RH5RH
When the output current (IOUT) is relatively small, topen<toff as illustrated in the above diagram. In this case, the energy charged in the inductor during the time period of ton is discharged in its entirely during the time period of toff, so that ILmin becomes zero (ILmin=0). When IOUT is gradually increased, topen eventually becomes equal to toff (topen=toff), and when IOUT is further increased. ILmin becomes larger than zero (ILmin>0). The former mode is referred to as the discontinuous mode and the latter mode is referred to as the continuous mode.
In the continuous mode, when Equation 1 is solved for ton and the solution is tonc,
tonc =T ·
When ton<tonc, the mode is the discontinuous mode, and when ton=tonc, the mode is the continuous mode.
•Output Current in Discontinuous Mode
In the discontinuous mode, when LxTr is on, the energy PON charged in the inductor is provided by Equation 3 as follows :
PON=∫ 0ton VIN · IL (t) dt =∫ 0ton (VIN2 · t/L) dt
=VIN2 · ton2/(2 · L).................................................................................................Equation 3
In the case of the
Thus, POFF=∫0topen VIN · IL (t) dt =∫0topen
Here, topen=VIN ·
3 | 2 | .......................................................................... |
=VIN | · ton /(2 · L · | Equation 4 |
Input power is (PON+POFF)/T. When this is converted in its entirely to the output.
PIN=(PON+POFF)/T=VOUT · IOUT=POUT | ..................................................................... |
Equation 5 |
Equation 6 can be obtained as follows by solving Equation 5 for IOUT by substituting Equations 3 and 4 into Equation 5 :
IOUT=VIN2 · ton2/(2 · L · T ·
The peak current which flows through L · LxTr · SD is
ILmax=VIN · ton/L ......................................................................................................Equation 7
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