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MIC3232 Datasheet(PDF) 14 Page - Micrel Semiconductor |
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MIC3232 Datasheet(HTML) 14 Page - Micrel Semiconductor |
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14 / 19 page ![]() Micrel, Inc. MIC3230/1/2 November 2009 14 M9999-113009-B (see the current waveforms in Figure 5). It can be difficult to find large inductor values with high saturation currents in a surface mount package. Due to this, the percentage of the ripple current may be limited by the available inductor. It is recommended to operate in the continuous conduction mode. The selection of L described here is for continuous conduction mode. Eq. (13) PP in IN I T D V L _ × × = Using the nominal values, we get: H A s V L μ μ 43 31 . 0 2 56 . 0 12 = × × = Select the next higher standard inductor value of 47µH. Going back and calculating the actual ripple current gives: Eq. (13a) PP nom nom IN PP in A uh us v L T D V I 29 . 0 47 2 56 . 0 12 _ _ = × × = × × = The average input current is different than the RMS input current because of the ripple current. If the ripple current is low, then the average input current nearly equals the RMS input current. In the case where the average input current is different than the RMS, Equation 10 shows the following: Eq. (13b) () ( ) 12 2 _ 2 max _ _ max _ _ PP IN RMS IN AVE IN I I I − = () ( ) A I AVE IN 64 . 1 12 / 29 . 0 64 . 1 2 2 max _ _ ≈ − = The Maximum Peak input current IL_PK can found using equation 11: A I I I PP L AVE IN PK L 78 . 1 5 . 0 max _ _ max _ _ max _ _ = × + = The saturation current (ISAT) at the highest operating temperature of the inductor must be rated higher than this. The power dissipated in the inductor is: Eq. (13c) DCR I P RMS in INDUCTOR × = 2 max _ _ Current Limit and Slope Compensation Having calculated the IL_pk above, We can set the current limit 20% above this maximum value: A A I Limit pk L 9 . 1 6 . 1 2 . 1 _ = × = The internal current limit comparator reference is set at 0.45V, therefore when 45 . 0 _ = PIN IS V , the IC enters current limit. Eq. (14) ( ) PK A Vcs V PK + = 45 . 0 Where PK A V is the peak of the A V waveform and PK Vcs is the peak of the Vcs waveform Eq. (14a) CS pk L SLC RAMP R I D R I Limit × + × × = _ 45 . 0 To calculate the value of the slope compensation resistance, RSLC, we can use Equation 5: ( ) SW CS IN OUT SLC F A L R V V R MIN MAX × × × − = μ 250 First we must calculate RCS, which is given below in Equation 15: Eq. (15) () Limit pk L SW MIN MAX CS I F L D VIN VOUT R _ max 45 . 0 + × × − = Therefore; () ( ) Ω = + × × − = m A kHz H v v RCS 179 9 . 1 500 47 50 . 0 8 28 45 . 0 μ Using a standard value 150mΩ resistor for RCS, we obtain the following for RSLC: ( ) Ω = × × Ω × − = 511 500 250 47 150 8 28 kHz A H m RSLC μ μ Use the next higher standard value if this not a standard value. In this example 511Ω is a standard value. Check: Because we must use a standard value for Rcs and RSLC; Limit pk L I _ may be set at a different level (if the calculated value isn’t a standard value) and we must calculate the actual Limit pk L I _ value (remember Limit pk L I _ is the same as Limit pk in I _ ). Rearranging Equation 14a to solve for Limit pk L I _ : CS SLC RAMP pk in R D R I I Limit ) 45 . 0 ( _ × × − = A ua I Limit actual in 34 . 2 150 . ) 75 . 0 511 250 45 . 0 ( _ = × × − = This is higher than the initial A I PK L 9 . 1 2 . 1 max _ _ = × limit because we have to use standard values for RCS and for RSLC. If Limit actual in I _ is too high than use a higher value for RCS. The calculated value of RCS for a 1.9A current limit was 179mΩ. In this example, we have chosen a lower value which results in a higher current limit. If we use a higher standard value the current limit will have a lower value. The designer does not have the same choices for small valued resistors as with larger valued resistors. The choices differ from resistor manufacturers. If too large a current sense resistor is selected, the maximum output power may not be able to be achieved at low input line voltage levels. Make sure the inductor will not saturate at the actual current limit Limit actual in I _ . Perform a check at IIN=2.34Apk. ( ) V m A A V PIN IS 45 . 0 150 34 . 2 511 78 . 0 250 _ = Ω × + Ω × × = μ |
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