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LT1680ISW Datenblatt(PDF) 12 Page - Linear Technology |
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LT1680ISW Datenblatt(HTML) 12 Page - Linear Technology |
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12 / 16 page ![]() 12 LT1680 APPLICATIONS INFORMATION ments. Generally, the selection of inductor value can be reduced to desired maximum ripple current in the inductor ( ∆I). For a boost converter, the minimum inductor value for a given operating ripple current can be determined using the following relation: L VV V If V MIN IN OUT IN O OUT = () ()( )( ) – ∆ Given an inductor value (L), the peak inductor current is the sum of the average inductor current (IAVG) and half the inductor ripple current ( ∆I), or: II VV V Lf V PK AVG IN OUT IN O OUT =+ () ()()( )( ) – 2 The inductor core type is determined by peak current and efficiency requirements. The inductor core must with- stand this peak current without saturating, and the series winding resistance and core losses should be kept as small as is practical to maximize conversion efficiency. The LT1680 peak current threshold is 40% greater than the average limit threshold. Slope compensation effects reduce this margin as duty cycle increases. This margin must be maintained to prevent peak current limit from corrupting the programmed value for average current limit. Programming the peak ripple current to less than 15% of the desired average current limit value will assure proper operation of the average current limit feature through 90% duty cycle (see Slope Compensation). Slope Compensation Current mode switching regulators that operate with a duty cycle greater than 50% and have continuous inductor current can exhibit duty cycle instability. While a regulator will not be damaged and may even continue to function acceptably during this type of subharmonic oscillation, an irritating high-pitched squeal is usually produced. The criterion for current mode duty cycle instability is met when the increasing slope of the inductor ripple current is less than the decreasing slope, which is the case at duty cycles greater than 50%. This condition is illustrated in Figure 9a. The inductor ripple current starts at I1, the beginning of each oscillator switch cycle. Current increases at a rate S1 until the current reaches the control trip level I2. The controller servo loop then disables the switch and inductor current begins to de- crease at a rate S2. If the current switch point (I2) is perturbed slightly and increased by ∆I, the cycle time ends such that the minimum current point is increased by a factor of 1 + (S2/S1) to start the next cycle. On each successive cycle, this error is multiplied by a factor of S2/ S1. Therefore, if S2/S1 is ≥1, the system is unstable. Subharmonic oscillations can be eliminated by augment- ing the increasing ripple current slope (S1) in the control loop. This is accomplished by adding an artificial ramp on the inductor current waveform internal to the IC (with a slope SX) as shown in Figure 9b. If the sum of the slopes S1 + SX is greater than S2, this condition for subharmonic oscillation no longer exists. OSCILLATOR PERIOD TIME 0 0 ab ∆I T1 I2 I1 S1 S1 S2 S2 S1 + SX 1680 F09 Figure 9. Inductor Current at DC > 50% and Slope Compensation Adjusted Signal For boost topologies, the required additional current wave- form slope, or “Slope Compensation,” follows the relation: S SDC DC X ≥ ()( ) () 12 1 1 – – For duty cycles less than 50% (DC < 0.5), SX is negative and is not required. For duty cycles greater than 50%, SX takes on values dependent on S1 and duty cycle. S1 is simply VIN/ L. This leads to a minimum inductance requirement for a given VIN, duty cycle and slope compensation (SX) of: L V S DC DC MIN IN X = () 21 1 – – The LT1680 contains an internal slope compensation ramp that has an equivalent current referred value of: |
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