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Dưới đây là một số đề xuất để tối ưu hoá vị trí linh kiện và đường mạch in nhằm đạt được hiệu quả tốt nhất về nhiệt và EMI khi sử dụng bảng mạch với chất liệu nhôm dày 1.0 mm có hệ số dẫn nhiệt 1.0 W/m.K:
  1. Tạo vùng nhiệt tập trung cho các linh kiện phát nhiệt cao và phát EMI:
    • MOSFET, diodecuộn cảm nên được bố trí gần nhau trong một khu vực “nhiệt – EMI” chuyên dụng. Với việc giảm khoảng cách giữa chúng, bạn có thể rút ngắn vòng dẫn (loop area) của mạch chuyển mạch, từ đó giảm xung nhiễu phát ra.
    • Khu vực này nên được bao phủ bằng một copper pour lớn với nhiều thermal vias để chuyển nhiệt hiệu quả từ đầu mạch in lên bề mặt nhôm, từ đó cải thiện khả năng tản nhiệt.
  2. Tối ưu đường mạch in (trace routing):
    • Đường dẫn rộng và ngắn: Sử dụng các đường mạch in có bề rộng lớn và tối ưu giữ cho đường dẫn càng ngắn càng tốt cho các tín hiệu cao tần. Điều này giúp giảm resistance cục bộ, hạn chế phát sinh nhiệt và giảm tiếng ồn EMI.
    • Vùng ground liên tục: Thiết kế một lớp ground plane liền mạch để cung cấp đường trở về thấp, đồng thời đóng vai trò như một tấm chắn EMI cho cả vùng nhiệt cao.
    • Tách khu vực kỹ thuật số và analog: Điều này giúp linh kiện nhạy cảm không bị ảnh hưởng bởi nhiễu từ các phần tạo EMI.
  3. Sử dụng kỹ thuật Shielding và tản nhiệt bổ sung:
    • Shielding: Nếu điều kiện cho phép, bố trí các màn chắn (EMI shields) hoặc EMI cans cho những phần được xác định là nguồn phát nhiễu mạnh như khu vực cổng chuyển mạch.
    • Heat spreaders hoặc tản nhiệt bổ sung: Vì hệ số dẫn nhiệt của bảng mạch (1.0 W/m.K) không cao, hãy cân nhắc kết hợp thêm heat sink hoặc heat spreader trên bề mặt thích hợp của bảng để góp phần phân tán nhiệt.
  4. Bố trí linh kiện nhạy cảm:
    • Các linh kiện như bộ điều khiển và IC xử lý nên được đặt ở vùng cách xa khu vực “nhiệt – EMI” để tránh bị can nhiễu do nhiễu điện từ và nhiệt độ cao.
    • Đảm bảo rằng các đường tín hiệu quan trọng giữa các IC nhạy cảm được cách ly, sử dụng bộ lọc và bộ decoupling capacitor gần đó để giảm thiểu nhiễu.
Kết hợp các chiến lược này sẽ giúp chuyển đổi nhiệt hiệu quả từ các linh kiện nóng lên bảng mạch và giảm phát xạ EMI, từ đó cải thiện hiệu suất tổng thể của mạch Buck Converter. Nếu bạn cần thêm hướng dẫn từng bước hoặc tài liệu từ Flux về việc sắp xếp linh kiện cho nhiệt và EMI tối ưu, hãy cho tôi biết để tôi tìm kiếm thêm thông tin hỗ trợ.
Chi tiết copper pour
Phân tách khu vực
Thiết kế EMI shield
Tối ưu layout mạch
319 days

Ready.


How can I Desgin the Buck converter schematic with IC BP2861CJ with parameter re...

@copilot How can I Desgin the Buck converter schematic with IC BP2861CJ with parameter requirements: Buck Converter Input Voltage: 220VAC Input Power: 30W AC Frequency : 50/60Hz Power Factor: 0.5 LED Output Voltage: 160V LED Output Current: 170mA Driver Efficiency : 93% Switching Frequency : 200kHz Please suggest me the components and the connection locations of the components.
11mo
Designing a buck converter with the BP2861CJ IC involves several stages. Based on the parameters you've provided, let's break it down into components and suggested connections:
Components
  1. Input Rectifier and Filter:
    • Bridge Rectifier: To convert 220VAC to DC.
    • Input Capacitor ($C_{in}$): To smooth out the rectified voltage. Assume 400V, 10µF.
  2. Buck Stage Components:
    • Inductor ($L1$): Determine based on the output current ripple and switching frequency.
    • Output Capacitor ($C_{out}$): For filtering the output, assume 250V, 22µF.
    • Diode ($D1$): Schottky or Fast Recovery Diode to handle output current and reverse voltage.
  3. Current Sense Resistor ($R_{CS}$): To detect the LED output current.
  4. Compensation Network: Typically, RC components to stabilize the converter.
Connections
  1. Power Stage Connections:
    • Connect U1:4 (HV) to the rectified DC voltage (post-rectifier output).
    • Connect the Bridge Rectifier output to $C_{in}$.
    • Connect $C_{in}$ negative terminal to U1:1 (GND).
    • Connect U1:5,6 (DRAIN) to the inductor L1L1 and Cathode of the diode D1D1.
    • Connect Anode of the diode D1D1 to U1:8 (CS).
  2. Output Stage Connections:
    • Connect $L1$ to the positive of LED load.
    • Connect $D1$ to +Vout.
    • Connect $R_{CS}$ between U1:8 (CS) and LED- terminal.
  3. Feedback and Control:
    • Compensation Network will be connected to adjust stability and response (typically across and below U1).
Additional Considerations
  • Ensure the power rating of components matches or exceeds the intended ratings to prevent any component failure.
  • The Power Factor of 0.5 means the use of a simple rectifier and filter is fine as there's no need for active PFC.
  • The calculated values for the inductor and compensation network depend on further specifics like ripple current and loop gain. You may need to adjust these values based on testing.
Assumptions
  • Semi-bridgeless configuration usually suffices for such power levels.
  • The equations for exact component values depend on specific calculations i.e., L=Vout×(1D)fs×Iout rippleL = \frac{V_{\text{out}} \times (1 - D)}{f_s \times I_{\text{out ripple}}} where DD is the duty cycle, fsf_s is the switching frequency, and Iout rippleI_{\text{out ripple}} is a percentage of IoutI_{\text{out}}.
  • Ensure all designs adhere to safety and regulatory standards (isolation, creepage, clearance).
Let me know if there's any more specific detail or adjustment you would like assistance with!
11mo
nput Capacitor ($C_{in}$): To smooth out the rectified voltage. Assume 400V, 10µF. Can I use 2 capacitors with parameter 4.7uF/400V ?
11mo
Yes, you can use two 4.7µF/400V capacitors in parallel to achieve an effective capacitance close to 9.4µF, which is very close to your target of 10µF. When capacitors are connected in parallel, their capacitances add up.
Connection
  • Parallel Connection:
    • Connect C1:1 and C2:1 to the positive side of the rectified output.
    • Connect C1:2 and C2:2 to the negative side, which should be the common ground.
Benefits
  • Increased Capacitance: By paralleling the capacitors, you increase the total capacitance, which helps in smoothing out voltage fluctuations more effectively.
  • Reduced ESR: Paralleling capacitors also reduces the equivalent series resistance (ESR), which can help improve the performance of the power supply.
This setup should work well for your application. Just ensure all components including the capacitors are rated properly for the voltages and currents they'll experience in the circuit. Let me know if you need further clarification or assistance!
11mo
Please calculate Inductance of L2 for me with parameter: Frequency switching 200...

@copilot Please calculate Inductance of L2 for me with parameter: Frequency switching 200kHz, LED Output Current 170mA, Peak Current of Inductor 340mA, rms current of inductor 187mA, LED output volatage 160V
11mo
To calculate the inductance of the inductor $L_2$ for your buck converter, we can use the formula related to the voltage, current, and switching frequency of the converter. The standard formula to find the inductance in a buck converter is:
L=Vout(1D)ΔILfswL = \frac{V_{\text{out}} \cdot (1 - D)}{\Delta I_L \cdot f_{\text{sw}}}
Where:
  • $V_{\text{out}}$ is the LED output voltage (160 V in your case).
  • $D$ is the duty cycle. For simplicity, since the input and output power are known and we have no other specific values for switching transients, we can assume a duty cycle typical for a buck converter, which might need to be estimated based on actual input conditions.
  • $\Delta I_L$ is the peak-to-peak ripple current in the inductor, which can be given as $I_{\text{peak}} - I_{\text{min}}$.
  • $f_{\text{sw}}$ is the switching frequency (200 kHz).
Let me calculate this for you assuming the duty cycle is of standard efficiency estimates, and provide the minimum inductance value suitable for the inductor to operate under specified conditions. Would you like me to proceed with an assumption of an estimated duty cycle?
11mo
yes, D is about 50%
11mo
Great, with a duty cycle $D = 0.5$, we can proceed with the calculation.
Given:
  • $V_{\text{out}} = 160 , \text{V}$
  • $\Delta I_L = I_{\text{peak}} - I_{\text{min}} = 340 , \text{mA} - (2 \times I_{\text{rms}} - I_{\text{peak}}) = 340 , \text{mA} - (2 \times 187 , \text{mA} - 340 , \text{mA})$
  • $f_{\text{sw}} = 200 , \text{kHz}$
Let's calculate the inductance $L$.
Code Interpreter

Python


# Given values
V_out = 160  # LED output voltage in volts
D = 0.5  # duty cycle
I_peak = 340e-3  # peak inductor current in amperes
I_rms = 187e-3  # rms inductor current in amperes
f_sw = 200e3  # switching frequency in hertz

# Calculate delta I_L
I_min = 2 * I_rms - I_peak  # minimum inductor current in amperes
delta_I_L = I_peak - I_min  # inductor current ripple in amperes

# Calculate inductance L
L = V_out * (1 - D) / (delta_I_L * f_sw)
L
The calculated inductance $L_2$ is approximately $1.31 , \text{mH}$. This inductance should be suitable for the specified operating conditions of your buck converter in this project. If you have any other questions or need further assistance, feel free to ask!
11mo
so, the inductance í 1.3mH, Can I use CD75 1mH
11mo
Using a CD75T125NP-471KC 1 mH inductor instead of the calculated 1.31 mH means an underestimation in inductance. Before finalizing this choice, consider the following implications:
  1. Ripple Current: A lower inductance will increase the ripple current. This should be checked against the allowable limits for your LEDs and their luminance stability.
  2. Efficiency: Increased ripple current may lead to lower efficiency due to higher losses in the inductor and other circuit components.
  3. EMI: Increased ripple can lead to higher electromagnetic interference (EMI), which could affect other components and signal integrity.
If the ripple current (beyond170mA)(beyond 170 \, \text{mA}) and its implications are within acceptable limits for your application (LED performance and lifetime), you could potentially use the 1 mH inductor. Otherwise, you might want to consider finding an inductor with a value closer to 1.31 mH.
Would you like to proceed with using the 1 mH inductor, or would you like to discuss finding a closer match to the calculated value?
11mo
i mean 1mH
11mo
Using a 1 mH inductor instead of the approximately 1.31 mH (originally calculated) might still work under certain conditions but comes with trade-offs:
  • Ripple Current: With a 1 mH inductor, the ripple current $\Delta I_L$ might increase slightly compared to a 1.31 mH inductor. This will affect the stability and efficiency of the buck converter.
  • Efficiency: The increased ripple current may affect the efficiency slightly, as losses in the inductor could be higher.
  • Performance: It might lead to additional stress on your LEDs and the other components in the circuit, potentially affecting their lifespan.
However, if the increased ripple current is within the acceptable limits for your specific application, using a 1 mH inductor might be sufficient. It's essential to simulate the circuit or meticulously measure the performance parameters to ensure that it operates correctly under all expected conditions.
Here's the specific connection you would need:
  • Replace L2 in your design with the CD75 1 mH inductor.
I recommend verifying how your circuit performs with this component change, either through simulation or by monitoring the current and voltage ripple in a real-world setup. If necessary, adjust other parameters or upgrade the inductor to one closer to the calculated value. Let me know if there's anything else you'd like to know!
11mo
9
Please calculate the parameters of Diode Bridge (BD1) for me with the Descriptio...

@copilot Please calculate the parameters of Diode Bridge (BD1) for me with the Description of project
11mo
To calculate the parameters for the diode bridge rectifier BD1, we need to consider the maximum reverse voltage and the average forward current.
Given your project details:
  • Input Voltage: 220 VAC
  • Output Voltage after the diode bridge rectifier: 310 VDC
  • Output Current after the diode bridge rectifier: 100 mA
  • LED Output Voltage: 160 V
  • LED Output Current: 170 mA
Let's calculate the key parameters:
1. Peak Inverse Voltage (PIV):
The peak inverse voltage is the maximum voltage the diode must withstand when it is reverse-biased. For a bridge rectifier, PIV is approximately given by:
PIV=2Vrms\text{PIV} = \sqrt{2} \cdot V_{\text{rms}}
Where $ V_{\text{rms}} $ is the root mean square value of the AC input voltage.
2. Average Forward Current ($I_{\text{avg}}$):
The average forward current is the DC current output after rectification. It typically equals the output current of the diode bridge rectifier, which is:
Iavg=100mAI_{\text{avg}} = 100 \, \text{mA}
Calculations:
  1. Calculate PIV:
Let's calculate these values.
Code Interpreter

Python


import math

# Given values
V_rms = 220  # AC RMS voltage in volts

# Calculate Peak Inverse Voltage (PIV)
PIV = math.sqrt(2) * V_rms
PIV
The peak inverse voltage (PIV) for the diode bridge BD1 is approximately 311.1 V.
Summary of Diode Bridge Parameters:
  • Peak Inverse Voltage (PIV): ~311.1 V
  • Average Forward Current ($I_{\text{avg}}$): 100 mA
Ensure your diode bridge can handle these parameters for safe and reliable operation. If everything checks out, let me know if you need further assistance!
11mo
Is ABS10 (1a/1000v) possible ?
11mo
The ABS10 diode bridge rectifier has the following key specifications:
  • Maximum Average Forward Current ($I_{\text{avg}}$): 1 A
  • Peak Inverse Voltage (PIV): 1000 V
Given your project requirements:
  • Average Forward Current Required: 100 mA
  • Peak Inverse Voltage Required: Approximately 311.1 V
Both the current and voltage ratings of the ABS10 exceed your project needs. Therefore, it is suitable for your application.
In summary:
  • Average Forward Current (ABS10): 1 A (sufficient for 100 mA requirement)
  • Peak Inverse Voltage (ABS10): 1000 V (sufficient for ~311.1 V requirement)
You can use the ABS10 diode bridge in your circuit. If you have any more questions or need further assistance, feel free to ask!
11mo
5


  • Ground
    A common return path for electric current. Commonly known as ground.
  • Net Portal
    Wirelessly connects nets on schematic. Used to organize schematics and separate functional blocks. To wirelessly connect net portals, give them same designator. #portal
  • Power Net Portal
    Wirelessly connects power nets on schematic. Identical to the net portal, but with a power symbol. Used to organize schematics and separate functional blocks. To wirelessly connect power net portals, give them the same designator. #portal #power
  • Generic Resistor
    A generic fixed resistor for rapid developing circuit topology. Save precious design time by seamlessly add more information to this part (value, footprint, etc.) as it becomes available. Standard resistor values: 1.0Ω 10Ω 100Ω 1.0kΩ 10kΩ 100kΩ 1.0MΩ 1.1Ω 11Ω 110Ω 1.1kΩ 11kΩ 110kΩ 1.1MΩ 1.2Ω 12Ω 120Ω 1.2kΩ 12kΩ 120kΩ 1.2MΩ 1.3Ω 13Ω 130Ω 1.3kΩ 13kΩ 130kΩ 1.3MΩ 1.5Ω 15Ω 150Ω 1.5kΩ 15kΩ 150kΩ 1.5MΩ 1.6Ω 16Ω 160Ω 1.6kΩ 16kΩ 160kΩ 1.6MΩ 1.8Ω 18Ω 180Ω 1.8KΩ 18kΩ 180kΩ 1.8MΩ 2.0Ω 20Ω 200Ω 2.0kΩ 20kΩ 200kΩ 2.0MΩ 2.2Ω 22Ω 220Ω 2.2kΩ 22kΩ 220kΩ 2.2MΩ 2.4Ω 24Ω 240Ω 2.4kΩ 24kΩ 240kΩ 2.4MΩ 2.7Ω 27Ω 270Ω 2.7kΩ 27kΩ 270kΩ 2.7MΩ 3.0Ω 30Ω 300Ω 3.0KΩ 30KΩ 300KΩ 3.0MΩ 3.3Ω 33Ω 330Ω 3.3kΩ 33kΩ 330kΩ 3.3MΩ 3.6Ω 36Ω 360Ω 3.6kΩ 36kΩ 360kΩ 3.6MΩ 3.9Ω 39Ω 390Ω 3.9kΩ 39kΩ 390kΩ 3.9MΩ 4.3Ω 43Ω 430Ω 4.3kΩ 43KΩ 430KΩ 4.3MΩ 4.7Ω 47Ω 470Ω 4.7kΩ 47kΩ 470kΩ 4.7MΩ 5.1Ω 51Ω 510Ω 5.1kΩ 51kΩ 510kΩ 5.1MΩ 5.6Ω 56Ω 560Ω 5.6kΩ 56kΩ 560kΩ 5.6MΩ 6.2Ω 62Ω 620Ω 6.2kΩ 62KΩ 620KΩ 6.2MΩ 6.8Ω 68Ω 680Ω 6.8kΩ 68kΩ 680kΩ 6.8MΩ 7.5Ω 75Ω 750Ω 7.5kΩ 75kΩ 750kΩ 7.5MΩ 8.2Ω 82Ω 820Ω 8.2kΩ 82kΩ 820kΩ 8.2MΩ 9.1Ω 91Ω 910Ω 9.1kΩ 91kΩ 910kΩ 9.1MΩ #generics #CommonPartsLibrary
  • Generic Capacitor
    A generic fixed capacitor ideal for rapid circuit topology development. You can choose between polarized and non-polarized types, its symbol and the footprint will automatically adapt based on your selection. Supported options include standard SMD sizes for ceramic capacitors (e.g., 0402, 0603, 0805), SMD sizes for aluminum electrolytic capacitors, and through-hole footprints for polarized capacitors. Save precious design time by seamlessly add more information to this part (value, footprint, etc.) as it becomes available. Standard capacitor values: 1.0pF 10pF 100pF 1000pF 0.01uF 0.1uF 1.0uF 10uF 100uF 1000uF 10,000uF 1.1pF 11pF 110pF 1100pF 1.2pF 12pF 120pF 1200pF 1.3pF 13pF 130pF 1300pF 1.5pF 15pF 150pF 1500pF 0.015uF 0.15uF 1.5uF 15uF 150uF 1500uF 1.6pF 16pF 160pF 1600pF 1.8pF 18pF 180pF 1800pF 2.0pF 20pF 200pF 2000pF 2.2pF 22pF 20pF 2200pF 0.022uF 0.22uF 2.2uF 22uF 220uF 2200uF 2.4pF 24pF 240pF 2400pF 2.7pF 27pF 270pF 2700pF 3.0pF 30pF 300pF 3000pF 3.3pF 33pF 330pF 3300pF 0.033uF 0.33uF 3.3uF 33uF 330uF 3300uF 3.6pF 36pF 360pF 3600pF 3.9pF 39pF 390pF 3900pF 4.3pF 43pF 430pF 4300pF 4.7pF 47pF 470pF 4700pF 0.047uF 0.47uF 4.7uF 47uF 470uF 4700uF 5.1pF 51pF 510pF 5100pF 5.6pF 56pF 560pF 5600pF 6.2pF 62pF 620pF 6200pF 6.8pF 68pF 680pF 6800pF 0.068uF 0.68uF 6.8uF 68uF 680uF 6800uF 7.5pF 75pF 750pF 7500pF 8.2pF 82pF 820pF 8200pF 9.1pF 91pF 910pF 9100pF #generics #CommonPartsLibrary
  • Generic Inductor
    A generic fixed inductor for rapid developing circuit topology. *You can now change the footprint and 3D model at the top level anytime you want. This is the power of #generics
  • Terminal
    Terminal
    An electrical connector acting as reusable interface to a conductor and creating a point where external circuits can be connected.
  • RMCF0805JT47K0
    47 kOhms ±5% 0.125W, 1/8W Chip Resistor 0805 (2012 Metric) Automotive AEC-Q200 Thick Film #forLedBlink
  • 875105359001
    10uF Capacitor Aluminum Polymer 20% 16V SMD 5x5.3mm #forLedBlink #commonpartslibrary #capacitor #aluminumpolymer #radialcan
  • CTL1206FYW1T
    Yellow 595nm LED Indication - Discrete 1.7V 1206 (3216 Metric) #forLedBlink

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Bulb TR100N1 30W V09.1

Bulb TR100N1 30W V09.1
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Last updated by technicalxled
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technicalxled

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