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RT8011APF Datasheet(PDF) 13 Page - Richtek Technology Corporation |
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RT8011APF Datasheet(HTML) 13 Page - Richtek Technology Corporation |
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13 / 17 page ![]() RT8011/A 13 DS8011/A-00 August 2006 www.richtek.com Efficiency Considerations The efficiency of a switching regulator is equal to the output power divided by the input power times 100%. It is often useful to analyze individual losses to determine what is limiting the efficiency and which change would produce the most improvement. Efficiency can be expressed as : Efficiency = 100% − (L1+ L2+ L3+ ...) where L1, L2, etc. are the individual losses as a percentage of input power. Although all dissipative elements in the circuit produce losses, two main sources usually account for most of the losses: VDD quiescent current and I 2R losses. The VDD quiescent current loss dominates the efficiency loss at very low load currents whereas the I2R loss dominates the efficiency loss at medium to high load currents. In a typical efficiency plot, the efficiency curve at very low load currents can be misleading since the actual power lost is of no consequence. 1. The VDD quiescent current is due to two components : the DC bias current as given in the electrical characteristics and the internal main switch and synchronous switch gate charge currents. The gate charge current results from switching the gate capacitance of the internal power MOSFET switches. Each time the gate is switched from high to low to high again, a packet of charge ΔQ moves from VDD to ground. The resulting ΔQ/Δt is the current out of VDD that is typically larger than the DC bias current. In continuous mode, IGATECHG= f(QT+QB) where QT and QB are the gate charges of the internal top and bottom switches. Both the DC bias and gate charge losses are proportional to VDD and thus their effects will be more pronounced at higher supply voltages. 2. I2R losses are calculated from the resistances of the internal switches, RSW and external inductor RL. In continuous mode the average output current flowing through inductor L is “chopped” between the main switch and the synchronous switch. Thus, the series resistance looking into the LX pin is a function of both top and bottom MOSFET RDS(ON) and the duty cycle (D) as follows : RSW = RDS(ON)TOP x D + RDS(ON)BOT x (1"D) The RDS(ON) for both the top and bottom MOSFETs can be obtained from the Typical Performance Characteristics curves. Thus, to obtain I2R losses, simply add RSW to RL and multiply the result by the square of the average output current. Other losses including CIN and COUT ESR dissipative losses and inductor core losses generally account for less than 2% of the total loss. Thermal Considerations In most applications, the RT8011/A does not dissipate much heat due to its high efficiency. But, in applications where the RT8011/A is running at high ambient temperature with low supply voltage and high duty cycles, such as in dropout, the heat dissipated may exceed the maximum junction temperature of the part. If the junction temperature reaches approximately 150 °C, both power switches will be turned off and the SW node will become high impedance. To avoid the RT8011/A from exceeding the maximum junction temperature, the user will need to do some thermal analysis. The goal of the thermal analysis is to determine whether the power dissipated exceeds the maximum junction temperature of the part. The temperature rise is given by : TR = PD x θJA Where PD is the power dissipated by the regulator and θJA is the thermal resistance from the junction of the die to the ambient temperature. The junction temperature, TJ, is given by : TJ = TA + TR Where TA is the ambient temperature. As an example, consider the RT8011/A in dropout at an input voltage of 3.3V, a load current of 2A and an ambient temperature of 70 °C. From the typical performance graph of switch resistance, the RDS(ON) of the P-Channel switch at 70 °C is approximately 121mΩ. Therefore, power dissipated by the part is : PD = (ILOAD) 2 (RDS(ON)) = (2A)2 (121m Ω) = 0.484W For the DFN3x3 package, the θJA is 110°C/W. Thus the junction temperature of the regulator is : TJ = 70 °C + (0.484W) (110 °C/W) = 123.24°C Which is below the maximum junction temperature of 125 °C. Note that at higher supply voltages, the junction temperature is lower due to reduced switch resistance (RDS(ON)). Checking Transient Response The regulator loop response can be checked by looking at the load transient response. Switching regulators take several cycles to respond to a step in load current. When a load step occurs, VOUT immediately shifts by an amount equal to ΔILOAD(ESR), where ESR is the effective series |
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