SNVSA15B December 2013 – December 2015 LP8557
PRODUCTION DATA.
Figure 50 shows an example layout which applies the required proper layout guidelines to be used as a guide for laying out the LP8557 circuit.
COMPONENT | MANUFACTURER | VALUE | PART NUMBER | SIZE (mm) | CURRENT/VOLTAGE RATING, RESISTANCE, TEMPERATURE |
---|---|---|---|---|---|
L | Cyntec | 10 µH | PIME051E | 5.4 × 5.2 × 1.5 | 2 A, 0.153 Ω |
COUT | Murata | 4.7 µF (×2) | GRM188R6YA475KE15D | 0603 (1.6 × 0.8 × 0.8) |
35 V, X5R |
CIN | TDK | 10 µF | C1608X5R1A106M080AC | 0603 (1.6 × 0.8 × 0.8) |
10 V, X5R |
Diode | Rohm Semiconductor | Schottky | RB160M-40 | SOD-123 (3.5 × 1.6 × 0.8) |
VR = 40 V, VF = 0.5 V |
The following guidelines apply to both LP8557 and LP8557I.
The LP8557 inductive boost converter sees a high switched voltage at the SW pin, and a step current through the Schottky diode and output capacitor each switching cycle. The high switching voltage can create interference into nearby nodes due to electric field coupling (I = C × dV/dt). The large step current through the diode and the output capacitor can cause a large voltage spike at the SW and FB pins due to parasitic inductance in the step current conducting path (V = L × di/dt). Board layout guidelines are geared towards minimizing this electric field coupling and conducted noise. Figure 48 highlights these two noise-generating components.
The following list details the main (layout sensitive) areas of the LP8557’s inductive boost converter in order of decreasing importance:
Because the output capacitor is in the path of the inductor current discharge path, it detects a high-current step from 0 to IPEAK each time the switch turns off and the Schottky diode turns on. Any inductance along this series path from the diodes cathode, through COUT, and back into the LP8557 GND pin contributes to voltage spikes (VSPIKE = LP_ × dI/dt) at SW and OUT. These spikes can potentially over-voltage the SW and FB pins, or feed through to GND. To avoid this, COUT+ must be connected as close to the cathode of the Schottky diode as possible, and COUT− must be connected as close to the LP8557 GND pins as possible. The best placement for COUT is on the same layer as the LP8557 to avoid any vias that can add excessive series inductance.
In the LP8557’s boost circuit the Schottky diode is in the path of the inductor current discharge. As a result the Schottky diode sees a high-current step from 0 to IPEAK each time the switch turns off, and the diode turns on. Any inductance in series with the diode can cause a voltage spike (VSPIKE = LP_ × dI/dt) at SW and OUT. This can potentially over-voltage the SW pin, or feed through to VOUT and through the output capacitor, into GND. Connecting the anode of the diode as close to the SW pin as possible, and connecting the cathode of the diode as close to COUT+ as possible, reduces the inductance (LP_) and minimize these voltage spikes.
The node where the inductor connects to the LP8557 SW bump has 2 challenges. First, a large switched voltage (0 to (VOUT + VF_SCHOTTKY)) appears on this node every switching cycle. This switched voltage can be capacitively coupled into nearby nodes. Second, there is a relatively large current (input current) on the traces connecting the input supply to the inductor and connecting the inductor to the SW bump. Any resistance in this path can cause voltage drops that can negatively affect efficiency and reduce the input operating voltage range.
To reduce the capacitive coupling of the signal on SW into nearby traces, the SW bump-to-inductor connection must be minimized in area. This limits the PCB capacitance from SW to other traces. Additionally, high-impedance nodes that are more susceptible to electric field coupling need to be routed away from SW and not directly adjacent or beneath. This is especially true for traces such as ISET/SCL, FSET/SDA, and PWM. A GND plane placed directly below SW dramatically reduces the capacitance from SW into nearby traces.
Lastly, limit the trace resistance of the VBATT-to-inductor connection and from the inductor-to-SW connection, by use of short, wide traces.
The LP8557 input capacitor filters the inductor current ripple and the internal MOSFET driver currents. The inductor current ripple can add input voltage ripple due to any series resistance in the input power path. The MOSFET driver currents can add voltage spikes on the input due to the inductance in series with the VIN/VDD and the input capacitor. Close placement of the input capacitor to the VDD pin and to the GND pin is critical because any series inductance between VIN/VDD and CIN+ or CIN– and GND can create voltage spikes that could appear on the VIN/VDD supply line and GND.
Close placement of the input capacitor at the input side of the inductor is also critical. The source impedance (inductance and resistance) from the input supply, along with the input capacitor of the LP8557, forms a series RLC circuit. If the output resistance from the source (RS, Figure 49) is low enough, the circuit is underdamped and has a resonant frequency (typically the case). Depending on the size of LS, the resonant frequency could occur below, close to, or above the LP8557's switching frequency. This can cause the supply current ripple to be:
The circuit is redrawn for the AC case where the VIN supply is replaced with a short to GND and the LP8557 + Inductor is replaced with a current source (ΔIL). Equation 1 is the criteria for an under-damped response. Equation 2 is the resonant frequency. Equation 3 is the approximated supply current ripple as a function of LS, RS, and CIN.
As an example, consider a 3.8-V supply with 0.1-Ω of series resistance connected to CIN (10 µF) through 50 nH of connecting traces. This results in an under-damped input-filter circuit with a resonant frequency of 225 kHz. Because both the 1-MHz and 500-kHz switching frequency options lie above the resonant frequency of the input filter, the supply current ripple is probably smaller than the inductor current ripple. In this case, using Equation 3, the supply current ripple can be approximated as 0.2 times the inductor current ripple (using a 500-kHz switching frequency) and 0.051 times the inductor current ripple using a 1-MHz switching frequency.
Low-pass filter near VDD input pin is recommended for noisy power condition to prevent unstable LED current. 10 Ω plus approximately 2.2 µF to 10 µF can be used as low-pass filter components.