小功率充电器的设计文献翻译

小功率充电器的设计文献翻译
小功率充电器的设计文献翻译

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小功率充电器的设计

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2010年月6日

黄河科技学院毕业设计(文献翻译)第1页1 引言

为了使手机、电动自行车等所使用的充电器实现自动充电的功能,大都采用各种各样的专用IC充电器集成电路和各种采样电路。本文介绍一种既能省去复杂的IC电路及其外围电路,又能够实现自动充电功能的电路。

2 工作原理

图1充电器的原理图

原理图如图1所示,它由如下元件构成:C1,V1~V4,C2组成滤波整流电路,变压器T为高频变压器,V5,R2,C11组成功率开关管V7的保护电路,NF为供给IC电源的绕组。单端输出IC为UC3842,其8脚输出5 V基准电压,2脚为反相输入,1脚为放大器输出,4脚为振荡电容C9,电阻R7输入端,5脚为接地端,3脚为过流保护端,6脚为调宽单脉冲输出端,7脚为电源输入端。R6、C7组成负反馈,IC启动瞬间

黄河科技学院毕业设计(文献翻译)第2页由R1供给启动电压,电路启动后由NF产生电势经V6,C4,C5整流滤波后供给IC工作电压。R12为过流保护取样电阻,V8,C3组成反激整流滤波输出电路。R13为内负载,V9~V12及R14~R19组成发光管显示电路。V5,V6选用FR107,V8选用FR154,V7选用K792,当V7导通时,整流电压加在变压器T初级绕组Np上的电能变成磁能储存在变压器中,在V7导通结束时,Np绕组中电流达到最大值:Ipmax:Ipmax=(E/Lp)ton式中:E为整流电压;Lp为变压器初级绕组电感;ton为V7导通时间。在V7关闭瞬间,变压器次级绕组放电电流为最大值Ismax,若忽略各种损耗应为:Ismax=nIpmax=n(E/Lp)ton。式中:n为变压器变比,n=Np/Ns,Np,Ns为变压器初、次级绕组匝数。

高频变压器在V7导通期间初级绕组储存能量与V7关闭期间次级绕组释放能量应相等:n(E/Lp)ton=(Uo/Ls)toff,式中:Ls为变压器次级绕组电感;Uo为输出电压;toff为V7关闭时间。

因为Lp=n2Ls,则:(E/nLs)ton=(Uo/Ls)toffEton=nUotoffUo=(ton/ntoff)E,上式说明输出电压Uo与ton成

正比,与匝比n及toff成反比。

变压器在导通期间储存的能量WLp为:WLp=(1/2)LpI2pmax

变压器Lp愈大储能愈多。

变压器储存的能量能否在toff期间释放完,不仅与变压器的工作频率f有关,而且与次级绕组电感量Ls有关,更与负载的大小有关。

储能释放时间常数τ和V7关闭时间toff之间的差异形成变换器三种工作状态,下面分开介绍:

(1)toff=τ这种状态为临界状态。各参数波形如图2所示。

图2中ub为Vp的控制电压波形;up为变压器初级Np电势波形;φ为变压器磁通变化波形;uces为V7集电极电压波形;ip,is为初、次级电流波形。

(2)toff>τ各参数波形如图3所示。

从图3中可以看出磁通φ复位时V7关闭还持续一段时间,ip呈线性上升,is线性下降。

黄河科技学院毕业设计(文献翻译)第3页

图2 t off=的波形图

图3t off>的波形图

变压器储存的能量等于电路输出能量:(1/2)LPIpmax2f=Uo2/RL

Uo2=(1/2)LpIpmax2RLf将Ipmax=(E/Lp)ton代入上式,则式中:RL为电路负载电阻;T=1/f为变压器工作周期。式中E,ton,T,Lp为定值,所以输出电压Uo随负载电阻RL的大小而变化,若忽略整流器件压降,则输出电压最大值应为:Uomax=(1/n)Up=(1/n)EV7

承受的反压应为:Ucc=E+ Up=E+nUo。

(3)toff<τ各参数波形如图4所示。从图4中可以看出磁通φ在toff期间不能复位,ip也不是从0开始线性增加,is下降不到0,这种工作状态输出电压Uo应满足如下关

黄河科技学院毕业设计(文献翻译)第4页系:Etou=(Np/Ns)Uot

Uo=(ton/toff)(Ns/Np)E

上式说明在Lp较大的情况下,Uo只决定于变压器匝数、导通截止脉宽和电源电压E,而与负载电阻RL无关。

图4 t off<的波形图

图5充电特性曲线

上述三种工作状态中,第二种工作状态输出电压Uo随负载电阻大小而变化,我们正好利用这个特点,满足充电器的充电特性。从电路中可知,电路的负载电阻RL实际上是被充电电池的等效内阻,当电池电量放空时,等效内阻RL很小,随着充电量增大,其等效内阻升高,而电路输出电压Uo就是充电电压,其变化是随RL增大而升高,所以有如图5所示的充电特性曲线。从图5可以看出充电电流是随着RL增大而下降。

黄河科技学院毕业设计(文献翻译)第5页IO=UO/RL充电电压UO、充电电流IO都是随RL而变化,RL的变化曲线是电池的充电特性决定的,所以用单端反激电路作成的充电器其充电电压、电流有很好的跟随性当电池充满后,RL也就大到一定限度,充电电压也就进入饱和状态,充电电流自动进入浮充状态。这样便大大简化了自动充电的控制电路。与相同性能的其他充电器电路相比,成本大大降低,可靠性大大提高。

图6磁滞回线图

3 电路设计计算

(1)高频变压器的设计

变压器是变换器的主要部件,其设计内容主要是磁芯选定,绕组匝数和导线直径的选定。

变压器主要参数计算公式:

输出功率PO=UOIO;输入功率PI=PO/Η;占空比D=TON/T;变压器效率为Η=PO /PI;负载电阻RL=UO/IO。

变压器输入电流最大值IPMAX=2UO2/DΗEMINRL;变压器输入电流有效值IPEFF=DIP;变压器工作频率F的确定:

F高虽然体积、重量可减小,但V7开关损耗增大,F低则变压器体积变大重量加大,综合考虑,一般选F=50 KHZ左右。

当电池充满后,RL也就大到一定限度,充电电压也就进入饱和状态,充电电流自动进入浮充状态。这样便大大简化了自动充电的控制电路。与相同性能的其他充电器电路相比,成本大大降低,可靠性大大提高。

(2)磁芯尺寸选取

黄河科技学院毕业设计(文献翻译)第6页因电路为单端反激电路,所以励磁电流是单方向的,变压器磁芯中产生的磁通只沿着磁滞回线在第一象限上下移动,如图6所示。

变压器初、次级功率关系为:

PS=ΗPTPO=PS-PD

式中:PS为变压器次级输出功率;PD为输出端二极管等损耗功率。若忽略PD,则:PO=ΗPT;SOSC=2POTON/Η△BJKOKC(PO单位为CM4)据式计算SO,SC,选取磁芯尺寸、规格。

(3)绕组匝数的计算

为了满足电路要求,式中E,TON应取最大值,单端反激电路变压器原边绕组兼有电感作用。其电感LP(单位:ΜH)所需量由下式计算:LP=ETON/IP。

式中:TON单位为ΜS。用下式核算NP绕组匝数能否满足电感量要求:LP''=(0.4ΠNP2SC×10-8)/(LΔ+LC/ΜC)式中:ΜC为磁芯材料有效导磁率;LC为磁芯磁路平均长度(CM);LΔ为磁芯中空气隙长度(单位为CM)。若LP≤LP'',则加大NP,以达到电感量要求。变压器匝比的选取:若不考虑次级整流压降及变压器内损等因素的影响,则N=EP/EO,NS=NNP/D,同理可计算NF=(NS/UO)UP。

(4)导线直径选取计算

若取J=2.5 A/MM2则:

D=0.7

由此计算出各绕组导线直径D(单位为MM)并选取规格值,验算磁芯窗口面积能否绕下各绕组,若绕不下,则重复上述有关设计计算。

(5)验算次级绕组放电常数,ΤS应小于TOFFΤS=LS/RL=(LP''/N2)/RL=LP''/(N2RL)TOFF=T/2,T=1/F,所以TOFF=1/(2F),TOFF>ΤS为验算原则。若不能满足,则重复上面有关计算。

来源于:开关电源技术开发应用

黄河科技学院毕业设计(文献翻译)第7页附录英文原文

Design of low-power charger

1 Introduction

In order for mobile phones, electric bicycles used by the charger for automatic charging function, mostly using a variety of specific IC charger IC and a variety of sampling circuits. This paper presents a complex IC eliminates the need for both circuit and peripheral circuits, but also be able to automatic recharge function of electricd.

2 works

Schematic shown in Figure 1, which consists of the following component composition:

C1, V1 ~ V4, C2 component filter rectifier, transformer T for the high-frequency transformer, V5, R2, C11-power switch V7 composition of the protection circuit, NF for the supply of IC power supply winding. Single-ended output IC for the UC3842, the 8-pin output of 5 V reference voltage for the inverting input pin 2, a pin for the amplifier output, 4 pin for oscillation capacitor C9, resistor R7 input, 5 feet for the ground side, 3 feet for the

over-current protection side, 6 feet for the single pulse-width-modulated output, 7 pin power input. R6, C7 composed of negative feedback, IC start an instant start from R1 supply voltage, the circuit starts electrical potential generated by the NF after V6, C4,

C5 rectified filtered supply IC operating voltage. Sampling resistor R12 for over-current protection, V8, C3 integral flyback rectifier filter output circuit. R13 as an internal load, V9 ~ V12 and R14 ~ R19 integral LED display circuit. V5, V6 choose FR107, V8 selected FR154, V7 selected K792, when the V7 conduction, the rectifier voltage is added to the transformer T primary winding Np on the energy into magnetic energy stored in the transformer, in turn V7 end, Np windings current reaches its maximum: Ipmax: Ipmax = (E / Lp) ton formula: E for the rectifier voltage; Lp for the transformer primary winding inductance; ton for the V7-time. V7 closed in an instant, transformer sub -

黄河科技学院毕业设计(文献翻译)第8页Winding discharge current maximum Ismax, if it ignores all kinds of losses should be: Ismax = nIpmax = n (E / Lp) ton. Where: n is transformer turns ratio, n = Np / Ns, Np, Ns for the transformer primary and secondary winding turns. Figure 1 Schematic diagram

Figure 1 Schematic diagram

High-frequency transformer in the primary winding during the conduction V7 store energy and V7 release energy during the shutdown of secondary windings should be equal to: n (E / Lp) ton = (Uo / Ls) toff, where: Ls of transformer secondary winding inductance; Uo is the output voltage; toff closing time for the V7.

Because Lp = n2Ls, then: (E / nLs) ton = (Uo / Ls) toffEton = nUotoffUo = (ton / ntoff) E, the type shows the output voltage Uo is proportional with the ton, and inversely proportional to the turns ratio n and the toff.

Transformer stored energy during the conduction WLp as follows:

Greater energy storage transformer Lp more. Transformer stored energy released during toff Can End, not only with the transformer operating frequency f, but also to the secondary

黄河科技学院毕业设计(文献翻译)第9页

winding inductance Ls, but also with the size of the load.

Stored energy release time constant τ and V7 closing time toff the differences between the three modes of operation the formation of converters, the following description separately:

(1) toff = τ in this state as a critical state. The parameters of the waveform shown in Figure1.

Figure2t off=waveform

Figure3t off>waveform

Figure 2 shows the waveform diagram toff = τ; Figure 2, ub for the Vp of the control voltage waveform; up for the transformer primary Np potential waveform; φ for the transformer flux changes in the waveform; uces for V7 collector voltage waveform; ip, is for

黄河科技学院毕业设计(文献翻译)第10页the beginning of , secondary current waveform.

(2) toff>τparameters of the waveform shown in Figure 3.

As can be seen from Figure 3, when the magnetic flux φ reset V7 closure also continue for some time, ip linear increase, is a linear decline.

Figure4t off

Figure5charger characteristics curve

Transformer stored energy is equal to the circuit output energy.

(1 / 2) LPIpmax2f = Uo2/RL

Uo2 = (1 / 2) LpIpmax2RLf will Ipmax = (E / Lp) ton substitution on the type, then type in: RL for the circuit load resistance; T = 1 / f for the transformer work cycle. Where E, ton, T, Lp is fixed value, so the output voltage Uo with the size of the load resistor RL changes, if ignored rectifiers drop, then the maximum output voltage should be: Uomax = (1 / n) Up = (1 / n) EV7 withstand back pressure should be: Ucc = E + Up = E + nUo.

黄河科技学院毕业设计(文献翻译)第11页

(3) toff <τ parameters of the waveform shown in Figure 4.

As can be seen from Figure4 the magnetic flux φ can not be reset at the toff period, ip is not a linear increase from 0 to the beginning, is down less than 0, this working condition the output voltage Uo should satisfy the following relationship:

On the Lp-type indicate a larger context, Uo is only determined by transformer number of turns, turn-on pulse width and power cut-off voltage E, has nothing to do with the load resistor RL.

The above-mentioned three kinds of working state, the second working condition the output voltage Uo with the size of the load resistance changes, we use this feature to meet the charger charging characteristics. We can see from the circuit, the circuit load resistor RL is actually the equivalent resistance by rechargeable batteries, when the battery shorting, the equivalent resistance RL is small, with the charge increase and the equivalent resistance increases , while the circuit output voltage Uo is the charge voltage, the change is increased with the increase of RL, so there are shown in Figure5, the charging characteristic curves. As can be seen from Figure 5, the charge current is decreased with the increase of RL.

IO = UO / RL charge voltage UO, the charge current with the RL change IO are, RL curve of the battery charging characteristics of the decision, so with the single-ended flyback circuit made into a charger of its charging voltage and current have a good The following performance when the battery is full, RL also great to a certain limit, also enter the saturation charge voltage, charge current is automatically floating state. This will greatly simplify the automatic charge control circuit. With the same performance as compared to other battery charger circuit, greatly reduce the cost and reliability greatly increased.

Figure 6magnetic circuit

黄河科技学院毕业设计(文献翻译)第12页3 Circuit design and calculation

(1) the design of high-frequency transformer

Converter transformer is a major component, designed mainly for core selection, winding turns and wire diameter selected.

Transformer main parameters of the formula:

Output power PO = UOIO; input power PI = PO / Η; duty cycle D = TON / T; transformer effi ciency Η = PO / PI; load resistor RL = UO / IO.

Transformer input current maximum IPMAX = 2UO2/DΗEMINRL; transformer input current RMS IPEFF = DIP; transformer operating frequency F, to determine: Paper the design of low-power charger for free papers from the https://www.360docs.net/doc/4c13225986.html, Network

F Gao Although the size, weight can be reduced, but the V7 switching loss increases, F low is to increase the weight of transformer size larger, comprehensive consideration, the general election about F = 50 K HZ.

When the battery is full, RL also great to a certain limit, also enter the saturation charge voltage, charge current is automatically floating state. This will greatly simplify the automatic charge control circuit. With the same performance as compared to other battery charger circuit, greatly reduce the cost and reliability greatly increased.

(2) core size selected

Due to the circuit for the single-ended flyback circuit, so the direction of excitation current is a single transformer core magnetic flux generated only along the hysteresis loop moves up and down in the first quadrant, as shown in Figure6.

Transformer primary and secondary power relationship:

PS = ΗPTPO = PS-PD

Where: PS output power for the transformer secondary; PD for the output diode power loss. If ignored PD, then: PO = ΗPT; SOSC = 2POTON / Η △ BJKOKC (PO unit CM4) was calculated SO, SC, select the core size, specifications.

黄河科技学院毕业设计(文献翻译)第13页

(3) The winding turns of the calculation of

In order to meet the circuit requirements, where E, TON shall be taken as the maximum, single-ended flyback circuit transformer primary side winding of the role of both inductors. The inductance LP (Unit: ΜH) the amount required for the calculation by the following formula: LP = ETON / IP.

Where: TON unit ΜS. With the following formula accounti ng for NP inductance winding turns can meet requirements: LP''= (0.4ΠNP2SC × 10-8) / (LΔ + LC / ΜC) formula: ΜC the effective permeability for the core material; LC for the The average length of core magnetic circuit (CM); LΔ for the core in the air gap length (in CM). If the LP ≤ LP'', then the increase NP, in order to achieve the inductance requirements. Transformer turns ratio select: It would not be within the secondary rectifier voltage drop, and transformer losses and other factors, then N = EP / EO, NS = NNP / D, By the same token calculate the NF = (NS / UO) UP.

(4) The calculation of wire diameter selected

If you take J = 2.5 A/MM2:

D = 0.7

Thus calculated for each winding wire diameter D (in units of MM) and select the specification value, checking whether the core area around the window, under the winding, if no less than around, then repeated the above-mentioned design calculations.

(5) checking secondary winding discharge constant, ΤS should be less than TOFFΤS = LS / RL = (LP''/ N2) / RL = LP''/ (N2RL) TOFF = T / 2, T = 1 / F, so TOFF = 1 / (2F), TOFF> ΤS principles for checking. If it is not satisfied, then repeat the calculation above.

From:China Technology Development and Application of Switching Power Supply

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