written 8.4 years ago by | modified 2.8 years ago by |
Mumbai University > Electronics Engineering > Sem7 > Power Electronics 2
Marks: 10M
written 8.4 years ago by | modified 2.8 years ago by |
Mumbai University > Electronics Engineering > Sem7 > Power Electronics 2
Marks: 10M
written 8.4 years ago by | • modified 8.4 years ago |
1. Basic buck converter or regulator
The fundamental circuit for a step down converter or buck converter consists of an inductor, diode, capacitor, switch and error amplifier with switch control circuitry.
The circuit for the buck regulator operates by varying the amount of time in which inductor receives energy from the source.
In the basic block diagram the operation of the buck converter or buck regulator can be seen that the output voltage appearing across the load is sensed by the sense / error amplifier and an error voltage is generated that controls the switch.
Typically the switch is controlled by a pulse width modulator, the switch remaining on of longer as more current is drawn by the load and the voltage tends to drop and often there is a fixed frequency oscillator to drive the switching.
2. Buck converter operation
When the switch in the buck regulator is on, the voltage that appears across the inductor is Vin - Vout. Using the inductor equations, the c urrent in the inductor will rise at a rate of (Vin-Vout)/L. At this time the diode D is reverse biased and does not conduct.
When the switch opens, current must still flow as the inductor works to keep the same current flowing. As a result current still flows through the inductor and into the load. The diode, D then forms the return path with a current Idiode equal to Iout flowing through it.
With the switch open, the polarity of the voltage across the inductor has reversed and therefore the current through the inductor decreases with a slope equal to -Vout/L.
3. Current waveforms at different times during the overall cycle
$$ u_1=L\dot{x_1}+x_2 \ \ \ x_1=C\dot{x_2}+\frac{x_2}{R} $$
$ \begin{bmatrix} \ \dot{x_1}\\ \ \dot{x_2} \\ \end{bmatrix} =\begin{bmatrix} \ 0 & -\frac{1}L \\ \ \frac{1}C & \ -\frac{1}{RC} \\ \end{bmatrix} \begin{bmatrix} \ {x_1}\\ \ {x_2} \\ \end{bmatrix} \begin{bmatrix} \ \frac{1}L \\ \ \ 0 \\ \end{bmatrix} [u_1] $
$0=L\dot{x_1}+{x_2} \ \ \ x_1=C\dot{x_2}+\frac{x_2}{R}$