按一匝计算,i表示第i匝;Among them, n represents the total number of turns of the single-layer multi-turn coil, the number of turns is calculated from the current inflow point, one turn is counted for every 2π revolution, and less than one turn is counted as one turn, and i represents the i-th turn;

4)相邻两层多匝原边绕组与单匝副边绕组电容能量计算4) Calculation of capacitance energy of adjacent two-layer multi-turn primary winding and single-turn secondary winding

相邻两层绕组一层是多匝原边绕组,另一层是单匝副边绕组,此时二者电流方向相反,由式(2)、(9)、(12),相邻两层多匝原边绕组与单匝副边绕组电容能量表示为:Two adjacent layers of windings: One layer is a multi-turn primary winding, and the other is a single-turn secondary winding. At this time, the current directions of the two are opposite. The capacitance energy of multi-turn primary winding and single-turn secondary winding is expressed as:

Figure GDA0002562175680000051
Figure GDA0002562175680000051

(3)等效寄生电容计算(3) Calculation of equivalent parasitic capacitance

设Ck,k+1表示第k层与第k+1层相邻两绕组间的寄生电容,Wk,k+1表示Ck,k+1的电容能量,根据PCB型平面变压器相邻绕组情况,利用式(10)、(11)、(13)、(14),计算所有相邻两层绕组之间电容能量之和WpsLet C k,k+1 represent the parasitic capacitance between the two adjacent windings of the kth layer and the k+1th layer, and W k,k+1 represent the capacitance energy of C k,k+1 . According to the adjacent PCB-type planar transformer For the winding condition, use equations (10), (11), (13), (14) to calculate the sum of capacitance energy W ps between all adjacent two-layer windings:

Wps=W12+W23...+Wk,k+1+...(15)W ps =W 12 +W 23 ...+W k,k+1 +...(15)

原副边总压降分别为Vp与Vs,原边侧每层上的总压降相同,即每层原边绕组输入电压和输出电压能够分别用Vp表示,而副边侧采用并联结构,每层压降都为Vs,用E表示项

Figure GDA0002562175680000052
的系数和、F表示项Vp·Vs的系数和、G表示项Vs 2的系数和,将(15)整理为:The total voltage drops on the primary and secondary sides are respectively V p and V s . The total voltage drop on each layer on the primary side is the same, that is, the input voltage and output voltage of the primary winding of each layer can be represented by V p respectively, while the secondary side adopts a parallel connection. structure, each pressure drop is Vs , term E
Figure GDA0002562175680000052
, F represents the coefficient sum of the term V p ·V s , G represents the coefficient sum of the term V s 2 , and (15) is organized as:

Figure GDA0002562175680000053
Figure GDA0002562175680000053

PCB绕组的寄生电容所包含的总能量,等于三个等效电容C1,C2,C3所包含的能量之和,等效电容C1,C2,C3三个电容中存储的能量计算得,The total energy contained in the parasitic capacitance of the PCB winding is equal to the sum of the energy contained in the three equivalent capacitances C 1 , C 2 , and C 3 , and the energy stored in the three equivalent capacitances C 1 , C 2 , and C 3 calculated,

Figure GDA0002562175680000054
Figure GDA0002562175680000054

由于Wps=W1+W2+W3,对比式(16)、(17),得到:Since W ps =W 1 +W 2 +W 3 , comparing formulas (16) and (17), we get:

Figure GDA0002562175680000055
Figure GDA0002562175680000055

由(18)计算得到三个等效电容C1,C2,C3的电容值。The capacitance values of the three equivalent capacitances C 1 , C 2 , and C 3 are calculated from (18).

与现有方法相比,本发明具有以下优点及显著效果:Compared with the existing method, the present invention has the following advantages and remarkable effects:

1.充分考虑单层绕组不同位置的电压变化,而非将单层绕组视作一个等势体,计算结果更加准确。1. Fully consider the voltage changes at different positions of the single-layer winding instead of treating the single-layer winding as an equipotential body, and the calculation results are more accurate.

2.利用能量与电容关系求解平面变压器PCB绕组寄生电容,将整体寄生电容等效为原边绕组与副边绕组之间的电容,具有更高的实用价值。2. Using the relationship between energy and capacitance to solve the parasitic capacitance of the PCB winding of the planar transformer, the overall parasitic capacitance is equivalent to the capacitance between the primary winding and the secondary winding, which has higher practical value.

3.本发明对现有PCB型平面变压器寄生电容计算具有广泛的适应性,为解决平面变压器寄生参数分析以及电磁兼容领域中EMI传导模型的建立提供一种思路。计算快速、准确,适应性强,具有较高的工程价值。3. The present invention has wide adaptability to the calculation of the parasitic capacitance of the existing PCB-type planar transformer, and provides an idea for solving the parasitic parameter analysis of the planar transformer and the establishment of an EMI conduction model in the field of electromagnetic compatibility. The calculation is fast, accurate, adaptable, and has high engineering value.

附图说明Description of drawings

图1是等效电容示意图;Figure 1 is a schematic diagram of equivalent capacitance;

图2a、2b、2c分别是平面变压器PCB绕组三种结构示意图;Figures 2a, 2b, and 2c are schematic diagrams of three structures of planar transformer PCB windings;

图3是单匝原边侧绕组电压梯度示意图;Figure 3 is a schematic diagram of a single-turn primary side winding voltage gradient;

图4是单匝副边侧绕组电压梯度示意图;Figure 4 is a schematic diagram of a single-turn secondary winding voltage gradient;

图5是多匝原边侧绕组电压梯度示意图;FIG. 5 is a schematic diagram of a multi-turn primary side winding voltage gradient;

图6是单匝原边侧绕组与单匝原边侧绕组电容能量计算示意图;Figure 6 is a schematic diagram of calculating the capacitance energy of a single-turn primary side winding and a single-turn primary side winding;

图7是单匝原边侧绕组与单匝副边侧绕组电容能量计算示意图;Fig. 7 is a schematic diagram of calculating the capacitance energy of a single-turn primary side winding and a single-turn secondary side winding;

图8是多匝原边侧绕组与多匝原边侧绕组电容能量计算示意图;FIG. 8 is a schematic diagram of calculating the capacitance energy of a multi-turn primary side winding and a multi-turn primary side winding;

图9是多匝原边侧绕组与单匝副边侧绕组电容能量计算示意图。FIG. 9 is a schematic diagram of the calculation of the capacitance energy of the multi-turn primary side winding and the single-turn secondary side winding.

具体实施方式Detailed ways

平面变压器内寄生电容的大小等于无数电容的叠加,不可能一一表示出来。电容的产生本质上是由于两个有不同电位差的导体之间产生了电场,而电场的存在意味着能量。因此,电容实际上就表征了存储能量的能力。换句话说,等效整体电容实际上等效了一个变压器整体的存储能量的能力。因此,可以通过计算能量来计算等效电容的大小。在开关电源的设计分析过程中,建立等效模型来表示平面变压器PCB绕组间的寄生电容。如图1所示,本发明将平面变压器PCB绕组间的寄生电容等效为三部分:(1)原边绕组同名端与副边绕组同名端之间的电容C1;(2)原边绕组同名端与副边绕组异名端之间的电容C2;(3)原边绕组异名端与副边绕组同名端之间的电容C3The size of the parasitic capacitance in the planar transformer is equal to the superposition of countless capacitances, and it is impossible to express them one by one. Capacitance is essentially due to an electric field between two conductors with different potential differences, and the presence of an electric field means energy. Therefore, capacitance actually characterizes the ability to store energy. In other words, the equivalent bulk capacitance is actually equivalent to the overall energy storage capacity of a transformer. Therefore, the size of the equivalent capacitance can be calculated by calculating the energy. In the design and analysis process of the switching power supply, an equivalent model is established to represent the parasitic capacitance between the PCB windings of the planar transformer. As shown in FIG. 1 , the present invention equivalently divides the parasitic capacitance between the PCB windings of the planar transformer into three parts: (1) the capacitance C 1 between the same-named end of the primary winding and the same-named end of the secondary winding; (2) the primary winding Capacitance C 2 between the synonymous end of the secondary winding and the synonymous end of the secondary winding; ( 3 ) Capacitance C3 between the synonymous end of the primary winding and the synonymous end of the secondary winding.

电容的大小与分布于PCB平面变压器的绕组方式密切相关。如图2所示,PCB型平面变压器的绕组结构可以分为简单结构(图2a)、三明治结构(图2b)和交错结构(图2c)。以八层PCB绕组为例,实心部分表示原边绕组(P),由四层绕组串联而成,绕组都是单匝形式或者都是多匝形式,假设其电流方向为顺时针方向;空心部分表示副边绕组(S),由四层绕组并联而成,绕组都为单匝结构,其电流方向与原边侧相反,为逆时针方向。寄生电容的计算分为两种情况:第一种情况是相邻两层绕组位于同侧,都是原边侧绕组,此时二者电流方向相同;第二种情况是相邻两层绕组分别位于两侧,一层是原边绕组,另一层是副边绕组,此时二者电流方向相反。现分别计算当原边侧绕组分别为单匝和多匝时,两种情况各自寄生电容所包含的能量。The size of the capacitance is closely related to the way the windings of the planar transformer are distributed on the PCB. As shown in Fig. 2, the winding structure of the PCB-type planar transformer can be divided into a simple structure (Fig. 2a), a sandwich structure (Fig. 2b), and a staggered structure (Fig. 2c). Taking the eight-layer PCB winding as an example, the solid part represents the primary winding (P), which is formed by connecting four layers of windings in series. The windings are either single-turn or multi-turn, assuming that the current direction is clockwise; the hollow part Indicates the secondary winding (S), which is composed of four layers of windings in parallel. The windings are all single-turn structures, and the current direction is opposite to the primary side, which is counterclockwise. The calculation of parasitic capacitance is divided into two cases: the first case is that two adjacent layers of windings are located on the same side, both of which are primary side windings, and the current directions of the two are the same; the second case is that the two adjacent layers of windings are respectively On both sides, one layer is the primary winding, the other is the secondary winding, and the current directions of the two are opposite. Now calculate the energy contained in the respective parasitic capacitances of the two cases when the primary side windings are single-turn and multi-turn respectively.

(一)单层绕组电势计算(1) Calculation of single-layer winding potential

1.单层单匝原边侧绕组电势表示1. Single-layer single-turn primary side winding potential representation

如图3所示单匝原边侧绕组,假设电流流入点电压为V1P,电流流出点电压为V2P。不难发现,绕组上电压是随电流流入点的距离下降,并且电流按顺时针方向流动。采用图3所示极坐标系,假设绕组内径为r,外径为R。取圆环上的一段圆弧作为微元dθ,其位置极坐标的角度参数为θ,假设从流入点到流出点的电压降在线圈上均匀分布,则该段微元圆弧上的电压为:As shown in Figure 3, the single-turn primary side winding is assumed to be V 1P at the current inflow point and V 2P at the current outflow point. It is not difficult to find that the voltage on the winding decreases with the distance from the point where the current flows, and the current flows in a clockwise direction. Using the polar coordinate system shown in Figure 3, it is assumed that the inner diameter of the winding is r and the outer diameter is R. Take an arc on the ring as the micro-element dθ, and the angle parameter of its position polar coordinate is θ. Assuming that the voltage drop from the inflow point to the outflow point is evenly distributed on the coil, the voltage on this micro-element arc is :

Figure GDA0002562175680000071
Figure GDA0002562175680000071

2.单层单匝副边侧绕组电势表示2. Single-layer single-turn secondary winding potential representation

如图4所示单匝副边侧绕组,由于原边电流和副边电流流入位置互为镜像且电流流动方向相反,则副边侧绕组上某段微元圆弧上的电压为:As shown in Figure 4, for the single-turn secondary side winding, since the inflow positions of the primary side current and the secondary side current are mirror images of each other and the current flow directions are opposite, the voltage on a certain segment of the micro-element arc on the secondary side winding is:

Figure GDA0002562175680000072
Figure GDA0002562175680000072

3.单层多匝原边侧绕组电势表示3. Single-layer multi-turn primary side winding potential representation

当原边侧绕组为多匝情况时,与原边单匝绕组不同,线圈本身是一段螺旋线,每匝螺旋线之间也会有寄生电容存在,但平面变压器各层绕组的厚度小到可以忽略螺旋线间的寄生电容,应用阿基米德螺旋方程进行拟合绕组形状,方程表示为:When the primary side winding is multi-turn, different from the primary side single-turn winding, the coil itself is a helix, and there will also be parasitic capacitance between each turn of the helix, but the thickness of each layer of the planar transformer is small enough to Ignoring the parasitic capacitance between the spirals, the Archimedes spiral equation is used to fit the winding shape, and the equation is expressed as:

r*=h·θx (3)r*=h·θ x (3)

其中,r*表示极径,h是常数表示螺线比。Among them, r* represents the polar diameter, and h is a constant representing the helical ratio.

如图5所示,假设电流流入点电压为V1PM,电流流出点电压为V2PM。不难发现,螺旋线上电压是随电流流入点的距离线性下降。采用图中所示的极坐标系,取多匝线圈上的一段长度作为微元,其长度为dL,位置极坐标的角度参数为θx,表示该微元沿螺旋线到极心o绕过的角度;θ1表示从电流流入点沿螺旋线到极心o绕过的角度;θ2表示线圈从电流流出点沿螺旋线到极心o绕过的角度。由此,该段微元长度上的电压为:As shown in FIG. 5 , it is assumed that the current inflow point voltage is V 1PM , and the current outflow point voltage is V 2PM . It is not difficult to find that the voltage on the helix decreases linearly with the distance from the point where the current flows. Using the polar coordinate system shown in the figure, take a length of a multi-turn coil as a micro-element, its length is dL, and the angle parameter of the position polar coordinate is θx, indicating that the micro-element bypasses along the spiral line to the polar center o Angle; θ1 represents the angle from the current inflow point along the spiral to the pole center o ; θ2 represents the coil from the current outflow point along the spiral to the pole center o around the angle. Therefore, the voltage on the length of the micro-element is:

Figure GDA0002562175680000081
Figure GDA0002562175680000081

A表示从电流流入点到极心的直线距离,θ1表示从电流流入点沿螺旋线到极心绕过的角度,大小为:A represents the straight-line distance from the current inflow point to the pole center, θ 1 represents the angle from the current inflow point along the spiral line to the pole center, and the magnitude is:

Figure GDA0002562175680000082
Figure GDA0002562175680000082

L表示电流流入点到电流流出点的长度,大小为:L represents the length from the current inflow point to the current outflow point, and its size is:

Figure GDA0002562175680000083
Figure GDA0002562175680000083

(r*)'表示对r*求一阶导数,B表示从电流流出点到极心的直线距离,θ2表示从电流流出点沿螺旋线到极心绕过的角度,大小为:(r*)' represents the first derivative with respect to r*, B represents the straight-line distance from the current outflow point to the pole center, θ 2 represents the angle from the current outflow point along the spiral line to the pole center, the size is:

Figure GDA0002562175680000084
Figure GDA0002562175680000084

(二)相邻两层绕组电容能量计算(2) Calculation of capacitance energy of adjacent two-layer windings

1.相邻两层单匝原边绕组与单匝原边绕组电容能量计算1. Calculation of capacitance energy between two adjacent layers of single-turn primary winding and single-turn primary winding

此时,相邻两层单匝绕组处于第一种情况,即相邻两层绕组都是原边绕组,此时二者电流方向相同。如图6所示,上下相邻两层PCB绕组,假设上层绕组记做绕组1,下层绕组记做绕组2。a、c端分别是电流流入端,b、d端分别是电流流出端。绕组1中,a端电压为V1P,b端电压为V2P,V1P>V2P,电流按顺时针方向流动;绕组2中,c端电压为V3P,d端电压为V4P,V3P>V4P,电流也按顺时针方向流动。R为圆环外径,r为圆环内径,ε为板间介电常数,d为两层绕组之间的直线距离。电容微元可以表示为,At this time, the two adjacent layers of single-turn windings are in the first situation, that is, the two adjacent layers of windings are both primary windings, and the current directions of the two are the same. As shown in Figure 6, there are two adjacent layers of PCB windings up and down, assuming that the upper layer winding is recorded as winding 1, and the lower layer winding is recorded as winding 2. The a and c terminals are the current inflow terminals respectively, and the b and d terminals are the current outflow terminals respectively. In winding 1, the voltage of terminal a is V 1P , the voltage of terminal b is V 2P , V 1P > V 2P , and the current flows clockwise; in winding 2, the voltage of terminal c is V 3P , the voltage of terminal d is V 4P , V 3P > V 4P , the current also flows clockwise. R is the outer diameter of the ring, r is the inner diameter of the ring, ε is the dielectric constant between the plates, and d is the straight-line distance between the two layers of windings. The capacitance element can be expressed as,

Figure GDA0002562175680000085
Figure GDA0002562175680000085

电容C与能量W的关系表示为,The relationship between capacitance C and energy W is expressed as,

Figure GDA0002562175680000086
Figure GDA0002562175680000086

U1,U2分别表示电容上下极板的电势大小。U 1 and U 2 respectively represent the potential of the upper and lower plates of the capacitor.

由式(1)、(8)、(9),相邻两层单匝原边绕组与单匝原边绕组电容能量表示为,By formulas (1), (8), (9), the capacitance energy of two adjacent layers of single-turn primary winding and single-turn primary winding is expressed as,

Figure GDA0002562175680000087
Figure GDA0002562175680000087

2.相邻两层单匝原边绕组与单匝副边绕组电容能量计算2. Calculation of capacitance energy between two adjacent layers of single-turn primary winding and single-turn secondary winding

此时,相邻两层单匝绕组处于第二种情况,即相邻两层绕组一层是原边绕组,另一层是副边绕组,此时二者电流方向相反,如图7所示。V1P和V1S分别表示单匝原边侧和副边侧绕组电流流入点电压,V2P和V2S分别表示单匝原边侧和副边侧绕组电流流出点电压。由式(2)、(8)、(9),相邻两层单匝原边绕组与单匝副边绕组电容能量表示为:At this time, the two adjacent layers of single-turn windings are in the second situation, that is, one layer of the adjacent two layers of windings is the primary winding, and the other layer is the secondary winding. At this time, the current directions of the two are opposite, as shown in Figure 7 . V 1P and V 1S represent the current inflow point voltages of the primary and secondary windings of a single turn, respectively, and V 2P and V 2S represent the current outflow point voltages of the primary and secondary windings of a single turn, respectively. By formulas (2), (8), (9), the capacitance energy of two adjacent layers of single-turn primary winding and single-turn secondary winding is expressed as:

Figure GDA0002562175680000091
Figure GDA0002562175680000091

3.相邻两层多匝原边绕组与多匝原边绕组电容能量计算3. Calculation of capacitance energy between adjacent two-layer multi-turn primary windings and multi-turn primary windings

电容微元可以表示为:The capacitance element can be expressed as:

Figure GDA0002562175680000092
Figure GDA0002562175680000092

w表示多匝线圈绕组每匝的宽度,如果相邻两层多匝绕组处于第一种情况,如图8所示,只需对长度积分即可,此时,由式(1)、(9)、(12),相邻两层多匝原边绕组与多匝原边绕组电容能量表示为:w represents the width of each turn of the multi-turn coil winding. If the adjacent two-layer multi-turn windings are in the first case, as shown in Figure 8, it is only necessary to integrate the length. At this time, by formulas (1) and (9) ), (12), the capacitance energy of two adjacent layers of multi-turn primary winding and multi-turn primary winding is expressed as:

Figure GDA0002562175680000093
Figure GDA0002562175680000093

其中,n表示单层多匝线圈总匝数(匝数从电压流入端开始计算,每转过2π计一匝,不足一匝按一匝计算),i表示第i匝。Among them, n represents the total number of turns of the single-layer multi-turn coil (the number of turns is calculated from the inflow end of the voltage, one turn is counted for every 2π revolution, and the less than one turn is counted as one turn), and i is the i-th turn.

4.相邻两层多匝原边绕组与单匝副边绕组电容能量计算4. Capacitance energy calculation of adjacent two-layer multi-turn primary winding and single-turn secondary winding

如果相邻两层绕组处于第二种情况,且原边绕组为多匝,副边绕组为单匝,如图9所示。此时,由式(2)、(9)、(12),相邻两层绕组能量表示为:If two adjacent layers of windings are in the second case, and the primary winding is multi-turn, the secondary winding is single-turn, as shown in Figure 9. At this time, according to equations (2), (9) and (12), the energy of two adjacent layers of windings is expressed as:

Figure GDA0002562175680000094
Figure GDA0002562175680000094

(三)等效寄生电容计算(3) Calculation of equivalent parasitic capacitance

以八层PCB绕组为例,C12,C23。。。C78表示相邻两层绕组间的寄生电容,W12,W23...W78分别表示C12,C23。。。C78的能量,根据PCB型平面变压器相邻绕组情况,利用式(10)、(11)、(13)、(14),计算所有相邻两层绕组之间电容能量之和:Take the eight-layer PCB winding as an example, C 12 , C 23 . . . C 78 represents the parasitic capacitance between two adjacent layers of windings, W 12 , W 23 . . . W 78 represent C 12 , C 23 , respectively. . . The energy of C 78 , according to the situation of the adjacent windings of the PCB-type planar transformer, use the formulas (10), (11), (13), (14) to calculate the sum of the capacitance energy between all the adjacent two-layer windings:

Wps=W12+W23+W34+W45+W56+W67+W78 (15)W ps = W 12 +W 23 +W 34 +W 45 +W 56 +W 67 +W 78 (15)

原副边总压降分别为Vp与Vs,原边侧每层上的总压降相同,即每层原边绕组输入电压和输出电压能够分别用Vp表示,而副边侧采用并联结构,每层压降都为Vs,用E表示项

Figure GDA0002562175680000101
的系数和、F表示项Vp·Vs的系数和、G表示项Vs 2的系数和,将(15)整理为:The total voltage drops on the primary and secondary sides are respectively V p and V s . The total voltage drop on each layer on the primary side is the same, that is, the input voltage and output voltage of the primary winding of each layer can be represented by V p respectively, while the secondary side adopts a parallel connection. structure, each pressure drop is Vs , term E
Figure GDA0002562175680000101
, F represents the coefficient sum of the term V p ·V s , G represents the coefficient sum of the term V s 2 , and (15) is organized as:

Figure GDA0002562175680000102
Figure GDA0002562175680000102

PCB绕组的寄生电容所包含的总能量,等于三个等效电容C1,C2,C3所包含的能量之和,等效电容C1,C2,C3三个电容中存储的能量计算得,The total energy contained in the parasitic capacitance of the PCB winding is equal to the sum of the energy contained in the three equivalent capacitances C 1 , C 2 , and C 3 , and the energy stored in the three equivalent capacitances C 1 , C 2 , and C 3 calculated,

Figure GDA0002562175680000103
Figure GDA0002562175680000103

由于Wps=W1+W2+W3,对比式(16)、(17),得到:Since W ps =W 1 +W 2 +W 3 , comparing formulas (16) and (17), we get:

Figure GDA0002562175680000104
Figure GDA0002562175680000104

由(18)计算得到三个等效电容C1,C2,C3的电容值。由此得平面变压器的等效模型中寄生电容的具体数值。The capacitance values of the three equivalent capacitances C 1 , C 2 , and C 3 are calculated from (18). From this, the specific value of the parasitic capacitance in the equivalent model of the planar transformer is obtained.

本发明计算结果具有准确性,能够用来计算平面变压器PCB绕组的寄生电容,进而可用于应用于平面变压器寄生参数分析以及电磁兼容领域中EMI传导模型的建立。The calculation result of the invention is accurate, can be used to calculate the parasitic capacitance of the PCB winding of the planar transformer, and can be applied to the parasitic parameter analysis of the planar transformer and the establishment of the EMI conduction model in the field of electromagnetic compatibility.

本发明的一种平面变压器PCB绕组寄生电容计算方法,经过实际应用的结果表明,实现了本发明目的和达到了所述的效果。The practical application of the method for calculating the parasitic capacitance of the PCB winding of the planar transformer of the present invention shows that the purpose of the present invention is achieved and the stated effect is achieved.

本发明的特定实施例已对本发明的内容作出了详尽的说明,但不局限本实施例,本领域技术人员根据本发明的启示所做的任何显而易见的改动,都属于本发明权利保护的范围。The specific embodiment of the present invention has made a detailed description to the content of the present invention, but is not limited to this embodiment, and any obvious changes made by those skilled in the art according to the inspiration of the present invention belong to the scope of protection of the present invention.

Claims (1)

1.一种平面变压器PCB绕组寄生电容等效计算方法,所述平面变压器包括平面磁芯、PCB绕组和绝缘层,PCB绕组为多层结构,每一层上设置一个绕组,原边绕组与副边绕组设置在不同层上,原边绕组采用单匝或多匝其中之一,副边绕组采用单匝圆环形,多匝采用螺旋形,不同层上的原边绕组以串联方式连接,不同层上的副边绕组以并联方式连接,在相邻两层同为原边绕组及相邻两层分别为原边绕组和副边绕组的情况下,此时的相邻两层之间存在不可忽略的寄生电容;1. An equivalent calculation method for the parasitic capacitance of a PCB winding of a planar transformer, the planar transformer includes a planar magnetic core, a PCB winding and an insulating layer, the PCB winding is a multi-layer structure, and each layer is provided with a winding, the primary winding and the secondary winding; The side windings are arranged on different layers, the primary winding is one of single-turn or multi-turn, the secondary winding is a single-turn circular ring, and the multi-turn is spiral. The primary windings on different layers are connected in series, different The secondary windings on the layers are connected in parallel. When the two adjacent layers are both primary windings and the adjacent two layers are primary windings and secondary windings respectively, there is an inability between the two adjacent layers at this time. Negligible parasitic capacitance; 其特征在于:通过对平面变压器PCB绕组的建模和分析,模拟PCB绕组寄生电容的分布情况,通过计算存在寄生电容的各相邻两层之间寄生电容存储能量的大小并进行叠加,利用能量和寄生电容之间的关系以及能量守恒定律,对PCB绕组整体的寄生电容进行计算,然后将其等效为三个部分的电容,即原边绕组同名端与副边绕组同名端之间的电容C1、原边绕组同名端与副边绕组异名端之间的电容C2以及原边绕组异名端与副边绕组同名端之间的电容C3;包括以下步骤:It is characterized in that: through the modeling and analysis of the PCB winding of the planar transformer, the distribution of the parasitic capacitance of the PCB winding is simulated, and the energy stored in the parasitic capacitance between the two adjacent layers where the parasitic capacitance exists is calculated and superimposed, and the energy is utilized. The relationship between the parasitic capacitance and the energy conservation law, the parasitic capacitance of the PCB winding as a whole is calculated, and then it is equivalent to the capacitance of three parts, that is, the capacitance between the same-named end of the primary winding and the same-named end of the secondary winding C1 . Capacitor C2 between the same - named end of the primary winding and the synonymous end of the secondary winding, and capacitance C3 between the synonymous end of the primary winding and the same - named end of the secondary winding; including the following steps: (1)单层绕组电势计算(1) Calculation of single-layer winding potential 1)单层单匝原边侧绕组电势表示1) Single-layer single-turn primary side winding potential representation 假设原边绕组电流按顺时针方向流动,且绕组电压沿着电流方向均匀下降,以极心到电流流入点的射线为极径建立极坐标系,取绕组上的一段圆弧作为微元dθ,微元dθ位置极坐标的角度参数为θ,该微元电压表示为:Assuming that the primary winding current flows in a clockwise direction, and the winding voltage drops uniformly along the current direction, a polar coordinate system is established with the ray from the pole center to the current inflow point as the pole diameter, and a segment of the arc on the winding is taken as the micro-element dθ, The angle parameter of the polar coordinate of the position of the micro-element dθ is θ, and the voltage of the micro-element is expressed as:
Figure FDA0002562175670000011
Figure FDA0002562175670000011
V1P是单匝原边侧绕组电流流入点电压,V2P是单匝原边侧绕组电流流出点电压;V 1P is the current inflow point voltage of single-turn primary side winding, V 2P is the current outflow point voltage of single-turn primary side winding; 2)单层单匝副边侧绕组电势表示2) Representation of single-layer single-turn secondary winding potential 原边电流与副边电流进入位置互为镜像且电流流动方向相反,副边侧绕组上微元dθ电压表示为:The primary side current and the secondary side current entry position are mirror images of each other and the current flows in opposite directions. The micro-element dθ voltage on the secondary side winding is expressed as:
Figure FDA0002562175670000012
Figure FDA0002562175670000012
V1S是单匝副边侧绕组电流流入点电压,V2S是单匝副边侧绕组电流流出点电压;V 1S is the current inflow point voltage of the single-turn secondary side winding, V 2S is the current outflow point voltage of the single-turn secondary side winding; 3)单层多匝原边侧绕组电势表示3) Single-layer multi-turn primary side winding potential representation 当原边侧绕组为多匝情况时,与原边单匝绕组不同,线圈本身是一段螺旋线,每匝螺旋线之间也会有寄生电容存在,但平面变压器各层绕组的厚度小到能够忽略螺旋线间的寄生电容,应用阿基米德螺旋方程进行拟合绕组形状,阿基米德螺旋方程表示为:When the primary side winding is multi-turn, different from the primary side single-turn winding, the coil itself is a helix, and there will also be parasitic capacitance between each turn of the helix, but the thickness of each layer of the planar transformer is small enough to Ignoring the parasitic capacitance between the spirals, the Archimedes spiral equation is used to fit the winding shape. The Archimedes spiral equation is expressed as: r*=h·θx (3)r*=h·θ x (3) r*表示极径,h是常数表示螺线比,r* represents the polar diameter, h is a constant representing the helical ratio, 以极心到电流流入点的射线为极径建立极坐标系,取多匝线圈上的一段长度dL作为微元,θx表示微元dL沿螺旋线到极心绕过的角度参数;该微元电压表示为:The polar coordinate system is established with the ray from the pole center to the current inflow point as the pole diameter, and a length dL on the multi-turn coil is taken as the micro-element, and θ x represents the angle parameter of the micro-element dL along the spiral line to the pole center; the micro-element The element voltage is expressed as:
Figure FDA0002562175670000021
Figure FDA0002562175670000021
A表示从电流流入点到极心的直线距离,θ1表示从电流流入点沿螺旋线到极心绕过的角度,大小为:A represents the straight-line distance from the current inflow point to the pole center, θ 1 represents the angle from the current inflow point along the spiral line to the pole center, and the magnitude is:
Figure FDA0002562175670000022
Figure FDA0002562175670000022
L表示电流流入点到电流流出点的长度,大小为:L represents the length from the current inflow point to the current outflow point, and its size is:
Figure FDA0002562175670000023
Figure FDA0002562175670000023
(r*)'表示对r*求一阶导数,B表示从电流流出点到极心的直线距离,θ2表示从电流流出点沿螺旋线到极心绕过的角度,大小为:(r*)' represents the first derivative with respect to r*, B represents the straight-line distance from the current outflow point to the pole center, θ 2 represents the angle from the current outflow point along the spiral line to the pole center, the size is:
Figure FDA0002562175670000024
Figure FDA0002562175670000024
(2)相邻两层绕组电容能量计算(2) Calculation of capacitance energy of adjacent two-layer windings 1)相邻两层单匝原边绕组与单匝原边绕组电容能量计算1) Calculation of capacitance energy between two adjacent layers of single-turn primary winding and single-turn primary winding 相邻两层单匝绕组都是原边绕组,此时二者电流方向相同,电容微元表示为:The two adjacent layers of single-turn windings are both primary windings. At this time, the current direction of the two layers is the same, and the capacitance element is expressed as:
Figure FDA0002562175670000025
Figure FDA0002562175670000025
R为绕组外径,r为绕组内径,ε为板间介电常数,d为两层绕组之间的垂直距离;R is the outer diameter of the winding, r is the inner diameter of the winding, ε is the dielectric constant between the plates, and d is the vertical distance between the two layers of windings; 电容C与能量W的关系表示为:The relationship between capacitance C and energy W is expressed as:
Figure FDA0002562175670000026
Figure FDA0002562175670000026
U1,U2分别表示电容上下极板的电势大小;U 1 , U 2 respectively represent the electric potential of the upper and lower plates of the capacitor; 由式(1)、(8)、(9),相邻两层单匝原边绕组与单匝原边绕组电容能量表示为
Figure FDA0002562175670000031
From equations (1), (8) and (9), the capacitance energy of two adjacent layers of single-turn primary winding and single-turn primary winding is expressed as
Figure FDA0002562175670000031
2)相邻两层单匝原边绕组与单匝副边绕组电容能量计算2) Capacitance energy calculation of two adjacent layers of single-turn primary winding and single-turn secondary winding 相邻两层绕组一层是单匝原边绕组,另一层是单匝副边绕组,此时二者电流方向相反,由式(2)、(8)、(9),相邻两层单匝原边绕组与单匝副边绕组电容能量表示为:Two adjacent layers of windings: One layer is a single-turn primary winding, and the other layer is a single-turn secondary winding. At this time, the current directions of the two are opposite. The single-turn primary winding and single-turn secondary winding capacitance energy is expressed as:
Figure FDA0002562175670000032
Figure FDA0002562175670000032
3)相邻两层多匝原边绕组与多匝原边绕组电容能量计算3) Calculation of capacitance energy between two adjacent layers of multi-turn primary winding and multi-turn primary winding 相邻两层多匝绕组都是原边绕组,此时二者电流方向相同,电容微元表示为:The two adjacent layers of multi-turn windings are all primary windings. At this time, the two current directions are the same, and the capacitance element is expressed as:
Figure FDA0002562175670000033
Figure FDA0002562175670000033
w表示多匝线圈绕组每匝的宽度,w represents the width of each turn of the multi-turn coil winding, 由式(1)、(9)、(12),相邻两层多匝原边绕组与多匝原边绕组电容能量表示为:From equations (1), (9) and (12), the capacitance energy of two adjacent layers of multi-turn primary windings and multi-turn primary windings is expressed as:
Figure FDA0002562175670000034
Figure FDA0002562175670000034
其中,n表示单层多匝线圈总匝数,匝数从电流流入点开始计算,每转过2π计一匝,不足一匝按一匝计算,i表示第i匝;Among them, n represents the total number of turns of the single-layer multi-turn coil, the number of turns is calculated from the current inflow point, one turn is counted for every 2π revolution, and less than one turn is counted as one turn, and i represents the i-th turn; 4)相邻两层多匝原边绕组与单匝副边绕组电容能量计算4) Calculation of capacitance energy of adjacent two-layer multi-turn primary winding and single-turn secondary winding 相邻两层绕组一层是多匝原边绕组,另一层是单匝副边绕组,此时二者电流方向相反,由式(2)、(9)、(12),相邻两层多匝原边绕组与单匝副边绕组电容能量表示为:Two adjacent layers of windings: One layer is a multi-turn primary winding, and the other is a single-turn secondary winding. At this time, the current directions of the two are opposite. The capacitance energy of multi-turn primary winding and single-turn secondary winding is expressed as:
Figure FDA0002562175670000035
Figure FDA0002562175670000035
(3)等效寄生电容计算(3) Calculation of equivalent parasitic capacitance 设Ck,k+1表示第k层与第k+1层相邻两绕组间的寄生电容,Wk,k+1表示Ck,k+1的电容能量,根据PCB型平面变压器相邻绕组情况,利用式(10)、(11)、(13)、(14),计算所有相邻两层绕组之间电容能量之和WpsLet C k,k+1 represent the parasitic capacitance between the two adjacent windings of the kth layer and the k+1th layer, and W k,k+1 represent the capacitance energy of C k,k+1 . According to the adjacent PCB-type planar transformer For the winding condition, use equations (10), (11), (13), (14) to calculate the sum of capacitance energy W ps between all adjacent two-layer windings: Wps=W12+W23...+Wk,k+1+...(15)W ps =W 12 +W 23 ...+W k,k+1 +...(15) 原副边总压降分别为Vp与Vs,原边侧每层上的总压降相同,即每层原边绕组输入电压和输出电压能够分别用Vp表示,而副边侧采用并联结构,每层压降都为Vs,用E表示项
Figure FDA0002562175670000041
的系数和、F表示项Vp·Vs的系数和、G表示项Vs 2的系数和,将(15)整理为:
The total voltage drops on the primary and secondary sides are respectively V p and V s . The total voltage drop on each layer on the primary side is the same, that is, the input voltage and output voltage of the primary winding of each layer can be represented by V p respectively, while the secondary side adopts a parallel connection. structure, each pressure drop is Vs , term E
Figure FDA0002562175670000041
, F represents the coefficient sum of the term V p ·V s , G represents the coefficient sum of the term V s 2 , and (15) is organized as:
Figure FDA0002562175670000042
Figure FDA0002562175670000042
PCB绕组的寄生电容所包含的总能量,等于三个等效电容C1,C2,C3所包含的能量之和,等效电容C1,C2,C3三个电容中存储的能量计算得,The total energy contained in the parasitic capacitance of the PCB winding is equal to the sum of the energy contained in the three equivalent capacitances C 1 , C 2 , and C 3 , and the energy stored in the three equivalent capacitances C 1 , C 2 , and C 3 calculated,
Figure FDA0002562175670000043
Figure FDA0002562175670000043
由于Wps=W1+W2+W3,对比式(16)、(17),得到:Since W ps =W 1 +W 2 +W 3 , comparing formulas (16) and (17), we get:
Figure FDA0002562175670000044
Figure FDA0002562175670000044
由(18)计算得到三个等效电容C1,C2,C3的电容值。The capacitance values of the three equivalent capacitances C 1 , C 2 , and C 3 are calculated from (18).
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