Efficiency of Buck-Boost Converter

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SUMMARY

The discussion focuses on deriving the efficiency (η) of a Buck-Boost converter, defined as η = 100 * PO/PIN. Key equations include the relationships between input power (PIN) and output power (PO), factoring in the transistor on-resistance (R_{ON}) and diode voltage drop (V_{D_0}). The participants confirm that setting R_{ON} and V_{D_0} to zero results in an efficiency of 100%. The conversation emphasizes the importance of accurately deriving expressions for both input and output power to validate efficiency calculations.

PREREQUISITES
  • Understanding of Buck-Boost converter topology
  • Familiarity with power electronics terminology
  • Knowledge of duty cycle (D) in converter operation
  • Ability to manipulate and derive equations in electrical engineering
NEXT STEPS
  • Study the derivation of efficiency in Buck-Boost converters
  • Learn about the impact of R_{ON} and V_{D_0} on converter performance
  • Explore the role of duty cycle in power electronics
  • Investigate other converter topologies and their efficiency calculations
USEFUL FOR

Electrical engineers, power electronics students, and professionals involved in designing or analyzing Buck-Boost converters will benefit from this discussion.

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Homework Statement


Consider a Buck-Boost converter. If in addition to the transistor on resistance (R_{ON}), the converter diode has a voltage drop (V_{D_0}), symbolically derive an expression for the efficiency, η of the converter, where η = 100* PO/PIN. Verify that that when R_{ON} and V_{D_0} are set to 0, the efficiency is 100%.

Homework Equations


<V_L>=0
<I_C>=0
D'=(1-D), where D is the duty cycle

The Attempt at a Solution


Analysis of the two modes of Buck-Boost converter:
IqvCYzc.jpg


When <V_L>=0
\frac{DT_s(V_{IN}-R_{ON}I_L)+D'T_s(V_O+V_{D_0})}{T_s}=0
Equation 1: DV_{IN}-DR_{ON}I_L+D'V_O+D'V_{D_0}

When <I_C>=0
\frac{DT_s(\frac{-V_O}{R})+D'T_s(I_L-\frac{-V_O}{R})}{T_s}=0
-D\frac{V_O}{R}+D'I_L-D'\frac{V_O}{R}=0=\frac{-V_O}{R}+D'I_L
Equation 2: I_L=\frac{V_O}{D'R}

Plug 1 into 2:
Equation 3: V_O=\frac{DV_{IN}+D'V_{D_0}}{\frac{DR_{ON}}{D'R}-D'}

Equation 4: P_{IN}=V_{IN}*I_{IN}=V_{IN}*I_L=V_{IN}\frac{V_O}{D'R}=\frac{V_{IN}(DV_{IN}+D'V_{D_0})}{D'R(\frac{DR_{ON}}{D'R}-D')}

Equation 5: P_O=\frac{V_O^2}{R}=\frac{(DV_{IN}+D'V_{D_0})^2}{R(\frac{DR_{ON}}{D'R}-D')^2}

Dividing equation 5 by Equation 4 yields Equation 6: \frac{D'(DV_{IN}+D'V_{D_0})}{V_{IN}(\frac{DR_{ON}}{D'R}-D')}

Setting R_{ON}=0 and V_{D_0}=0 in Equation 6 yields: \frac{D'(DV_{IN})}{-D'V_{IN}}

I need Equation 6 to equal 1 when R_{ON} and V_{D_0} are set to 0.
 
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Im having trouble following your thought process.

I would go about it a different way.

eff = 100 * Po / Pin

So derive an expression for Po and Pin.

since Roff is inf, you can assume no current is transferred during the off state of the transistor. So use your duty cycle to determine the current. P=IV so you now should have an expression for input power.

As you stated earlier the inductor voltage and capacitor current averages will be zero. You can use this to derive an expression for your output power. You will then see that setting Vdo and Ro to zero will cause Po=Pin
 
You show the output as + but I assume you know the output will be -.
If you want I'm willing to do the problem and compare answers if you manage to get an expression that = 100% when Ron and Vd are both zero.
 
I figured out my mistake. My line for Equation 4 should say P_{IN}=V_{IN}*DI_L=...
After that it worked out.
 

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