| 数据搜索系统,热门电子元器件搜索 |
|
LT1319CS 数据表(PDF) 8 Page - Linear Technology |
|
|
|||||||||||||||||||||||||||||
LT1319CS 数据表(HTML) 8 Page - Linear Technology |
|
8 / 12 page ![]() 8 LT1319 APPLICATIONS INFORMATION interaction. Overshoot becomes especially important for high input levels because it can cause false pulses which may not be tolerated in certain modulation schemes. It is also more of a problem in modulation schemes such as IRDA-SIR and FIR where the duty cycle can get very low (i.e., transmitting data with lots of ones which are signaled with the absence of pulses). AC coupled receivers when faced with low duty cycle data set their thresholds close to the baseline DC level of the data stream which converts small overshoots into erro- neously received pulses. 4. As a general rule, place the lowest frequency highpass around the preamp and the highest highpass around the gain stage or between the preamp and gain stage. The reason for this is again due to high signal levels where there can be slow photocurrent tails. The tail response can be filtered out by high enough frequency filters. 5. In all cases with custom filtering, or when modifying one of the applications presented in this data sheet, try the system over the full distance range with a full range of duty cycle data streams. Modulation methods with fixed or limited duty cycle are superior because they have little or no data dependent problems. Dynamic Range The calculation of dynamic range can only be made in the context of a specific modulation scheme and with the system variations taken into account. The required infor- mation includes: minimum signal-to-noise ratio (or BER, Bit Error Rate requirement), photodiode capacitance at 1.9V back bias, preamp noise spectrum, preamp output filtering, AC loop cutoff frequencies, modulation method, demodulation method including allowable pulse widths and the effect of missing or extra pulses, photodiode rise and fall times, and ambient interference. The best solution is to experimentally determine the maximum and minimum distances at which a desired BER is obtained. This measure of dynamic range is more meaningful in terms of the overall system than any analytic solution. Using the IRDA-SIR modulation scheme as an example, however, we can illustrate how some limits on the required receiver/photodiode combination can be obtained. The minimum light intensity in the angular range is 40mW/sr which translates to a photodiode current as follows (using the BPW34FA data sheet specs): ImW sr mm mm AW nA PD MIN () = () () ( )()() = 40 7 1000 0 65 0 95 0 95 164 2 2 /• ./ . . The 7mm2 term is the photodiode area. The 1000mm is the distance from the light source. The 0.65A/W is the spectral sensitivity at 880nm wavelength. The first 0.95 term is the relative sensitivity at 850nm wavelength and the second term is the sensitivity at 15 ° off axis. Similar calculations are detailed in the Infrared Data Association Serial Infrared (SIR) Physical Layer Link Specification, version 1.0. This minimum photocurrent implies that the input-referred noise current of the receiver be less than 13.7nA rms for a bit error rate of 1E-9. With an 800kHz lowpass filter on the preamp output the LT1319 has approximately 3.6nA rms of input-referred current noise. The maximum photodiode current at 20mm, on-axis with 500mW/sr intensity: ImW sr mm mm PD MAX () = () () ()( )= 500 7 20 2 2 /• ./ . . 0 65A W 0 95 5 4mA so we see that the dynamic range requirement is 90.4dB. What is not obvious, however, is that the photodiode output current is not simply a pulse of current, there is a significant tail at high current levels that has a time constant of more than 1 µs which can cause distortion in the output pulse width of the LT1319. This tail can be shown in the following photograph which shows the voltage across a 5k resistor that is connected between the anode of a photo- diode and ground. The cathode of the photodiode is connected to 2V. There is a 2pF Schottky diode across the resistor to clamp the voltage swing to less than 0.5V. With about 30pF photodiode capacitance and 10pF for an oscil- loscope probe, any tail observed with a time constant greater than 210ns is due to decaying photocurrent. The |
|
|
链接网址 |
| ALLDATASHEET是否为您带来帮助? [ DONATE ] |
关于 Alldatasheet | 广告服务 | 联系我们 | 隐私政策 | 数据表链接 | 链接交换 | 制造商名单 All Rights Reserved©Alldatasheet.com |
| Russian : Alldatasheetru.com | Korean : Alldatasheet.co.kr | Spanish : Alldatasheet.es | French : Alldatasheet.fr | Italian : Alldatasheetit.com Portuguese : Alldatasheetpt.com | Polish : Alldatasheet.pl | Vietnamese : Alldatasheet.vn Indian : Alldatasheet.in | Mexican : Alldatasheet.com.mx | British : Alldatasheet.co.uk | New Zealand : Alldatasheet.co.nz |
|
Family Site : ic2ic.com |
icmetro.com |