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LT3435EFE датащи(PDF) 21 Page - Linear Technology |
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LT3435EFE датащи(HTML) 21 Page - Linear Technology |
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21 / 24 page ![]() LT3435 21 3435fa APPLICATIO S I FOR ATIO Example: with VIN = 25V, VOUT = 5V and IOUT = 2A: Pe e PW PW SW BOOST Q = ( )()() + ()()()( )( ) += = () () = = ()+ ()= 015 2 5 25 77 12 2 25 500 3 012 0962 108 5240 40 003 40 0 0026 5 0 001 0 11 2 9 2 . / .. . / . .. . – Total power dissipation is: PTOT = 1.08 + 0.03+ 0.11 = 1.22W Thermal resistance for the LT3435 package is influenced by the presence of internal or backside planes. With a full plane under the FE16 package, thermal resistance will be about 45 °C/W. No plane will increase resistance to about 150 °C/W. To calculate die temperature, use the proper thermal resistance number for the desired package and add in worst-case ambient temperature: TJ = TA + QJA (PTOT) With the FE16 package (QJA = 45°C/W) at an ambient temperature of 70 °C: TJ = 70 + 45(1.22) = 125°C Input Voltage vs Operating Frequency Considerations The absolute maximum input supply voltage for the LT3435 is specified at 60V. This is based solely on internal semi- conductor junction breakdown effects. Due to internal power dissipation the actual maximum VIN achievable in a particular application may be less than this. A detailed theoretical basis for estimating internal power loss is given in the section Thermal Considerations. Note that AC switching loss is proportional to both operating frequency and output current. The majority of AC switch- ing loss is also proportional to the square of input voltage. For example, while the combination of VIN = 40V, VOUT = 5V at 2A and fOSC = 500kHz may be easily achievable, si- multaneously raising VIN to 60V and fOSC to 700kHz is not possible. Nevertheless, input voltage transients up to 60V can usually be accommodated, assuming the resulting increase in internal dissipation is of insufficient time dura- tion to raise die temperature significantly. A second consideration is controllability. A potential limi- tation occurs with a high step-down ratio of VIN to VOUT, as this requires a correspondingly narrow minimum switch on time. An approximate expression for this (assuming continuous mode operation) is given as follows: tON(MIN) = VOUT + VF/VIN(fOSC) where: VIN = input voltage VOUT = output voltage VF = Schottky diode forward drop fOSC = switching frequency A potential controllability problem arises if the LT3435 is called upon to produce an on time shorter than it is able to produce. Feedback loop action will lower then reduce the VC control voltage to the point where some sort of cycle- skipping or Burst Mode behavior is exhibited. In summary: 1. Be aware that the simultaneous requirements of high VIN, high IOUT and high fOSC may not be achievable in practice due to internal dissipation. The Thermal Con- siderations section offers a basis to estimate internal power. In questionable cases a prototype supply should be built and exercised to verify acceptable operation. 2. The simultaneous requirements of high VIN,lowVOUTand high fOSC can result in an unacceptably short minimum switch on time. Cycle skipping and/or Burst Mode be- havior will result causing an increase in output voltage ripple while maintaining the correct output voltage. FREQUENCY COMPENSATION Before starting on the theoretical analysis of frequency response the following should be remembered—the worse the board layout, the more difficult the circuit will be to stabilize. This is true of almost all high frequency analog circuits. Read the Layout Considerations section first. Common layout errors that appear as stability problems are distant placement of input decoupling capacitor and/or |
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