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LT1105IN Datasheet(PDF) 21 Page - Linear Technology |
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LT1105IN Datasheet(HTML) 21 Page - Linear Technology |
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21 / 32 page ![]() 21 LT1103/LT1105 to zero or changing polarity. Therefore, the voltage on the bias winding is only valid as a representation of the output voltage while the secondary is delivering current. Although the bias winding flyback voltage is a representa- tion of the output voltage, its voltage is not constant. For a brief period following the leakage inductance spike, the bias winding flyback voltage decreases due to nonlinearities and parasitics present in the transformer. Following this nonlinear behavior is a period where the bias winding flyback voltage decreases linearly. This behavior is easily explained. Current flow in the secondary decreases lin- early at a rate determined by the voltage across the secondary and the inductance of the secondary. The parasitic secondary leakage inductance appears as an impedance in series with the secondary winding. In addi- tion, parasitic resistances exist in the secondary winding, the output diode and the output capacitor. These imped- ances can be combined to form a lumped sum equivalent and which cause a voltage drop as secondary current flows. This voltage drop is coupled from the secondary to the bias winding flyback voltage and becomes more sig- nificant as the output is loaded more heavily. This voltage drop is largest at the beginning of “switch off” time and smallest just prior to either all transformer energy being depleted or the switch turning on again. The best representation of the output voltage is just prior to either all transformer energy being used up and the bias winding voltage collapsing to zero or just prior to the switch turning on again and the bias winding going negative. This point in time also represents the smallest forward voltage for the output diode. It is possible to redefine the relationship between the secondary winding voltage and the bias winding voltage as: V VVf I • R N1 BIAS OUT P = ++ () where Vf is the forward voltage of the output diode, I is the current flowing in the secondary, RP is the lumped sum equivalent secondary parasitic impedance and N1 is the transformer turns ratio from the secondary to the bias winding. It is apparent that even though the above point in APPLICATIONS INFORMATION voltage, the secondary voltage, the bias voltage and the winding currents are indicated in the figures found on the following page for both continuous and discontinuous modes of operation. Simplified Flyback Converter D1 1:N LT1103 AI01 VBIAS S1 R L(lkSEC) VOUT C1 COMMON L(IkPRI) VIN 1:N1 N = TURNS RATIO FROM SECONDARY TO PRIMARY. N1 = TURNS RATIO FROM SECONDARY TO BIAS. N2 = N/N1 L(lkPRI) = PRIMARY LEAKAGE INDUCTANCE. L(lkSEC) = SECONDARY LEAKAGE INDUCTANCE. R = PARASITIC WINDING, DIODE AND OUTPUT CAPACITOR RESISTANCE. When the switch “turns on,” the primary winding sees the input voltage and the secondary and bias windings go to negative voltages as a function of the turns ratio. Current builds in the primary winding as the transformer stores energy. When the switch “turns off,” the voltage across the switch flies back to a clamp level as defined by a snubber network until the energy in the leakage induc- tance of the primary dissipates. Leakage inductance is one of the main parasitic elements in a flux-sensed converter and is modeled as an inductor in series with the primary and secondary of the transformer. These parasitic induc- tances contribute to changes in the bias winding voltage and thus the output voltage with increasing load current. The energy stored in the transformer transfers through the secondary and bias windings during “switch off” time. Ideally, the voltage across the bias winding is set by the DC output voltage, the forward voltage of the output diode, and the turns ratio of the transformer after the energy in the leakage inductance spike of the primary is dissipated. This relationship holds until the energy in the transformer drops to zero (discontinuous mode) or the switch turns on again (continuous mode). Either case results in the volt- age across the secondary and bias windings decreasing |
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