Diode Power Loss Calculator
Calculate conduction loss, switching loss, junction temperature, and heatsink requirements for Si, Schottky, SiC, and GaN diodes. Includes rectifier topology comparison and live thermal visualisation.
× trr × fsw
× Rth(j-a)
| Package | Rth(j-c) typical | Max current |
|---|---|---|
| DO-41 (axial) | 15–25 °C/W | 1 A |
| DO-15 | 10–20 °C/W | 1.5 A |
| DO-201AD | 4–8 °C/W | 6 A |
| TO-220 (2-pin) | 1.5–3 °C/W | 15 A |
| TO-247 | 0.5–1.5 °C/W | 30 A |
| D2PAK (SMD) | 1.5–3 °C/W | 15 A |
| SOD-323 (SMD) | 150–300 °C/W | 0.3 A |
| Topology | Diodes conducting | Total Vf drop | Power Loss | Efficiency |
|---|
| Diode Type | Vf typ. | trr | Pcond | Psw | Ptotal | Relative Eff. | Best for |
|---|
| Part Number | Type | Vf @ If | VRRM | IF(av) | trr | Package |
|---|---|---|---|---|---|---|
| 1N4001 | Si PN | 0.93V @ 1A | 50V | 1A | 2 μs | DO-41 |
| 1N4007 | Si PN | 0.93V @ 1A | 1000V | 1A | 2 μs | DO-41 |
| 1N5408 | Si PN | 1.0V @ 3A | 800V | 3A | 3 μs | DO-201 |
| 1N5819 | Schottky | 0.45V @ 1A | 40V | 1A | <10 ns | DO-41 |
| 1N5822 | Schottky | 0.525V @ 3A | 40V | 3A | <10 ns | DO-201 |
| SS34 | Schottky | 0.5V @ 3A | 40V | 3A | <10 ns | SMA |
| MBRS360 | Schottky | 0.5V @ 3A | 60V | 3A | <10 ns | SMB |
| MBR20100 | Schottky | 0.75V @ 20A | 100V | 20A | <10 ns | TO-220 |
| UF4007 | Ultrafast | 1.0V @ 1A | 1000V | 1A | 75 ns | DO-41 |
| BYW29-200 | Ultrafast | 0.95V @ 8A | 200V | 8A | 25 ns | TO-220 |
| MUR1560 | Ultrafast | 0.87V @ 15A | 600V | 15A | 35 ns | TO-220 |
| C3D04060A | SiC | 1.5V @ 4A | 600V | 4A | <5 ns | TO-220 |
| IDH06SG60C | SiC | 1.5V @ 6A | 600V | 6A | <5 ns | TO-220 |
| GS1M | Si PN | 1.0V @ 1A | 1000V | 1A | 150 ns | SMA |
| Technology | Vf range | VRRM max | trr | Leakage | Tj,max |
|---|---|---|---|---|---|
| Standard Silicon (PN) | 0.6–1.2V | Up to 5kV | 1–10 μs | Low | 150°C |
| Fast Recovery (FR) | 0.8–1.2V | Up to 1.2kV | 50–500 ns | Low | 150°C |
| Ultrafast Recovery | 0.8–1.1V | Up to 1.2kV | 15–75 ns | Medium | 150°C |
| Schottky (Si) | 0.2–0.5V | Up to 200V | <10 ns | High | 175°C |
| Silicon Carbide (SiC) | 1.4–2.0V | Up to 1.7kV | <5 ns | Very Low | 200°C |
| GaN (HEMT-based) | 0.5–1.5V | Up to 650V | <2 ns | Very Low | 150°C |
Understanding Diode Power Loss
Every diode dissipates power when conducting current. This loss has two distinct components: conduction loss and switching loss. Conduction loss (Pcond = Vf × Iavg) occurs continuously whenever the diode is forward biased and is the dominant loss mechanism in low-frequency applications like mains rectifiers. A standard silicon diode with Vf = 0.7V carrying 10A dissipates 7W as heat — a substantial efficiency penalty in high-current systems.
Switching loss (Psw = ½ × Vr × Ipk × trr × fsw) arises from reverse recovery. When a conducting diode is reverse biased, minority carriers stored in the junction must recombine before the diode blocks. During this reverse recovery time (trr), a brief reverse current flows through the diode, dissipating energy proportional to switching frequency. At 100 kHz with a 2 μs recovery time, switching loss can dwarf conduction loss — making diode technology selection critical for switched-mode power supplies.
Junction Temperature and Thermal Management
Diode reliability depends critically on junction temperature. Every 10°C rise in Tj approximately halves the expected device lifetime (Arrhenius degradation model). Junction temperature is calculated through the thermal resistance network: Tj = Ta + Ptotal × Rth(j-a), where Rth(j-a) = Rth(j-c) + Rth(c-s) + Rth(s-a). Each thermal resistance stage adds temperature rise: junction-to-case (from the datasheet), case-to-sink (thermal interface material, typically 0.1–0.5 °C/W with good thermal paste), and sink-to-ambient (the heatsink itself).
Always apply a derating margin: design for Tj ≤ 80% of the datasheet maximum. For a 150°C rated device, target Tj ≤ 120°C. This provides margin for thermal impedance degradation over time, hotspot variation within the die, and ambient temperature excursions.
Rectifier Topology Comparison
The choice of rectifier topology directly affects how many diode voltage drops appear in series with the load. A half-wave rectifier uses one diode (one Vf drop) but only conducts on alternate half-cycles, wasting half the input energy. A full-wave bridge uses four diodes but two conduct simultaneously, producing 2 × Vf drop. A centre-tap full-wave rectifier uses two diodes with one Vf drop but requires a centre-tapped transformer.
For a 12V, 10A application using standard silicon (Vf = 0.7V): the bridge rectifier loses 14W (2 × 0.7 × 10), achieving 89.6% efficiency. Substituting Schottky diodes (Vf = 0.35V) reduces losses to 7W — doubling the useful power and eliminating the need for active cooling.
Frequently Asked Questions
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