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LT1683 Datasheet(PDF) 13 Page - Linear Technology |
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LT1683 Datasheet(HTML) 13 Page - Linear Technology |
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13 / 24 page ![]() 13 LT1683 1683f APPLICATIO S I FOR ATIO Reducing EMI from switching power supplies has tradi- tionally invoked fear in designers. Many switchers are designed solely on efficiency and as such produce wave- forms filled with high frequency harmonics that then propagate through the rest of the system. The LT1683 provides control over two of the more impor- tant variables for controlling EMI with switching inductive loads: switch voltage slew rate and switch current slew rate. The use of this part will reduce noise and EMI over conventional switch mode controllers. Because these variables are under control, a supply built with this part will exhibit far less tendency to create EMI and less chance of encountering problems during production. It is beyond the scope of this data sheet to get into EMI fundamentals. Application Note 70 contains much infor- mation concerning noise in switching regulators and should be consulted. Oscillator Frequency The oscillator determines the switching frequency and therefore the fundamental positioning of all harmonics. The use of good quality external components is important to ensure oscillator frequency stability. The oscillator is of a sawtooth design. A current defined by external resistor RT is used to charge and discharge the capacitor CT . The discharge rate is approximately ten times the charge rate. By allowing the user to have control over both compo- nents, trimming of oscillator frequency can be more easily achieved. The external capacitance CT is chosen by: CnF f kHz R k T T () ()• ( ) = Ω 2180 where f is the desired oscillator frequency in kHz. For RT equal to 16.9k, this simplifies to: CnF f kHz T () () = 129 e.g., CT = 1.29nF for f = 100kHz Nominally RT should be 16.9k. Since it sets up current, its temperature coefficient should be selected to compliment the capacitor. Ideally, both should have low temperature coefficients. Oscillator frequency is important for noise reduction in two ways. First the lower the oscillator frequency the lower the waveform’s harmonics, making it easier to filter them. Second the oscillator will control the placement of the output voltage harmonics which can aid in specific prob- lems where you might be trying to avoid a certain fre- quency bandwidth. Oscillator Sync If a more precise frequency is desired (e.g., to accurately place harmonics) the oscillator can be synchronized to an external clock. Set the RC timing components for an oscillator frequency 10% lower than the desired sync frequency. Drive the SYNC pin with a square wave (with greater than 1.4V amplitude). The rising edge of the sync square wave will initiate clock discharge. The sync pulse should have a minimum pulse width of 0.5 µs. Be careful in sync’ing to frequencies much different from the part since the internal oscillator charge slope deter- mines slope compensation. It would be possible to get into subharmonic oscillation if the sync doesn’t allow for the charge cycle of the capacitor to initiate slope compensa- tion. In general, this will not be a problem until the sync frequency is greater than 1.5 times the oscillator free-run frequency. Slew Rate Setting The primary reason to use this part is to gain advantage of lower EMI and noise due to slew control. The rolloff in higher frequency harmonics has its theoretical basis with two primary components. First, the clock frequency sets the fundamental positioning of harmonics and second, the associated normal frequency rolloff of harmonics. |
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