[Menu]>[Electronic circuit beans collection]>[Switching regulator (2)]>[Step-down converter]
![]() ![]() ![]() ![]() When TR is ON, the input electric power is supplied to the capacitor (C2) and the load through the coil (L1). At this time, the electrical energy is stored up at the coil (L1) and the capacitor (C2). At this time, the side of the input of the coil becomes positive and the side of the output becomes the negative potential. ![]() ![]() ![]() ![]() ![]() The circuit which was made this time used the 470-pF capacitor. In this case, it becomes ton=20µS, toff=3µS. Because it is, the frequency is f = 1/(ton+toff) = 43kHz. I used the value which is mentioned to the sample circuit of the data sheet as the value of the capacitor. I think that the high frequency can do the coil and so on smaller. However, because the high-speed switching made the loss of the switching transistor and the diode big, I used the value of the data sheet. ![]() ![]() The main coil (L1) is preparatory to pass the electric current continuously to the load when TR becomes OFF. The output power with the stable one with the bigger inductance value can be gotten. However, in case of the big inductance value, the high voltage occurs in the both edges of the coil when TR is OFF. As for this voltage, the leveling is done with the capacitor on the side of the output but the ripple increases when the coil is big. I could not understand the calculation formula which finds the inductance value which is mentioned to the data sheet. So, I used the inductance which is near the value of the sample circuit. L(min) = ((Vin(min) - Vsat - Vout) / Ipk(switch) ) x ton(max)
There is an effect in the value of the capacitor in the bigger one. You must consider the use because the size of the capacitor with the big capacity is big and the many inflow electric currents occur. Because the big charging and discharge electric current flows through this capacitor, you use the small one of the ESR(Equivalent Series Resistance). There is a way of connecting the capacitor in parallel as the means of making the ESR small. ![]() ![]() ![]() The over-current is detected by the voltage drop of the resistance which is put in the input circuit in series. The regulator judges the over-current when the voltage difference between Vcc and the over-current detection terminal(Ipk) is more than 0.3 V and limits the supply of electric power to the output. Because I used the 0.22-ohm resistor at the circuit this time, as the input current limiting value, it becomes 0.3V / 0.22ohm = 1.36A. I make the connection between the side of the output of R1 and the 7th pin of the regulator the independent pattern on the printed board. This is to more correctly detect the voltage which is applied to R1. The sheet copper of the printed board is small but has the resistance value. When few electric currents occur, the voltage drop with the printed board can be ignored. Because the over-current detection detects the voltage of the milli-volt, when the electric current is big, the voltage drop of the printed board can not be ignored. I connect the pattern with the side of the output of R1 directly and prevent the influence of the big electric current which flows through the printed wiring. ![]() ![]() ![]() MC34063A compares the reference voltage of 1.25-V and the output voltage and is controlling the output voltage to be constant. The output voltage can be calculated by the following formula.
Vout = ((R2+VR1+R3)/R3)x1.25
At the circuit this time, R2 = 1k-ohm, R3 = 1.5k-ohm, VR1 = 10k-ohm, it changes as follows in the output voltage by the change of VR1.
![]() ![]() ![]() The sample circuit of the data sheet is using the 1µH one as the coil. I used the 25µH one. Because, I could not acquire the coil of 1µH, 2A. When the inductance value is big, the filter is effective but the efficiency rather falls. The toroidal coil can be made by yourself, too. ![]() |