TWI898767B - Design method for the layout of output capacitors in a switch-mode power supply with constant current output - Google Patents
Design method for the layout of output capacitors in a switch-mode power supply with constant current outputInfo
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Abstract
Description
本發明係有關於一種應用於切換式電源定電流輸出的輸出電容佈局設計方法,尤其是指一種於電路迴路中能改善電荷移動的速率,令電荷移動速率不受頻率變動影響,且減少在定電流輸出時的雜訊,而在其整體施行使用上更增實用功效特性者。This invention relates to a design method for output capacitor layouts used in switching power supplies with constant current output. Specifically, the design improves the charge transfer rate within the circuit loop, making it independent of frequency variations and reducing noise during constant current output, thereby enhancing overall practicality and performance.
按,在傳統的切換式電源在輸出濾波設計上一般都會採用到耦合電容進行濾波,在常見的做法中主要都會依據電容值的大小進行排列,依據輸入及輸出的電流方向並由容值由大至小的排列,一般都會採用緊密排列的方式來來排列電容,而採此方式雖可達濾波效果但無法有效過濾路徑上所產生的諧振頻率。以目前需採定電流輸出的應用大多以LED或馬達驅動有關,而此兩種應用都需要穩定的電壓及電流,所以在雜訊的抑制上就必須要符合應用所規範的範圍內才可使LED或馬達穩定的工作,在以定電流輸出的切換式電源架構上輸出端的耦合電容會因輸出路徑上所帶來的電流所影響,而電流的本質是由電荷移動所形成的,而其電流值之大小與移動之電荷多寡及速率均有關係,根據I=Q/t[Q=電荷,t=時間]可以得知在輸出路徑上的頻率[t=1/f]變動會影響到電荷移動的速率,由於輸出迴路中頻率的不穩定使輸出端耦合電容瞬間飽和,因頻率變動的關係之下也使耦合電容的電容量產生變化,輸出端的電流訊號就會開始產生雜訊。Traditional switching power supplies typically utilize coupled capacitors for output filtering. Common practice involves arranging capacitors based on their value, from largest to smallest, according to the direction of input and output current. This approach typically employs a dense arrangement of capacitors. While this approach achieves filtering effects, it cannot effectively filter out resonant frequencies generated along the path. Currently, most applications that require constant current output are related to LED or motor driving. Both applications require stable voltage and current. Therefore, noise suppression must be within the specified range of the application to ensure stable operation of the LED or motor. In a switching power supply architecture with constant current output, the coupling capacitor at the output end will be affected by the current brought by the output path. The essence of current is the movement of charge, and The magnitude of the current is related to the amount and rate of charge movement. According to the equation I = Q/t [Q = charge, t = time], frequency fluctuations in the output path [t = 1/f] affect the rate of charge movement. Frequency instability in the output loop causes the output coupling capacitor to become instantaneously saturated. This frequency fluctuation also causes the coupling capacitor's capacitance to vary, causing noise in the output current signal.
輸出端迴路中頻率不穩定使電荷流動速率產生變化與佈局走線的寬度、長度也有相當大的關係,會因電路板[PCB]中走線上所產生之寄生電感所影響,使雜訊無法完全被電容所抑制;當走線長度越長時容易產生出較高的頻率並且在這其中也需放置大量的耦合電容進行濾波,而放置過多的耦合電容則會使迴路上的頻率變高雜訊也會增加。當迴路上的頻率[迴路頻率與電源開關頻率有關]越高時,就會使輸出電容的體積縮小,而當輸出電流越大時,走線的寬度也會隨之變寬,寄生參數也就會跟著改變,因此在輸出端的濾波設計上就會變得更加困難。Frequency instability in the output loop causes changes in charge flow rate, which is closely related to the width and length of the layout traces. This parasitic inductance generated by the PCB traces can affect noise, preventing it from being completely suppressed by capacitors. Longer traces tend to generate higher frequencies, necessitating the placement of a larger number of coupling capacitors for filtering. However, placing too many coupling capacitors increases the frequency and noise in the loop. When the loop frequency (loop frequency is related to the power switching frequency) increases, the output capacitor size will be reduced. When the output current increases, the trace width will also increase, and the parasitic parameters will also change accordingly, making the output filtering design more difficult.
請參閱第二十四圖現有電路板產生寄生電感狀態示意圖所示,一般在整體電路系統(2)上電源轉換迴路會被稱為VRM[Voltage Regulator Module,電壓調節模組](21),從VRM(21)輸出電壓供給至負載(22)[如:LED或馬達]之間是透過電路板(23)上的走線[trace](231)作為導電路徑,該走線(231)通常是一條細銅線、銅箔或其他導電材料所製作而成,而在該走線(231)中帶有阻抗及頻率,因而產生出寄生電感(232),使得即會加入電容(24)來進行濾波;一般該電容(24)的參數及選用應用於迴路濾波中可有效抑制住該電路系統(2)中其他被動元件所產生出之雜訊,但在迴路上會因該電路板(23)之該走線(231)所帶有的頻率變動而產生不一的雜訊,並且造成迴路中產生高頻雜訊,即使加入該電容(24)也無法有效抑制。Please refer to the schematic diagram of the parasitic inductance generated by the existing circuit board in Figure 24. Generally, the power conversion circuit on the overall circuit system (2) is called VRM [Voltage Regulator Module, voltage regulation module] (21). The output voltage from the VRM (21) is supplied to the load (22) [such as LED or motor] through the trace [trace] (231) on the circuit board (23) as a conductive path. The trace (231) is usually made of a thin copper wire, copper foil or other conductive materials. The trace (231) has impedance and frequency, thereby generating parasitic inductance (2 32), so that the capacitor (24) is added to perform filtering; generally, the parameters and selection of the capacitor (24) used in the loop filtering can effectively suppress the noise generated by other passive components in the circuit system (2), but different noises will be generated in the loop due to the frequency variation of the trace (231) of the circuit board (23), and high-frequency noise will be generated in the loop, which cannot be effectively suppressed even if the capacitor (24) is added.
當該電路系統(2)之該VRM(21)與該負載(22)之間的該走線(231)越長時所帶來的寄生電感(232)、阻抗就會相對的大,反之當該走線(231)越短時所產生的寄生電感(232)就會相對的少,而不管該走線(231)或長或短,其都會產生共振現象;而要降低迴路中的共振現象就會先設立目標阻抗,迴路中目標阻抗的組成主要與迴路中所選用的電容特性有關,根據目標阻抗所選擇出的電容參數導入至該VRM(21)與該負載(22)之間的該走線(231)中,基本上可過濾掉絕大多數由被動元件所產生出的雜訊,剩下的雜訊則由電容(24)濾波與該電路板(23)平面所產生的噪聲[共振]所引起。When the line (231) between the VRM (21) and the load (22) of the circuit system (2) is longer, the parasitic inductance (232) and impedance will be relatively large. On the contrary, when the line (231) is shorter, the parasitic inductance (232) will be relatively small. Regardless of whether the line (231) is long or short, it will produce resonance. To reduce the resonance phenomenon in the loop, the target is first set. The target impedance in the loop is mainly related to the characteristics of the capacitor selected in the loop. The capacitor parameters selected according to the target impedance are introduced into the trace (231) between the VRM (21) and the load (22). Basically, most of the noise generated by the passive components can be filtered out. The remaining noise is caused by the noise (resonance) generated by the capacitor (24) filtering and the plane of the circuit board (23).
今,發明人有鑑於此,秉持多年該相關行業之豐富設計開發及實際製作經驗,針對現有之結構及缺失再予以研究改良,提供一種應用於切換式電源定電流輸出的輸出電容佈局設計方法,以期達到更佳實用價值性之目的者。With this in mind, the inventors, drawing on years of extensive design, development, and manufacturing experience in the relevant industry, have further researched and improved existing structures and shortcomings, providing a method for designing output capacitor layouts for constant-current output switching power supplies, aiming to achieve greater practical value.
本發明之主要目的在於提供一種應用於切換式電源定電流輸出的輸出電容佈局設計方法,其主要係於電路迴路中能改善電荷移動的速率,令電荷移動速率不受頻率變動影響,且減少在定電流輸出時的雜訊,而在其整體施行使用上更增實用功效特性者。The primary objective of this invention is to provide a method for designing an output capacitor layout for a constant-current switching power supply. This method improves the charge transfer rate within the circuit loop, making it independent of frequency variations and reducing noise during constant-current output. Overall, this method enhances practical performance.
本發明應用於切換式電源定電流輸出的輸出電容佈局設計方法之主要目的與功效,係由以下具體技術手段所達成:The primary purpose and effectiveness of the present invention's output capacitor layout design method for a switching power supply with a constant current output are achieved through the following specific technical means:
其主要係於電路迴路中,令電容在走線上以5mm之排列間距進行排列設計。This is mainly done by arranging capacitors on the traces in the circuit loop with a spacing of 5mm.
本發明應用於切換式電源定電流輸出的輸出電容佈局設計方法的較佳實施例,其中,該電路迴路中,輸出電流為1A、該走線寬度為1mm。The present invention is applied to a preferred embodiment of a method for designing an output capacitor layout for a switching power supply with a constant current output, wherein the output current in the circuit loop is 1A and the trace width is 1mm.
本發明應用於切換式電源定電流輸出的輸出電容佈局設計方法的較佳實施例,其中,該電路迴路中,輸出電流為5A、該走線寬度為5mm。The present invention is applied to a preferred embodiment of a method for designing an output capacitor layout for a switching power supply with a constant current output, wherein the output current in the circuit loop is 5A and the trace width is 5mm.
本發明應用於切換式電源定電流輸出的輸出電容佈局設計方法的較佳實施例,其中,該電路迴路中該走線係設置於電壓調節模組[Voltage Regulator Module,VRM]與負載之間。The present invention is applied to a preferred embodiment of a method for designing an output capacitor layout for a switching power supply with a constant current output, wherein the trace in the circuit loop is arranged between a voltage regulator module (VRM) and a load.
本發明應用於切換式電源定電流輸出的輸出電容佈局設計方法的較佳實施例,其中,該負載係為LED、馬達任一種。The present invention is applied to a preferred embodiment of a method for designing an output capacitor layout for a switching power supply with a constant current output, wherein the load is either an LED or a motor.
為令本發明所運用之技術內容、發明目的及其達成之功效有更完整且清楚的揭露,茲於下詳細說明之,並請一併參閱所揭之圖式及圖號:To provide a more complete and clear disclosure of the technical content, purpose of the invention, and the effects achieved by the present invention, the following is a detailed description thereof, and please refer to the accompanying drawings and figure numbers:
首先,請參閱第一圖本發明於走線中產生橫電波狀態示意圖及第二圖本發明於走線中產生橫電波之等效電路RL阻抗特性狀態示意圖所示,由於在電路迴路(1)中,因為帶有著一定的電壓,所以在走線(11)上產生出電場(12),而該電路迴路(1)中能量傳遞方向與磁場(13)相同且與該電場(12)垂直,當該走線(11)中的該電場(12)能量越大時,就會導致迴路中產生大小不一的共振,共振次數越多時就會使得輸出端訊號產生雜訊或訊號不穩定的現象,當共振頻率越大時可能會使走線產生阻抗並使輸出端產生壓降,此共振現象可採馬克斯威爾方程式求出,該走線(11)中所產生的橫電波(14)[Transverse Electric,TE Mode],其在波導中按橫截面內電磁場的幅度變化可寫成TE mn,其中m、n表示場強沿某座標維度的起伏次數。 First, please refer to the first figure of the invention, which shows the state of the transverse electromagnetic wave generated in the trace, and the second figure, which shows the state of the equivalent circuit RL impedance characteristic of the invention, as shown in FIG. Since there is a certain voltage in the circuit loop (1), an electric field (12) is generated on the trace (11), and the energy transfer direction in the circuit loop (1) is the same as the magnetic field (13) and is perpendicular to the electric field (12). When the The greater the energy of the electric field (12) in the trace (11), the more resonances of varying magnitudes will be generated in the loop. The more resonances occur, the more noise or signal instability will be generated in the output signal. When the resonance frequency is higher, the trace may generate impedance and a voltage drop may be generated at the output. This resonance phenomenon can be calculated using Maxwell's equations. The transverse electric wave (14) [Transverse Electric, TE Mode] generated in the trace (11) can be written as TE mn according to the amplitude change of the electromagnetic field in the cross section in the waveguide, where m and n represent the number of fluctuations in the field strength along a certain coordinate dimension.
在模擬實驗中採1mm及5mm的電容間距排列方式來進行共振模擬,並且逐一分析各間距排列方式應用於走線流經1A、5A銅箔寬度1mm及5mm中共振狀態:In the simulation experiment, 1mm and 5mm capacitor spacing arrangements were used for resonance simulation. The resonance state of each spacing arrangement when applied to the traces flowing through 1A and 5A copper foils with widths of 1mm and 5mm was analyzed one by one:
當電容間距:1mm、5mm,走線乘載電流及寬度:1A@1mm時,請再一併參閱第三圖本發明於電流1A、電容間距1mm進行諧振模式測試之波形圖[584KHz]、第四圖本發明於電流1A、電容間距1mm進行諧振模式測試之波形圖[731KHz]、第五圖本發明於電流1A、電容間距1mm進行諧振模式測試之波形圖[1.16MHz]、第六圖本發明於電流1A、電容間距1mm進行諧振模式測試之波形圖[2.74MHz]、第七圖本發明於電流1A、電容間距1mm進行諧振模式測試之波形圖[3.84GHz]所示,在共振模擬測試結果中,模擬軟體分別擷取出了五個共振頻率並且分別顯示出了共振位置,共振發生頻率分別發生在584KHz、731KHz、1.16MHz、2.74MHz、3.84GHz;一般來說,在迴路中的共振建議落在TE 01或是TE 10,從結果顯示產生出TE 01或是TE 10分別是584KHz、731KHz、1.16MHz、2.74MHz,在3.84GHz頻率時同時產生出兩個共振位置(TE 20),因這兩個共振點產生於高頻,所以在過濾高頻雜訊上效果不佳。 When the capacitor spacing is 1mm, 5mm, and the trace current and width is 1A@1mm, please also refer to the third figure, which is the waveform diagram of the resonance mode test at a current of 1A and a capacitor spacing of 1mm [584KHz], the fourth figure, which is the waveform diagram of the resonance mode test at a current of 1A and a capacitor spacing of 1mm [731KHz], the fifth figure, which is the waveform diagram of the resonance mode test at a current of 1A and a capacitor spacing of 1mm [1.16MHz], and the sixth figure, which is the waveform diagram of the resonance mode test at a current of 1A and a capacitor spacing of As shown in the waveform diagram of the resonance mode test at 1mm [2.74MHz], and the waveform diagram of the resonance mode test at 1A current and 1mm capacitor spacing [3.84GHz] of the present invention in the seventh figure, in the resonance simulation test results, the simulation software extracted five resonance frequencies and displayed the resonance positions respectively. The resonance frequencies occurred at 584KHz, 731KHz, 1.16MHz, 2.74MHz, and 3.84GHz respectively. Generally speaking, the resonance in the loop is recommended to fall on TE The results show that TE 01 or TE 10 are 584 kHz , 731 kHz, 1.16 MHz, and 2.74 MHz, respectively. At 3.84 GHz, two resonance positions (TE 20 ) are simultaneously generated. Because these two resonance points occur at high frequencies, they are not very effective in filtering high-frequency noise.
請再一併參閱第八圖本發明於電流1A、電容間距5mm進行諧振模式測試之波形圖[440KHz]、第九圖本發明於電流1A、電容間距5mm進行諧振模式測試之波形圖[558KHz]、第十圖本發明於電流1A、電容間距5mm進行諧振模式測試之波形圖[866KHz]、第十一圖本發明於電流1A、電容間距5mm進行諧振模式測試之波形圖[2.03MHz]、第十二圖本發明於電流1A、電容間距5mm進行諧振模式測試之波形圖[3.67GHz]所示,當電容間距改採5mm時可以發現到共振頻率明顯降低,而在高頻共振頻率上從原先的3.84GHz降低至3.67GHz並且共振點從原先的TE 20減少到TE 10,明顯有改善。 Please also refer to Figure 8, which is a waveform diagram of the resonance mode test at a current of 1A and a capacitor spacing of 5mm [440KHz], Figure 9, which is a waveform diagram of the resonance mode test at a current of 1A and a capacitor spacing of 5mm [558KHz], Figure 10, which is a waveform diagram of the resonance mode test at a current of 1A and a capacitor spacing of 5mm [866KHz], Figure 11, which is a waveform diagram of the resonance mode test at a current of 1A, As shown in the waveform diagram [2.03MHz] of the resonant mode test with a capacitor spacing of 5mm, and the waveform diagram [3.67GHz] of the resonant mode test with a current of 1A and a capacitor spacing of 5mm in Figure 12, when the capacitor spacing is changed to 5mm, the resonant frequency is significantly reduced. The high-frequency resonant frequency is reduced from the original 3.84GHz to 3.67GHz, and the resonance point is reduced from the original TE 20 to TE 10 , which is a clear improvement.
當電容間距:1mm、5mm,走線乘載電流及寬度:5A@5mm時,請再一併參閱第十三圖本發明於電流5A、電容間距1mm進行諧振模式測試之波形圖[661KHz]、第十四圖本發明於電流5A、電容間距1mm進行諧振模式測試之波形圖[784KHz]、第十五圖本發明於電流5A、電容間距1mm進行諧振模式測試之波形圖[1.2MHz]、第十六圖本發明於電流5A、電容間距1mm進行諧振模式測試之波形圖[2.98MHz]、第十七圖本發明於電流5A、電容間距1mm進行諧振模式測試之波形圖[2.96GHz]所示,因迴路需承受5A的電流,所以在走線寬度上改採5mm,而電容間距先以1mm來進行共振模擬;從模擬結果中分別產生出五個共振頻率,分別是:661KHz、784KHz、1.2MHz、2.98MHz、2.96GHz,在2.96GHz頻率時同時產生出兩個共振位置(TE 20),因這兩個共振點產生於高頻,所以在過濾高頻雜訊上效果不佳。 When the capacitor spacing is 1mm or 5mm, and the trace current and width are 5A@5mm, please also refer to Figure 13, which shows the waveform of the resonance mode test at 5A and 1mm capacitor spacing [661KHz], Figure 14, which shows the waveform of the resonance mode test at 5A and 1mm capacitor spacing [784KHz], Figure 15, which shows the waveform of the resonance mode test at 5A and 1mm capacitor spacing [1.2MHz], and Figure 16, which shows the waveform of the resonance mode test at 5A and 1mm capacitor spacing [1.2MHz]. The test waveform [2.98MHz] and Figure 17 show the waveform [2.96GHz] of the present invention tested in resonant mode with a current of 5A and a capacitor spacing of 1mm. Because the loop needs to withstand a current of 5A, the trace width is changed to 5mm, and the capacitor spacing is initially set at 1mm for resonance simulation. The simulation results generate five resonant frequencies: 661kHz, 784kHz, 1.2MHz, 2.98MHz, and 2.96GHz. At 2.96GHz, two resonance points (TE 20 ) are simultaneously generated. Because these two resonance points occur at high frequencies, they are not very effective in filtering high-frequency noise.
請再一併參閱第十八圖本發明於電流5A、電容間距5mm進行諧振模式測試之波形圖[628KHz]、第十九圖本發明於電流5A、電容間距5mm進行諧振模式測試之波形圖[970KHz]、第二十圖本發明於電流5A、電容間距5mm進行諧振模式測試之波形圖[2.4MHz]、第二十一圖本發明於電流5A、電容間距5mm進行諧振模式測試之波形圖[1.93GHz]所示,將電容間距改採用5mm的排列方式進行共振模擬,從模擬中可以發現頻率明顯降低,並且此次只產生出4個較大的共振頻率,而在高頻共振頻率中原先的2.96GHz降低至1.93GHz,並且也從原先的TE 20降低至TE 10,這也表示此間距的排列方式也適用於面積較大的走線濾波。 Please also refer to Figure 18, which shows the waveform of the present invention under the resonant mode test with a current of 5A and a capacitor spacing of 5mm [628KHz], Figure 19, which shows the waveform of the present invention under the resonant mode test with a current of 5A and a capacitor spacing of 5mm [970KHz], Figure 20, which shows the waveform of the present invention under the resonant mode test with a current of 5A and a capacitor spacing of 5mm [2.4MHz], and Figure 21. As shown in the waveform diagram [1.93GHz] of the resonance mode test conducted with a current of 5A and a capacitor spacing of 5mm, the present invention adopts a 5mm arrangement for the resonance simulation. The simulation shows a significant frequency reduction, with only four large resonant frequencies generated. The high-frequency resonant frequency decreases from 2.96GHz to 1.93GHz, and the TE is also reduced from 20 to 10. This also indicates that this spacing arrangement is also suitable for filtering traces with larger areas.
因此,根據上述模擬結果可以得知,請再一併參閱第二十二圖本發明之輸出電容佈局設計結構示意圖[輸出電流1A、走線寬度1mm]及第二十三圖本發明之輸出電容佈局設計結構示意圖[輸出電流5A、走線寬度5mm]所示,於電路迴路(1)中,在電壓調節模組[Voltage Regulator Module,VRM]與負載[如:LED或馬達]之間所設置的走線(11),令電容(15)在該走線(11)上以5mm之排列間距進行排列設計時,其濾波效果較佳,並且也可有效的減少高頻振盪的產生。Therefore, according to the above simulation results, it can be known that, please refer to the output capacitor layout design structure schematic diagram of the present invention in Figure 22 [output current 1A, trace width 1mm] and the output capacitor layout design structure schematic diagram of the present invention in Figure 23 [output current 5A, trace width 5mm]. As shown in the circuit loop (1), when the trace (11) is set between the voltage regulator module [Voltage Regulator Module, VRM] and the load [such as: LED or motor], the capacitor (15) is arranged on the trace (11) with an arrangement spacing of 5mm. The filtering effect is better and the generation of high-frequency oscillation can also be effectively reduced.
藉由以上所述,本發明之使用實施說明可知,本發明與現有技術手段相較之下,本發明主要係具有下列優點:From the above description of the use and implementation of the present invention, it can be seen that compared with the existing technical means, the present invention mainly has the following advantages:
1.本發明於電路迴路中能改善電荷移動的速率,令電荷移動速率不受頻率變動影響,而在其整體施行使用上更增實用功效特性者。1. The present invention can improve the rate of charge transfer in a circuit loop, making the charge transfer rate unaffected by frequency variations, and further enhances the practical performance characteristics of its overall implementation.
2.由於目前需採定電流輸出的應用大多以LED或馬達驅動有關,而此兩種應用都需要穩定的電壓及電流,所以在雜訊的抑制上就必須要符合應用所規範的範圍內才可使LED或馬達穩定的工作,使得本發明亦可減少在定電流輸出時的雜訊,以讓LED或馬達能穩定的進行工作。2. Currently, most applications requiring constant current output are related to LED or motor driving. Both applications require stable voltage and current. Therefore, noise suppression must comply with the application's specified range to ensure stable operation of the LED or motor. This invention can also reduce noise during constant current output, allowing the LED or motor to operate stably.
然而前述之實施例或圖式並非限定本發明之產品結構或使用方式,任何所屬技術領域中具有通常知識者之適當變化或修飾,皆應視為不脫離本發明之專利範疇。However, the aforementioned embodiments or drawings do not limit the product structure or usage of the present invention. Any appropriate changes or modifications by those skilled in the art should be considered as falling within the patent scope of the present invention.
綜上所述,本發明實施例確能達到所預期之使用功效,又其所揭露之具體構造,不僅未曾見諸於同類產品中,亦未曾公開於申請前,誠已完全符合專利法之規定與要求,爰依法提出發明專利之申請,懇請惠予審查,並賜准專利,則實感德便。In summary, the embodiments of this invention can indeed achieve the intended effects. Moreover, the specific structure disclosed therein is not only unprecedented in similar products, but has also not been disclosed prior to the filing of this application. Therefore, this invention fully complies with the provisions and requirements of the Patent Law. Therefore, we hereby file an application for an invention patent in accordance with the law and earnestly request your review and the granting of the patent. We would be grateful for your kindness.
1:電路迴路 11:走線 12:電場 13:磁場 14:橫電波 15:電容 2:電路系統 21:VRM 22:負載 23:電路板 231:走線 232:寄生電感 24:電容 1: Circuit loop 11: Trace 12: Electric field 13: Magnetic field 14: Transverse electromagnetic wave 15: Capacitor 2: Circuit system 21: VRM 22: Load 23: Circuit board 231: Trace 232: Parasitic inductance 24: Capacitor
第一圖:本發明於走線中產生橫電波狀態示意圖 第二圖:本發明於走線中產生橫電波之等效電路RL阻抗特性狀態示意圖 第三圖:本發明於電流1A、電容間距1mm進行諧振模式測試之波形圖[584KHz] 第四圖:本發明於電流1A、電容間距1mm進行諧振模式測試之波形圖[731KHz] 第五圖:本發明於電流1A、電容間距1mm進行諧振模式測試之波形圖[1.16MHz] 第六圖:本發明於電流1A、電容間距1mm進行諧振模式測試之波形圖[2.74MHz] 第七圖:本發明於電流1A、電容間距1mm進行諧振模式測試之波形圖[3.84GHz] 第八圖:本發明於電流1A、電容間距5mm進行諧振模式測試之波形圖[440KHz] 第九圖:本發明於電流1A、電容間距5mm進行諧振模式測試之波形圖[558KHz] 第十圖:本發明於電流1A、電容間距5mm進行諧振模式測試之波形圖[866KHz] 第十一圖:本發明於電流1A、電容間距5mm進行諧振模式測試之波形圖[2.03MHz] 第十二圖:本發明於電流1A、電容間距5mm進行諧振模式測試之波形圖[3.67GHz] 第十三圖:本發明於電流5A、電容間距1mm進行諧振模式測試之波形圖[661KHz] 第十四圖:本發明於電流5A、電容間距1mm進行諧振模式測試之波形圖[784KHz] 第十五圖:本發明於電流5A、電容間距1mm進行諧振模式測試之波形圖[1.2MHz] 第十六圖:本發明於電流5A、電容間距1mm進行諧振模式測試之波形圖[2.98MHz] 第十七圖:本發明於電流5A、電容間距1mm進行諧振模式測試之波形圖[2.96GHz] 第十八圖:本發明於電流5A、電容間距5mm進行諧振模式測試之波形圖[628KHz] 第十九圖:本發明於電流5A、電容間距5mm進行諧振模式測試之波形圖[970KHz] 第二十圖:本發明於電流5A、電容間距5mm進行諧振模式測試之波形圖[2.4MHz] 第二十一圖:本發明於電流5A、電容間距5mm進行諧振模式測試之波形圖[1.93GHz] 第二十二圖:本發明之輸出電容佈局設計結構示意圖[輸出電流1A、走線寬度1mm] 第二十三圖:本發明之輸出電容佈局設計結構示意圖[輸出電流5A、走線寬度5mm] 第二十四圖:現有電路板產生寄生電感狀態示意圖 Figure 1: Schematic diagram of the present invention generating transverse electromagnetic waves in traces Figure 2: Schematic diagram of the equivalent circuit RL impedance characteristics of the present invention generating transverse electromagnetic waves in traces Figure 3: Waveform diagram of the present invention tested in resonant mode with a current of 1A and a capacitor spacing of 1mm [584kHz] Figure 4: Waveform diagram of the present invention tested in resonant mode with a current of 1A and a capacitor spacing of 1mm [731kHz] Figure 5: Waveform diagram of the present invention tested in resonant mode with a current of 1A and a capacitor spacing of 1mm [1.16MHz] Figure 6: Waveform diagram of the present invention tested in resonant mode with a current of 1A and a capacitor spacing of 1mm [2.74MHz] Figure 7: Waveform diagram of the present invention tested in resonant mode with a current of 1A and a capacitor spacing of 1mm [3.84GHz] Figure 8: Waveform diagram of the present invention under resonant mode testing at a current of 1A and a capacitor spacing of 5mm [440KHz] Figure 9: Waveform diagram of the present invention under resonant mode testing at a current of 1A and a capacitor spacing of 5mm [558KHz] Figure 10: Waveform diagram of the present invention under resonant mode testing at a current of 1A and a capacitor spacing of 5mm [866KHz] Figure 11: Waveform diagram of the present invention under resonant mode testing at a current of 1A and a capacitor spacing of 5mm [2.03MHz] Figure 12: Waveform diagram of the present invention under resonant mode testing at a current of 1A and a capacitor spacing of 5mm [3.67GHz] Figure 13: Waveform diagram of the present invention under resonant mode testing at a current of 5A and a capacitor spacing of 1mm [661KHz] Figure 14: Waveform diagram of the present invention under resonant mode testing at a current of 5A and a capacitor spacing of 1mm [784KHz] Figure 15: Waveform diagram of the present invention under resonant mode testing at a current of 5A and a capacitor spacing of 1mm [1.2MHz] Figure 16: Waveform diagram of the present invention under resonant mode testing at a current of 5A and a capacitor spacing of 1mm [2.98MHz] Figure 17: Waveform diagram of the present invention under resonant mode testing at a current of 5A and a capacitor spacing of 1mm [2.96GHz] Figure 18: Waveform diagram of the present invention under resonant mode testing at a current of 5A and a capacitor spacing of 5mm [628KHz] Figure 19: Waveform diagram of the present invention under resonant mode testing at a current of 5A and a capacitor spacing of 5mm [970KHz] Figure 20: Waveform diagram of the present invention tested in resonant mode at 5A current and 5mm capacitor spacing [2.4MHz] Figure 21: Waveform diagram of the present invention tested in resonant mode at 5A current and 5mm capacitor spacing [1.93GHz] Figure 22: Schematic diagram of the output capacitor layout design structure of the present invention [output current 1A, trace width 1mm] Figure 23: Schematic diagram of the output capacitor layout design structure of the present invention [output current 5A, trace width 5mm] Figure 24: Schematic diagram of parasitic inductance generated in conventional circuit boards
1:電路迴路 1: Circuit loop
11:走線 11: Routing
15:電容 15: Capacitor
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Citations (17)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4879631A (en) * | 1989-01-18 | 1989-11-07 | Micron Technology, Inc. | Short-resistant decoupling capacitor system for semiconductor circuits |
| US6515868B1 (en) * | 1999-10-15 | 2003-02-04 | Nec Corporation | Printed circuit board |
| TW530229B (en) * | 2000-01-27 | 2003-05-01 | Matsushita Electric Industrial Co Ltd | A computer aided design apparatus for aiding design of a printed wiring board to effectively reduce noise |
| US20040136141A1 (en) * | 2002-12-19 | 2004-07-15 | Avx Corporation | Transmission line capacitor |
| TW200626011A (en) * | 2004-12-07 | 2006-07-16 | Mag Instr Inc | Improved circuitry for portable lighting devices and portable rechargeable electronic devices |
| US20060158828A1 (en) * | 2004-12-21 | 2006-07-20 | Amey Daniel I Jr | Power core devices and methods of making thereof |
| TW200631295A (en) * | 2004-11-02 | 2006-09-01 | Nec Electronics Corp | Apparatus and method for power conversion |
| US20060231947A1 (en) * | 2005-04-13 | 2006-10-19 | Toshiba America Elec. | Systems and methods for reducing simultaneous switching noise in an integrated circuit |
| TW200826444A (en) * | 2006-07-27 | 2008-06-16 | Koninkl Philips Electronics Nv | Switch mode power supply for in-line voltage applications |
| TW200936006A (en) * | 2008-02-13 | 2009-08-16 | Regulus Technologies Co Ltd | Twisted-overlap differential-pairs layout trace structure design |
| TW201251528A (en) * | 2011-06-10 | 2012-12-16 | Hon Hai Prec Ind Co Ltd | Capacitor performance optimization method and printed circuit boards using same |
| JP2013048142A (en) * | 2011-08-29 | 2013-03-07 | Rohm Co Ltd | Semiconductor integrated circuit system and arrangement wiring method thereof |
| US20150180351A1 (en) * | 2013-12-25 | 2015-06-25 | Delta Electronics (Shanghai) Co., Ltd. | Power electronic circuit and power module |
| US20200059201A1 (en) * | 2018-08-14 | 2020-02-20 | Nxp Usa, Inc. | Wideband biasing of high power amplifiers |
| CN111224542A (en) * | 2019-12-09 | 2020-06-02 | 北京航空航天大学 | Power module applied to miniaturized SERF magnetometer laser current source |
| US20210378090A1 (en) * | 2016-08-19 | 2021-12-02 | Nec Corporation | Electromagnetic wave reducing structure |
| CN117195808A (en) * | 2023-09-04 | 2023-12-08 | 电子科技大学长三角研究院(湖州) | System, method, medium, equipment and terminal for capacitor placement based on PCB resonance energy suppression |
-
2024
- 2024-08-07 TW TW113129601A patent/TWI898767B/en active
Patent Citations (17)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4879631A (en) * | 1989-01-18 | 1989-11-07 | Micron Technology, Inc. | Short-resistant decoupling capacitor system for semiconductor circuits |
| US6515868B1 (en) * | 1999-10-15 | 2003-02-04 | Nec Corporation | Printed circuit board |
| TW530229B (en) * | 2000-01-27 | 2003-05-01 | Matsushita Electric Industrial Co Ltd | A computer aided design apparatus for aiding design of a printed wiring board to effectively reduce noise |
| US20040136141A1 (en) * | 2002-12-19 | 2004-07-15 | Avx Corporation | Transmission line capacitor |
| TW200631295A (en) * | 2004-11-02 | 2006-09-01 | Nec Electronics Corp | Apparatus and method for power conversion |
| TW200626011A (en) * | 2004-12-07 | 2006-07-16 | Mag Instr Inc | Improved circuitry for portable lighting devices and portable rechargeable electronic devices |
| US20060158828A1 (en) * | 2004-12-21 | 2006-07-20 | Amey Daniel I Jr | Power core devices and methods of making thereof |
| US20060231947A1 (en) * | 2005-04-13 | 2006-10-19 | Toshiba America Elec. | Systems and methods for reducing simultaneous switching noise in an integrated circuit |
| TW200826444A (en) * | 2006-07-27 | 2008-06-16 | Koninkl Philips Electronics Nv | Switch mode power supply for in-line voltage applications |
| TW200936006A (en) * | 2008-02-13 | 2009-08-16 | Regulus Technologies Co Ltd | Twisted-overlap differential-pairs layout trace structure design |
| TW201251528A (en) * | 2011-06-10 | 2012-12-16 | Hon Hai Prec Ind Co Ltd | Capacitor performance optimization method and printed circuit boards using same |
| JP2013048142A (en) * | 2011-08-29 | 2013-03-07 | Rohm Co Ltd | Semiconductor integrated circuit system and arrangement wiring method thereof |
| US20150180351A1 (en) * | 2013-12-25 | 2015-06-25 | Delta Electronics (Shanghai) Co., Ltd. | Power electronic circuit and power module |
| US20210378090A1 (en) * | 2016-08-19 | 2021-12-02 | Nec Corporation | Electromagnetic wave reducing structure |
| US20200059201A1 (en) * | 2018-08-14 | 2020-02-20 | Nxp Usa, Inc. | Wideband biasing of high power amplifiers |
| CN111224542A (en) * | 2019-12-09 | 2020-06-02 | 北京航空航天大学 | Power module applied to miniaturized SERF magnetometer laser current source |
| CN117195808A (en) * | 2023-09-04 | 2023-12-08 | 电子科技大学长三角研究院(湖州) | System, method, medium, equipment and terminal for capacitor placement based on PCB resonance energy suppression |
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