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LTC3633 датащи(PDF) 12 Page - Linear Technology |
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LTC3633 датащи(HTML) 12 Page - Linear Technology |
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12 / 28 page ![]() LTC3633 12 3633f APPLICATIONS INFORMATION A general LTC3633 application circuit is shown on the first page of this data sheet. External component selection is largely driven by the load requirement and switching frequency. Component selection typically begins with the selection of the inductor L and resistor RT. Once the inductor is chosen, the input capacitor, CIN, and the out- put capacitor, COUT, can be selected. Next, the feedback resistors are selected to set the desired output voltage. Finally, the remaining optional external components can be selected for functions such as external loop compensation, track/soft-start, VIN UVLO, and PGOOD. Programming Switching Frequency Selection of the switching frequency is a trade-off between efficiency and component size. High frequency operation allows the use of smaller inductor and capacitor values. Operation at lower frequencies improves efficiency by reducing internal gate charge losses but requires larger inductance values and/or capacitance to maintain low output ripple voltage. Connecting a resistor from the RT pin to SGND programs the switching frequency (f) between 500kHz and 4MHz according to the following formula: RRT = 3.2E 11 f where RRT is in Ω and f is in Hz. When RT is tied to INTVCC, the switching frequency will default to approximately 2MHz, as set by an internal re- sistor. This internal resistor is more sensitive to process and temperature variations than an external resistor (see Typical Performance Characteristics) and is best used for applications where switching frequency accuracy is not critical. Inductor Selection For a given input and output voltage, the inductor value and operating frequency determine the inductor ripple current. More specifically, the inductor ripple current decreases with higher inductor value or higher operating frequency according to the following equation: IL = VOUT f• L 1– VOUT VIN Where ΔIL=inductorripplecurrent,f=operatingfrequency and L = inductor value. A trade-off between component size, efficiency and operating frequency can be seen from this equation. Accepting larger values of ΔIL allows the use of lower value inductors but results in greater inductor core loss, greater ESR loss in the output capacitor, and larger output voltage ripple. Generally, highest efficiency operation is obtained at low operating frequency with small ripple current. A reasonable starting point is to choose a ripple current that is about 40% of IOUT(MAX). Note that the largest ripple current occurs at the highest VIN. Exceeding 60% of IOUT(MAX) is not recommended. To guarantee that ripple current does not exceed a specified maximum, the inductance should be chosen according to: L = VOUT f• IL(MAX) 1– VOUT VIN(MAX) Once the value for L is known, the type of inductor must be selected. Actual core loss is independent of core size for a fixed inductor value, but is very dependent on the inductance selected. As the inductance increases, core losses decrease. Unfortunately, increased inductance requires more turns of wire, leading to increased DCR and copper loss. 0 1000 2000 3000 5000 200 700 600 3633 F01 0 6000 4000 100 300 400 500 RT RESISTOR (kΩ) Figure 1. Switching Frequency vs RT |
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