Gvg derivation of inverted Buck-Boost (IBB) converter

Ming Sun

Ming Sun / November 30, 2022

14 min read––– views

Step 1 - construct small-signal equations

Inverted Buck-Boost (IBB) block diagram
Fig. 11Inverted Buck-Boost (IBB) block diagram[1]

Voltage-second balance equation

Fig. 1 shows a synchronous inverted Buck-Boost (IBB) power stage, where it contains a low side switch S1 and a high side switch S2.

For the inductor, we can write the voltage-second balance as[1]:

`L{dI}/{dt} = D*V_g + D^'*V`
(1)

Where, I is the inductor current, Vg is the Boost converter's input voltage, and V is Boost converter's output voltage Vout. Next, let us perturb and linearize Eq. 1 by introducting the small signal perturbation as:

`L{d(I+hat(i))}/{dt} = D*(V_g+hat(v)_g) + D^'*(V+hat(v))`
(2)

Here we are trying to derive the transfer function of Gvg. As a result, we can assume duty cycle D is constant. Removing the DC terms from and second order small signal terms Eq. 2 , we have:

`L{dhat(i)}/{dt} = D*hat(v)_g + D^'*hat(v)`
(3)

Eq. 3 can be written in s domain as:

`sL*hat(i) = D*hat(v)_g + D^'*hat(v)`
(4)

charge balance equation

For the capacitor, we can write the charge balance as[1]:

`C{dV}/{dt} = -D^'*I-V/R`
(5)

Next, let us perturb and linearize Eq. 5 by introducting the small signal perturbation as:

`C{d(V+hat(v))}/{dt} = -D^'*(I+hat(i))-(V+hat(v))/R`
(6)

Removing the DC terms and second order small signal terms from Eq. 6, we have:

`C{dhat(v)}/{dt} = -D^'*hat(i) - hat(v)/R`
(7)

Eq. 7 can be written in s domain as:

`sC*hat(v) = -D^'*hat(i) - hat(v)/R`
(8)

Step 2 - solve the Gvg in Matlab

The Matlab script used to derive the Gvg transfer function is as shown below:

Gvg_ibb.m
clc; clear; close all;

syms s
syms v i vg
syms R L C V Dp I Vg D
syms Gvg Gig

eqn1 = s*L*i == D*vg + Dp*v;
eqn2 = s*C*v == -Dp*i - v/R;
eqn3 = I*Dp == -V/R;
eqn4 = D*Vg + Dp*V == 0;
eqn5 = Gvg == v/vg;
eqn6 = Gig == i/vg;

results = solve(eqn1, eqn2, eqn3, eqn4, eqn5, eqn6, [v i I Vg Gvg Gig]);

Gvg = simplify(results.Gvg)
Gig = simplify(results.Gig)

Fig. 2 shows the Gvg derived result from Matlab.

Gvg derived result from Matlab
Fig. 2Gvg derived result from Matlab

Next, we can use wxMaxima to simplify the results as shown in Fig. 3.

Gvg transfer function simplified results from wxMaxima
Fig. 3Gvg transfer function simplified results from wxMaxima

From Fig. 3, we have:

`G_{vg} = -(RDD^')/(RD^('2)+sL+RLCs^2)`
(9)

Eq. 9 can be rewritten as:

`G_{vg} = -D/D^'*1/(1+s*L/(RD^('2))+s^2*(LC)/(D^('2)))`
(10)

Simplis for verification of Gvg transfer function

To simulate Gvg transfer function in Simplis, the open loop Boost converter model is as shown in Fig. 4.

Open-loop IBB converter model for Gvg simulation
Fig. 4Open-loop IBB converter model for Gvg simulation

To set the property of the Laplace Transfer Function block, Eq. 10 can be re-written as:

`G_{vg} = -D/D^'*1/(1+s*L/(RD^('2))+s^2*(LC)/(D^('2))) = -(DD^')/(LC)*1/((D^('2))/(LC)+s/(RC)+s^2)`
(11)

We can plug in the inductor, capacitor, resistor, V and D' values into Eq. 11. We have:

`G_{vg} = -(DD^')/(LC)*1/((D^('2))/(LC)+s/(RC)+s^2) = -160G* 1/(640G + 800k*s + s^2)`
(12)

Based on Eq. 11, the property of the 2nd-order Laplace Transfer Function is as shown in Fig. 5.

2nd-order Laplace Transfer Function block property
Fig. 52nd-order Laplace Transfer Function block property

The Simplis simulation results are as shown in Fig. 6. From Fig. 6, we can see that the mathematical Laplace transfer function matches with the AC simulation results of Gvg very well at low frequency range.

Simulation results comparison between mathematical derivation and AC analysis
Fig. 6Simulation results comparison between mathematical derivation and AC analysis

But the difference is small enough and the it will not impact the actual design when we use the mathematical equations since in most of the design the closed loop cross over frequency is much less than the switching frequency fsw.

Gig verification

From Fig. 2, the Gig transfer function can be written as:

`G_{ig} = D*(1+sRC)/(RD^('2)+sL + RLCs^2)`
(13)

To verify the Gig transfer function, the Simplis test bench can be modified as shown in Fig. 6.

Gig test bench in Simplis for IBB converter
Fig. 7Gig test bench in Simplis for IBB converter

To set the property of the Laplace Transfer Function block, Eq. 12 can be re-written as:

`G_{ig} = D*(1+sRC)/(RD^('2)+sL + RLCs^2) = D/(RLC) * (1+sRC)/((D^('2))/(LC)+s/(RC) + s^2)`
(14)

We can plug in the inductor, capacitor, resistor and Vg values into Eq. 13. We have:

`G_{ig} = D/(RLC) * (1+sRC)/((D^('2))/(LC)+s/(RC) + s^2) = 160G*(1+s*1.25µ)/(640G+s*800k+s^2)`
(15)

Based on Eq. 14, the property of the 2nd-order Laplace Transfer Function is as shown in Fig. 7.

2nd-order Laplace Transfer Function block property for Gig simulation
Fig. 82nd-order Laplace Transfer Function block property for Gig simulation

The Simplis simulation results are as shown in Fig. 9. From Fig. 9, we can see that the mathematical Laplace transfer function matches with the AC simulation results of Gig.

Gig comparison between mathematical derivation and AC analysis
Fig. 9Gig comparison between mathematical derivation and AC analysis

References and downloads

[1] Fundamentals of power electronics - Chapter 2

[2] Open-loop IBB converter model for Gvg simulation in Simplis - pdf

[3] Open-loop IBB converter model for Gvg simulation in Simplis - download

[4] Open-loop IBB converter model for Gig simulation in Simplis - pdf

[5] Open-loop IBB converter model for Gig simulation in Simplis - download


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