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电源芯片-TD6810英文-Datasheet

电源芯片-TD6810英文-Datasheet
电源芯片-TD6810英文-Datasheet

General Description

The TD6810 is a high efficiency monolithic synchronous buck regulator using a constant frequency, current mode architecture. The device is available in an adjustable version and fixed output voltages of 1.5V and 1.8V.

Supply current during operation is only 20mA and drops to ≤1mA in shutdown. The 2.5V to 5.5V input voltage range makes the TD6810 ideally suited for single Li-Ion battery-powered applications. 100% duty cycle provides low dropout operation, extending battery life in portable systems.Automatic Burst Mode operation increases efficiency at light loads, further extending battery life. Switching frequency is internally set at 1.5MHz, allowing the use of small surface mount inductors and capacitors.The internal synchronous switch increases efficiency and eliminates the need for an external Schottky diode. Low output voltages are easily supported with the 0.6V

feedback reference voltage. The TD6810 is available in a low profile (1mm) TSOT23-5 package.

Features

z High Efficiency: Up to 96%

z High Efficiency at light loads

z Very Low Quiescent Current: Only 20uA During

Operation

z 800mA Output Current

z 2.5V to 5.5V Input Voltage Range z 1.5MHz Constant Frequency Operation z No Schottky Diode Required

z Low Dropout Operation: 100% Duty Cycle z 0.6V Reference Allows Low Output Voltages z Shutdown Mode Draws ≤1uA Supply Current

z Current Mode Operation for Excellent Line and Load

Transient Response z Overtemperature Protected

z Low Profile (1mm) TSOT23-5 Package

Applications

z Cellular Telephones

z Personal Information Appliances z Wireless and DSL Modems z Digital Still Cameras z MP3 Players z Portable Instruments

Package Types

gure 1. Package Types

of TD6810

SOT23-5

Pin Assignments

TSOT23‐5

Pin Name Description

1 RUN

Run Control Input. Forcing this pin above 1.5V enables the part. Forcing this pin below 0.3V shuts down the device. In shutdown, all functions are disabled drawing <1μA supply current. Do not leave RUN floating.

2 GND Ground Pin.

3 SW Switch Node Connection to

Inductor. This pin connects to the drains of the internal main and synchronous power MOSFET switches.

4 VIN Main Supply Pin. Must be closely

decoupled to GND, Pin 2, with a 2.2μF or greater ceramic capacitor.

5 VFB Feedback Pin. Receives the

feedback voltage from an external resistive divider across the output.

5 VOUT

Output Voltage Feedback Pin. An internal resistive divider divides the output voltage down for comparison to the internal reference voltage.

Ordering Information

TD6810 □ □

Circuit Type Output Versions Classifying:

Blank :Adj 12:1.2V Package 15:1.5V T :TSOT-23 18:1.8V

Functional Block Diagram

Figure2:Functional Block Diagram of TD6810

Type Application Circuit

Figure 3. Type Application Circuit of TD6810

Absolute Maximum Ratings

Note1: Stresses greater than those listed under Maximum Ratings may cause permanent damage to the device. This is a stress rating only and functional operation

of the device at these or any other conditions above those indicated in the operation is not implied. Exposure to absolute maximum rating conditions for extended

periods may affect reliability.

Parameter Value

Unit Input Supply Voltage -0.3 ~6 V

RUN, VFB Voltages -0.3 ~ VIN V

SW Voltage -0.3V ~(VIN+0.3) V

P-Channel Switch Source Current (DC) 1000 mA

N-Channel Switch Sink Current (DC) 1000 mA

Peak SW Sink and Source Current 1.3 A

Operating Temperature Range -40~+85 oC

Junction Temperature 125 oC

Lead Temperature (Soldering, 10 sec) 300 oC

Storage Temperature Range -65~150 oC

Electrical Characteristics

Unless otherwise specified, VIN= 3.6V TA=25 oC.

Symbol Parameter Conditions Min.

Typ.

Max.

Unit

IVFB Feedback

Current 30

nA

VFB Regulated Feedback

Voltage

TA = 25°C 0.5880 0.6000 0.6120

V

0°C TA ≤ 85°C 0.5865 0.6000 0.6135

–40°C ≤ TA ≤ 85°C 0.5850 0.6000 0.6150

VFB Reference Voltage Line

Regulation

VIN = 2.5V to 5.5V 0.04 0.4 %/ V

VOUT Regulated Output

Voltage

TD6810-1.5, IOUT = 100mA 1.455 1.500 1.545 V

TD6810-1.8, IOUT = 100mA 1.746 1.800 1.854

VOUT Output Voltage Line

Regulation

VIN = 2.5V to 5.5V 0.04 0.4 %/ V

Electrical Characteristics(Cont.)

Unless otherwise specified, VIN= 3.6V TA=25 oC.

Symbol Parameter Conditions Min.

Typ.

Max.

Unit

IPK Peak Inductor Current VIN = 3V, VFB = 0.5V or

VOUT = 90%, Duty Cycle <

35%

1.05 1.10 1.15 A

VLOADREG Output Voltage Load

Regulation

0.5

%

VIN Input Voltage Range 2.5 5.5 V

IS Input DC Bias Current

Active Mode

VFB = 0.5V or VOUT =

90%, ILOAD = 0A

300

400

uA Sleep Mode

VFB = 0.62V or VOUT =

103%, ILOAD = 0A

20

35

uA Shutdown VRUN = 0V, VIN = 4.2V 0.1 1 uA

fOSC

Oscillator Frequency VFB = 0.6V or VOUT =

100%

1 1.5

2 MHz VFB = 0V or VOUT = 0V 400 KHz

RPFET RDS(ON) of P-Channel

FET

ISW = 100mA 0.35 0.45 ?

RNFET RDS(ON) of N-Channel

FET

ISW = -100mA 0.35 0.45 ?

ILSW SW

Leakage VRUN = 0V, VSW = 0V or

5V, VIN = 5V

0.01

1 uA

VRUN RUN

Threshold 0.3

1 1.5

V IRUN RUN Leakage Current 0.01

1 uA

Typical Operating Characteristics

Oscillator Frequency Reference Voltage

Oscillator Frequency vs Supply Voltage

RDS(ON) vs Temperature

Typical Operating Characteristics(Cont.)

Efficiency vs Output Current RDS(ON) vs Input Voltage

Efficiency vs Output Current

Efficiency vs Output Current

Typical Operating Characteristics(Cont.)

Output Voltage vs Output Current Efficiency vs Output Current

Output Voltage vs Output Current Dynamic Supply Current vs Supply Voltage

Typical Operating Characteristics(Cont.)

P-FET Leakage vs Temperature

N-FET Leakage vs Temperature

Efficiency VS Output Current

Function Description

Main Control Loop

The TD6810 uses a constant frequency, current mode step-down architecture. Both the main (P-channel MOSFET) and synchronous (N-channel MOSFET) switches are internal. During normal operation, the internal top power MOSFET is turned on each cycle when the oscillator sets the RS latch, and turned off when the current comparator, ICOMP, resets the RS latch. The peak inductor current at which ICOMP resets the RS latch, is controlled by

the output of error amplifier EA. When the load current increases, it causes a slight decrease in the feedback voltage, FB, relative to the 0.6V reference, which in turn, causes the EA amplifier’s output voltage to increase until the average inductor current matches the new load current. While the top MOSFET is off, the bottom MOSFET is turned on until either the inductor current starts to reverse, as indicated by the current reversal comparator IRCMP, or the beginning of the next clock cycle.

Burst Mode Operation

The TD6810 is capable of Burst Mode operation in which the internal power MOSFETs operate intermittently based on load demand.

In Burst Mode operation, the peak current of the inductor is set to approximately 200mA regardless of the output load. Each burst event can last from a few cycles at light loads to almost continuously cycling with short sleep intervals at moderate loads. In between these burst events, the power MOSFETs and any unneeded circuitry are turned off, reducing the quiescent current to 20mA. In this sleep state, the load current is being supplied solely from the output capacitor. As the output voltage droops, the EA amplifier’s output rises above the sleep threshold signaling the BURST comparator to trip and turn the top MOSFET on. This process repeats at a rate that is dependent on the load demand.

Short-Circuit Protection

When the output is shorted to ground, the frequency of the oscillator is reduced to about 400kHz, 1/4 the nominal frequency. This frequency foldback ensures that the inductor current has more time to decay, thereby preventing runaway. The oscillator’s frequency will progressively increase to 1.5MHz when VFB or VOUT rises above 0V.

Dropout Operation

As the input supply voltage decreases to a value approaching the output voltage, the duty cycle increases toward the maximum on-time. Further reduction of the supply voltage forces the main switch to remain on for more than one cycle until it reaches 100% duty cycle. The output voltage will then be determined by the input voltage minus the voltage drop across the P-channel MOSFET and the inductor.

An important detail to remember is that at low input supply voltages, the RDS(ON) of the P-channel switch increases (see Typical Performance Characteristics). Therefore, the user should calculate the power dissipation when the TD6810 is used at 100% duty cycle with low input voltage (See Thermal Considerations in the Applications Information

section).

Function Description(Cont.)

Low Supply Operation

The TD6810 will operate with input supply voltages as

low as 2.5V, but the maximum allowable output current is

reduced at this low voltage. Figure 2 shows the reduction

in the maximum output current as a function of input

voltage for various output voltages.

Slope Compensation and Inductor Peak

Current

Slope compensation provides stability in constant

frequency architectures by preventing subharmonic

oscillations at high duty cycles. It is accomplished

internally by adding a compensating ramp to the inductor

current signal at duty cycles in excess of 40%. Normally,

this results in a reduction of maximum inductor peak

current for duty cycles >40%. However, the TD6810 uses

a patent-pending scheme that counteracts this

compensating ramp, which allows the maximum inductor

peak current to remain unaffected throughout all duty

cycles.

Maximum Output Current vs Input Voltag

The basic TD6810 application circuit is shown in Figure

3. External component selection is driven by the load

requirement and begins with the selection of L followed

by CIN and COUT.

Inductor Selection

For most applications, the value of the inductor will fall in

the range of 1uH to 4.7uH. Its value is chosen based on

the desired ripple current. Large value inductors lower

ripple current and small value inductors result in higher

ripple currents. Higher VIN or VOUT also increases the

ripple current as shown in equation 1. A reasonable

starting point for setting ripple current is DIL = 320mA

(40% of 800mA).

The DC current rating of the inductor should be at least

equal to the maximum load current plus half the ripple

current to prevent core saturation. Thus, a 920mA rated

inductor should be enough for most applications (800mA

+ 120mA). For better efficiency, choose a low

DC-resistance

inductor.

The inductor value also has an effect on Burst Mode

operation. The transition to low current operation begins

when the inductor current peaks fall to approximately

200mA. Lower inductor values (higher DIL) will cause

this to occur at lower load currents, which can cause a

dip in efficiency in the upper range of low current

operation. In Burst Mode operation, lower inductance

values will cause the burst frequency to increase.

Function Description(Cont.)

Inductor Core Selection

Different core materials and shapes will change the

size/current and price/current relationship of an inductor.

Toroid or shielded pot cores in ferrite or permalloy

materials are small and don’t radiate much energy, but

generally cost more than powdered iron core inductors

with similar electrical characteristics. The choice of which

style inductor to use often depends more on the price vs

size requirements and any radiated field/EMI

requirements than on what the TD6810 requires to

operate. Table 1 shows some typical surface mount

inductors that work well in TD6810 applications.

Table 1. Representative Surface Mount Inductors

CIN and COUT Selection

In continuous mode, the source current of the top

MOSFET is a square wave of duty cycle VOUT/VIN. To

prevent large voltage transients, a low ESR input

capacitor sized for the maximum RMS current must be

used. The maximum RMS capacitor current is given by:

This formula has a maximum at VIN = 2VOUT, where

IRMS = IOUT/2. This simple worst-case condition is

commonly used for design because even significant

deviations do not offer much relief. Note that the

capacitor manufacturer’s ripple current ratings are often

based on 2000 hours of life. This makes it advisable to

further derate the capacitor, or choose a capacitor rated

at a higher temperature than required. Always consult

the manufacturer if there is any question.

The selection of COUT is driven by the required effective

series resistance (ESR). Typically, once the ESR

requirement for COUT has been met, the RMS current

rating generally far exceeds the IRIPPLE(P-P)

requirement. The output ripple DVOUT is determined by:

where f = operating frequency, COUT = output

capacitanceand DIL = ripple current in the inductor. For a

fixed output voltage, the output ripple is highest at

maximum input voltage since DIL increases with input

voltage.

Aluminum electrolytic and dry tantalum capacitors are

both available in surface mount configurations. In the

case of tantalum, it is critical that the capacitors are

surge tested for use in switching power supplies. An

excellent choice is the AVX TPS series of surface mount

tantalum. These are specially constructed and tested for

low ESR so they give the lowest ESR for a given volume.

Other capacitor types include Sanyo POSCAP, Kemet

T510 and T495 series, and Sprague 593D and 595D

series. Consult the manufacturer for other specific

recommendations.

Function Description(Cont.)

Using Ceramic Input and Output Capacitors

Higher values, lower cost ceramic capacitors are now becoming available in smaller case sizes. Their high ripple current, high voltage rating and low ESR make them ideal for switching regulator applications. Because the TD6810’s control loop does not depend on the output capacitor’s ESR for stable operation, ceramic capacitors can be used freely to achieve very low output ripple and small circuit size.

However, care must be taken when ceramic capacitors are used at the input and the output. When a ceramic capacitor is used at the input and the power is supplied by a wall adapter through long wires, a load step at the output can induce ringing at the input, VIN. At best, this ringing can couple to the output and be mistaken as loop instability. At worst, a sudden inrush of current through the long wires can potentially cause a voltage spike at VIN, large enough to damage the part.

When choosing the input and output ceramic capacitors, choose the X5R or X7R dielectric formulations. These dielectrics have the best temperature and voltage characteristics of all the ceramics for a given value and size.

Output Voltage Programming

In the adjustable version, the output voltage is set by a resistive divider according to the following formula:

The external resistive divider is connected to the output, allowing remote voltage sensing as shown in Figure4.

Figure 4:Setting the output Voltage

Vout R1 R2

1.2V 150K 150K

1.5V

160K 240K

1.8V 150K 300K

2.5V 150K 470K

3.3V 150K 680K

Table 2. Vout VS. R1, R2, Cf Select Table Efficiency Considerations

The efficiency of a switching regulator is equal to the output power divided by the input power times 100%. It is often useful to analyze individual losses to determine what is limiting the efficiency and which change would produce the most improvement. Efficiency can be expressed as:

Efficiency = 100% – (L1 + L2 + L3 + ...)

where L1, L2, etc. are the individual losses as a percentage of input power.

Although all dissipative elements in the circuit produce losses, two main sources usually account for most of the losses in TD6810 circuits: VIN quiescent current and I2R losses. The VIN quiescent current loss dominates the efficiency loss at very low load currents whereas the I2R loss dominates the efficiency loss at medium to high load currents. In a typical efficiency plot, the efficiency curve at very low load currents can be misleading since the actual power lost is of no consequence as illustrated in Figure 5.

Function Description(Cont.)

Figure 4:Power Lost VS Load Current

1. The VIN quiescent current is due to two components: the DC bias current as given in the electrical characteristics and the internal main switch and synchronous switch gate charge currents. The gate charge current results from switching the gate capacitance of the internal power MOSFET switches. Each time the gate is switched from high to low to high again, a packet of charge, dQ, moves from VIN to ground. The resulting dQ/dt is the current out of VIN that is typically larger than

the DC bias current. In continuous mode, IGATECHG

=f(QT + QB) where QT and QB are the gate charges of the internal top and bottom switches. Both the DC bias and gate charge losses are proportional to VIN and thustheir effects will be more pronounced at higher supply voltages.

2. I2R losses are calculated from the resistances of the internal switches, RSW, and external inductor RL. In continuous mode, the average output current flowing through inductor L is “chopped” between the main switch and the synchronous switch. Thus, the series resistance looking into the SW pin is a function of both top and bottom MOSFET RDS(ON) and the duty cycle (DC) as follows: RSW = (RDS(ON)TOP)(DC) + (RDS(ON)BOT)(1 – DC) The RDS(ON) for both the top and bottom MOSFETs can be obtained from the Typical Performance Charateristics curves. Thus, to obtain I2R losses, simply add RSW to RL and multiply the result by the square of the average output current. Other losses including CIN and COUT ESR dissipative losses and inductor core losses generally account for less than 2% total additional loss.

Thermal Considerations

In most applications the TD6810 does not dissipate much heat due to its high efficiency. But, in applications where the TD6810 is running at high ambient temperature with low supply voltage and high duty cycles, such as in dropout, the heat dissipated may exceed the maximum junction temperature of the part. If the junction temperature reaches approximately 150°C, both power switches will be turned off and the SW node will become high impedance.

To avoid the TD6810 from exceeding the maximum junction temperature, the user will need to do some thermal analysis. The goal of the thermal analysis is to determine whether the power dissipated exceeds the maximum junction temperature of the part. The temperature rise is given by:

TR = (PD)(qJA)

where PD is the power dissipated by the regulator and qJA is the thermal resistance from the junction of the die to the ambient temperature.

The junction temperature, TJ, is given by:

TJ = TA + TR

where TA is the ambient temperature.

As an example, consider the TD6810 in dropout at an input voltage of 2.7V, a load current of 800mA and an ambient temperature of 70°C. From the typical performance graph of switch resistance, the RDS(ON) of the P-channel switch at 70°C is approximately 0.52W.

Function Description(Cont.)

Therefore,

power dissipated by the part is:

PD = ILOAD 2 ? RDS(ON) = 187.2mW

For the SOT-23 package, the qJA is 250°C/ W. Thus, the

junction temperature of the regulator is:

TJ = 70°C + (0.1872)(250) = 116.8°C

which is below the maximum junction temperature of

125°C.

Note that at higher supply voltages, the junction

temperature is lower due to reduced switch resistance

(RDS(ON)).

Checking Transient Response

The regulator loop response can be checked by looking

at the load transient response. Switching regulators take

several cycles to respond to a step in load current. When

a load step occurs, VOUT immediately shifts by an

amount equal to (ΔILOAD ? ESR), where ESR is the

effective series resistance of COUT. ΔILOAD also begins

to charge or discharge COUT, which generates a

feedback error signal. The regulator loop then acts to

return VOUT to its steadystate value. During this

recovery time VOUT can be monitored for overshoot or

ringing that would indicate a stability problem.

A second, more severe transient is caused by switching

in loads with large (>1μF) supply bypass capacitors. The

discharged bypass capacitors are effectively put in

parallel with COUT, causing a rapid drop in VOUT. No

regulator can deliver enough current to prevent this

problem if the load switch resistance is low and it is

driven quickly. The only solution is to limit the rise time of

the switch drive so that the load rise time is limited to

approximately (25 ? CLOAD).Thus, a 10μF capacitor

charging to 3.3V would require a 250μs rise time, limiting

the charging current to about 130mA.

Package Information

TSOT23-5 Package Outline Dimensions

Design Notes

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英文论文及中文翻译

International Journal of Minerals, Metallurgy and Materials Volume 17, Number 4, August 2010, Page 500 DOI: 10.1007/s12613-010-0348-y Corresponding author: Zhuan Li E-mail: li_zhuan@https://www.sodocs.net/doc/1119231141.html, ? University of Science and Technology Beijing and Springer-Verlag Berlin Heidelberg 2010 Preparation and properties of C/C-SiC brake composites fabricated by warm compacted-in situ reaction Zhuan Li, Peng Xiao, and Xiang Xiong State Key Laboratory of Powder Metallurgy, Central South University, Changsha 410083, China (Received: 12 August 2009; revised: 28 August 2009; accepted: 2 September 2009) Abstract: Carbon fibre reinforced carbon and silicon carbide dual matrix composites (C/C-SiC) were fabricated by the warm compacted-in situ reaction. The microstructure, mechanical properties, tribological properties, and wear mechanism of C/C-SiC composites at different brake speeds were investigated. The results indicate that the composites are composed of 58wt% C, 37wt% SiC, and 5wt% Si. The density and open porosity are 2.0 g·cm–3 and 10%, respectively. The C/C-SiC brake composites exhibit good mechanical properties. The flexural strength can reach up to 160 MPa, and the impact strength can reach 2.5 kJ·m–2. The C/C-SiC brake composites show excellent tribological performances. The friction coefficient is between 0.57 and 0.67 at the brake speeds from 8 to 24 m·s?1. The brake is stable, and the wear rate is less than 2.02×10?6 cm3·J?1. These results show that the C/C-SiC brake composites are the promising candidates for advanced brake and clutch systems. Keywords: C/C-SiC; ceramic matrix composites; tribological properties; microstructure [This work was financially supported by the National High-Tech Research and Development Program of China (No.2006AA03Z560) and the Graduate Degree Thesis Innovation Foundation of Central South University (No.2008yb019).] 温压-原位反应法制备C / C-SiC刹车复合材料的工艺和性能 李专,肖鹏,熊翔 粉末冶金国家重点实验室,中南大学,湖南长沙410083,中国(收稿日期:2009年8月12日修订:2009年8月28日;接受日期:2009年9月2日) 摘要:采用温压?原位反应法制备炭纤维增强炭和碳化硅双基体(C/C-SiC)复合材

C语言中英文翻译资料

一.C语言关键字对照 关键字,又称保留字,是C语言中已预先定义、具有特定含义的标识符。 注:C语言中共有32个关键字,所有关键字都用小写字母表示,且这些关键字不能用作用户标识符。即关键字由系统定义,具有特定的含义,不能重作其它定义。 32个关键字如下: 1.数据定义 C语言中所有的变量都具有某种类型,其定义的基本格式是:类型变量名; int:整型 short:短整型 long:长整型 signed:有符号型 unsigned:无符号型 char:字符型 float:单精度型 double:双精度型 const:定义常量 typedef:类型定义 2.存储类别 一般在变量的定义前面,用于指定变量的存储类别,如果缺省的话,则默认是auto。 auto:自动变量 static:静态变量 register:寄存器变量 extern:外部变量 3.结构 C语言中除了提供一些基本数据类型外,还提供了结构体,共有体以及枚举,用来实现多个变量的集合表示。 struct:结构体 union:共用体 enum:枚举类型 4.语句 C语言中提供了一些语句来实现程序的基本结构。 if:条件判断(假如) else:不满足条件(否则) for:循环 do:与while一起使用,直到型循环 while:当型循环 goto:无条件跳转语句 switch:多分支选择语句 case:分支,在switch语句块中表示不同的分支

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韶关学院 期末考核报告 科目:专业英语 学生姓名: 学号: 同组人: 院系: 专业班级: 考核时间:2012年10月9日—2012年11月1 日评阅教师: 评分:

第1章英文阅读材料翻译 (1) 第2章中文摘要翻译英文 (3) 第3章中文简历和英文简历 (4) 第4章课程学习体会和建议 (6) 参考文献 (7)

第1章英文阅读材料翻译 Mechanization and Automation Processes of mechanization have been developing and becoming more complex ever since the beginning of the Industrial Revolution at the end of the 18th century. The current developments of automatic processes are, however, different from the old ones. The “automation” of the 20th century is distinct from the mechanization of the 18th and 19th centuries inasmuch as mechanization was applied to individual operations, wherea s “automation” is concerned with the operation and control of a complete producing unit. And in many, though not all, instances the element of control is so great that whereas mechanization displaces muscle, “automation”displaces brain as well. The distinction between the mechanization of the past and what is happening now is, however, not a sharp one. At one extreme we have the electronic computer with its quite remarkable capacity for discrimination and control, while at the other end of the scale are “ transfer machines” , as they are now called, which may be as simple as a conveyor belt to another. An automatic mechanism is one which has a capacity for self-regulation; that is, it can regulate or control the system or process without the need for constant human attention or adjustment. Now people often talk about “feedback” as begin an essential factor of the new industrial techniques, upon which is base an automatic self-regulating system and by virtue of which any deviation in the system from desired condition can be detected, measured, reported and corrected. when “feedback” is applied to the process by which a large digital computer runs at the immense speed through a long series of sums, constantly rejecting the answers until it finds one to fit a complex set of facts which have been put to it, it is perhaps different in degree from what we have previously been accustomed to machines. But “feedback”, as such, is a familiar mechanical conception. The old-fashioned steam engine was fitted with a centrifugal governor, two balls on levers spinning round and round an upright shaft. If the steam pressure rose and the engine started to go too fast, the increased speed of the spinning governor caused it to rise up the vertical rod and shut down a valve. This cut off some of the steam and thus the engine brought itself back to its proper speed. The mechanization, which was introduced with the Industrial Revolution, because it was limited to individual processes, required the employment of human labor to control each machine as well as to load and unload materials and transfer them from one place to another. Only in a few instances were processes automatically linked together and was production organized as a continuous flow. In general, however, although modern industry has been highly mechanized ever since the 1920s, the mechanized parts have not as a rule been linked together. Electric-light bulbs, bottles and the components of innumerable mass-produced

机械专业外文翻译(中英文翻译)

外文翻译 英文原文 Belt Conveying Systems Development of driving system Among the methods of material conveying employed,belt conveyors play a very important part in the reliable carrying of material over long distances at competitive cost.Conveyor systems have become larger and more complex and drive systems have also been going through a process of evolution and will continue to do so.Nowadays,bigger belts require more power and have brought the need for larger individual drives as well as multiple drives such as 3 drives of 750 kW for one belt(this is the case for the conveyor drives in Chengzhuang Mine).The ability to control drive acceleration torque is critical to belt conveyors’performance.An efficient drive system should be able to provide smooth,soft starts while maintaining belt tensions within the specified safe limits.For load sharing on multiple drives.torque and speed control are also important considerations in the drive system’s design. Due to the advances in conveyor drive control technology,at present many more reliable.Cost-effective and performance-driven conveyor drive systems covering a wide range of power are available for customers’ choices[1]. 1 Analysis on conveyor drive technologies 1.1 Direct drives Full-voltage starters.With a full-voltage starter design,the conveyor head shaft is direct-coupled to the motor through the gear drive.Direct full-voltage starters are adequate for relatively low-power, simple-profile conveyors.With direct fu11-voltage starters.no control is provided for various conveyor loads and.depending on the ratio between fu11-and no-1oad power requirements,empty starting times can be three or four times faster than full load.The maintenance-free starting system is simple,low-cost and very reliable.However, they cannot control starting torque and maximum stall torque;therefore.they are

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