The buck converter is a common DC-DC converter used for efficiently stepping down voltage. In this design, one critical parameter is fixed based on the roll number 98. We demonstrate two options:
For our demonstration, we illustrate the design using the switching frequency constraint of 98 kHz while noting that similar techniques apply if the critical parameter is set on the inductance.
A typical buck converter circuit contains the following components:
The schematic diagram of the buck converter is illustrated below:
Vin
│
│
├─────────┐
│ │
│ [SW] ← Controlled Switch (MOSFET)
│ │
│ └───── L ─────┐
│ │
│ [ Diode ]
│ │
│ C
│ │
└──────────────────────┴──→ Vout → R (Load)
The design parameters chosen are as follows. We will use the roll number 98 to set the switching frequency as 98 kHz (or, in an alternative approach, fix the inductance to 98 μH). For this design, we assume:
Parameter | Value | Unit | Description |
---|---|---|---|
Vin | 12 | V | Input voltage (chosen for a low voltage application) |
Vout | 5 | V | Desired regulated output voltage |
Iout | 1 | A | Load current, providing baseline design currents |
fs | 98 | kHz | Switching frequency, fixed by the roll number as the critical design parameter |
In the alternative method, one could choose the inductance to be 98 μH and modify the other parameters accordingly. In our current synthesis, we will use fs = 98 kHz as the guiding design constraint.
In an ideal buck converter, the output voltage is related to the input voltage by the duty cycle (D):
Formula: D = Vout / Vin
Substituting the values:
D = 5 V / 12 V ≈ 0.4167, or approximately 41.67%
The inductor is designed to limit the current ripple (ΔIL) in the circuit. A typical design target is to set the ripple current as a percentage of the output current; here, we assume 20% of Iout:
ΔIL = 0.2 × 1 A = 0.2 A
Inductor Value Formula:
L = (Vin – Vout) × D / (fs × ΔIL)
Calculation:
L = (12 V – 5 V) × 0.4167 / (98,000 Hz × 0.2 A)
L = 7 V × 0.4167 / 19,600 ≈ 2.9169 V / 19,600 ≈ 0.000149 H or 149 µH
In a practical implementation, component tolerances may lead us to choose a standard inductor value near this calculated result.
The output capacitor helps smooth the output voltage by reducing voltage ripple (ΔVout). Let us assume the output voltage ripple is limited to 1% of Vout:
ΔVout = 0.01 × 5 V = 0.05 V
Capacitor Value Formula:
C = Iout × D / (fs × ΔVout)
Calculation:
C = 1 A × 0.4167 / (98,000 Hz × 0.05 V) ≈ 0.4167 / 4,900 ≈ 0.0000851 F or 85.1 µF
Due to component tolerances and non-ideal behaviors (such as equivalent series resistance, ESR), designers often select a higher standard capacitor value. For instance, a capacitor value of 100 µF might be chosen in practice.
The controlled switch, typically a MOSFET, must handle the input voltage (Vin) and the maximum current of the circuit. Similarly, the freewheeling diode must withstand a reverse voltage equal to at least Vin and conduct the inductor current when the switch is off.
For our low-voltage design, the following ratings are advisable:
With a switching frequency (fs) fixed at 98 kHz, the switch is driven by a PWM signal with the calculated duty cycle. The PWM signal is a square waveform that is high for approximately 41.67% of the period and low for the remaining 58.33%.
Time Period Calculation: The period T is the reciprocal of the switching frequency:
T = 1/fs = 1/98,000 ≈ 10.2 µs
Thus, the switch is ON for about 4.25 µs and OFF for about 5.95 µs.
The inductor current in a buck converter is characterized by a triangular ripple superimposed on an average DC level. When the switch is on, the inductor current ramps upward; when the switch is off, the current ramps downward due to the freewheeling diode conduction.
The calculated ripple (ΔIL) is approximately 0.2 A, meaning the inductor current will oscillate ±0.1 A around its average value of 1 A.
A simplified timing diagram for the inductor current is as follows:
Inductor Current (IL)
/\ /\ /\
/ \ / \ / \
/ \__/ \__/ \
The average inductor current equals the load current, while the peak-to-peak ripple is limited by the design.
The output voltage (Vout) should ideally remain at a steady DC level of 5 V with minimal ripple. The output capacitor filters the ripple caused by the switching action. In our design, the output ripple is constrained to roughly 0.05 V, resulting in a clean DC voltage.
Vout (5V DC)
────────|¯|───────|¯|───────
In practice, oscilloscope traces of Vout will reveal a small high-frequency ripple superimposed on the DC output voltage.
Alternatively, the critical parameter may be chosen as the inductor value, fixed at 98 μH according to the roll number. In this scenario, the switching frequency and other parameters will be recalculated to ensure that the design meets the required performance targets.
For example, let’s consider the following alternate specifications:
Parameter | Value | Unit | Description |
---|---|---|---|
Vin | 24 | V | Input voltage |
Vout | 12 | V | Desired output voltage |
Iout | ~4.17 | A | Output current for a 50W load |
L | 98 | µH | Critical parameter set by roll number |
fs | Typically, 100 kHz or higher | - | Chosen to manage ripple and switching losses |
With L fixed at 98 μH, the designer would then use:
ΔIL = (Vin – Vout) × D / (L × fs) and adjust fs and D to achieve the desired output, ensuring consistent performance while the inductor value remains anchored by the roll number.
The signal waveforms will remain similar in nature—PWM for the switching element, a triangular ripple for the inductor current, and filtered DC on the output. However, the amplitude and timing of these signals might adjust slightly owing to the changes in frequency and duty cycle that accompany the fixed inductance constraint. Designers must use simulation tools such as SPICE, MATLAB/Simulink, or equivalent to validate these signals and adjust component ratings.
When designing a real-world converter, component selection must account for non-ideal factors such as switching losses, parasitic resistances, and temperature variations. It is recommended to choose:
Prior to hardware implementation, simulation can help predict performance metrics. Tools like MATLAB/Simulink or SPICE allow designers to:
A typical simulation would involve setting up the buck converter model, running a transient analysis, and comparing the simulated waveforms with the theoretical predictions discussed above.
This design example demonstrates a comprehensive approach to constructing a buck converter with a critical design parameter derived from the roll number 98. By fixing the switching frequency at 98 kHz (or alternatively, the inductor at 98 μH), the remaining parameters such as duty cycle, inductor value, and output capacitor are computed to meet the desired electrical outputs. In our primary design, with Vin = 12 V, Vout = 5 V, Iout = 1 A, and a calculated duty cycle of approximately 41.67%, component values were derived leading to an inductor value of roughly 149 µH and a capacitor of about 85 µF.
Design considerations include careful component selection to manage real-world issues such as parasitic effects, ensuring a converter that functions reliably under various conditions. Additionally, simulation plays a pivotal role in validating the theoretical calculations and optimizing the design prior to fabrication.
Both design approaches—anchoring the switching frequency at 98 kHz or fixing the inductance to 98 μH—are valid, and the choice may depend on specific application requirements and component availability. The synthesized design herein provides a structured framework that meets academic assignment requirements while illustrating the practical integration of theory and engineering practice.