Understanding Hot Swap: Example of Hot-Swap Circuit Design Process INTRODUCTION Although the currents that must be interrupted and started up can be large, some of the subtleties of high-current design are often given very little consideration. Since the “devil is in the details,” this article will focus on the function and significance of the components of a hot-swap control circuit—and provide an in-depth look at design considerations and optimum component selection criteria in the design process using an Analog Devices ADM1177 hot-swap controller. Hot-Swap Topologies The –48-V approach originated in traditional telecommunications-exchange system technology. Examples can be seen in Advanced Telecommunications Computing Architecture (ATCA) systems, optical networks, base stations, and blade servers. As a voltage commonly obtained from battery stacks, 48 V was chosen because power and signals could be transmitted over distance without significant losses, yet the level is not high enough to risk severe electric shock under ordinary conditions. Negative polarity was chosen because, in the inevitable presence of moisture when exposed to the elements, the migration of metallic ions from anode to cathode is far less corrosive with the positive terminal grounded. In data communications systems, however, where distance is not an important factor, the +12-V supply is more reasonable, making it popular in blade-server and network-system designs. This article will concentrate on +12-V systems. The Hot-Swap
Event This can be resolved with a hot-swap controller (Figure 1), which carefully controls the inrush current to ensure a safe power-up interval. The hot-swap controller will also continually monitor the supply current after power-up for protection against short circuits and overcurrent conditions during normal operation.
Figure 1. Hot-swap application diagram. The Hot-Swap
Controller
Figure 2. ADM1177 functional block diagram. Inside the hot-swap controller, a current-sense amplifier monitors the voltage drop across the external sense resistor. This small voltage (typically ranging from 0 mV to 100 mV) must be amplified to a useful level. The amplifier gain in the ADM1177 is 10, so, for example, a 100-mV drop produced by a given amount of current will be amplified to 1 V. This voltage is compared to a fixed or variable reference voltage. With a 1-V reference, a current that produces a voltage greater than 100 mV (±3%) across the shunt will cause the comparator to indicate an overcurrent. The maximum-current trip point is thus principally determined by the shunt resistance, the amplifier gain, and the reference voltage; the shunt resistance value sets the maximum current. A TIMER circuit sets a limit to the length of time a given overcurrent condition can exist. The ADM1177 has a soft-start function in which the overcurrent reference is ramped up linearly rather than turned on abruptly, forcing the load current to follow in a similar manner. This is achieved by injecting current from an internal current source into an external capacitor (SS pin) to linearly ramp the comparator’s reference input from 0 V to 1 V. The external SS capacitor sets the rate of this ramp. If necessary, the SS pin can also be driven directly by voltage to set the maximum current limit. An ON circuit, consisting of a comparator and reference circuit, enables the device. It accurately programs the voltage that the supply must reach to enable the controller. Once the device is enabled, the gate begins to charge up. The gate of the N-channel MOSFET used in this type of circuit must be above the source. In order to achieve this over the range of supply voltage (VCC), the hot-swap controller has an integrated charge pump capable of maintaining the GATE pin as much as 10 V higher than VCC. The GATE pin requires a charge-pumped pull-up current to enable the MOSFET and pull-down currents to disable the MOSFET when necessary. Weak pull-down currents are used for regulation, and stronger pull-down currents are used to quickly disable the MOSFET in the event of a short circuit. The final essential block of the hot-swap controller is the TIMER, which limits the time the current is in regulation during an overcurrent event. MOSFETs are designed to withstand a given amount of power for a prescribed maximum time. The MOSFET manufacturers outline this range, or safe operating area (SOA), using a graph such as that shown in Figure 3.
Figure 3. MOSFET SOA graph. The SOA graph shows a relationship between the combined drain-source voltage, drain current, and the time duration that the MOSFET can withstand this dissipation. For example, the MOSFET in Figure 3 can withstand 10 V and 85 A (850 W) for 1 ms. If this condition persists for a greater duration, the MOSFET will be destroyed. The TIMER circuit can ensure that the length of time the MOSFET is subject to these worst-case conditions is limited by the external TIMER capacitor. For example, if the TIMER was set to 1 ms and the current exceeded the limit for more than 1 ms, the circuit would time out and shut down the MOSFET. In the ADM1177, to provide a margin of safety, the TIMER current-sense voltage activation threshold is set to 92 mV. The hot-swap controller will thus start timing the current conservatively as the sense voltage approaches the regulated value of 100 mV. Design Example
To simplify this discussion, the calculations exclude the effects of component tolerances. These tolerances should of course be considered when designing for worst-case conditions. ON Pin A resistive divider consisting of 10-kohm and 1.5 kohm resistors will have a suitable ratio of 0.130. Sense-Resistor
Selection
where VSENSETIMER = 92 mV. The maximum power dissipated by the sense resistor at 30 A is
So the sense resistor should be capable of dissipating 3 W. If a single resistor with the correct power rating or resistance is not available, the sense resistor can be made with multiple resistors. Load Capacitance
Charge Time
where VREGMIN = 97 mV, the minimum regulation voltage of the hot-swap controller. This equation assumes an ideal condition of load current ramping from 0 A to 30 A instantaneously. In reality, the gate charge, QGS, of larger MOSFETs serves to limit the slew rate of the gate voltage—and hence the power-up current profile—so that a quantity of charge is delivered to the load capacitor without triggering the TIMER function. In Figure 4, the MOSFET with the higher QGS results in the TIMER being active for a shorter period, T1 to T3, as compared to the MOSFET with the lower QGS, which causes the timer to be active during T0 to T2.
Figure 4. Effect of QGS on start-up profiles. This is because the charge delivered between T0 and T1 accumulates at less than the current limit. Thus, the calculated time required can be reduced accordingly. This amount is difficult to quantify; it depends on the controller gate current and MOSFET specification for gate charge and capacitances. Since it may account for as much as 30% of the total charge current in some cases, it needs to be considered, particularly in designs using large MOSFETs and high currents. For designs using MOSFETs with lower gate charge, a fast gate ramp can be assumed. This will result in a fast ramp from 0 A to ITRIP, which may cause unwanted transients; in this case, soft start should be used. Soft Start
Figure 5. Soft-start effect on TIMER. Therefore, a soft-start time of no more than 10% to 20% of the total TIMER is recommended. For this example, we can choose a time of 100 μs. The SS capacitance value can be determined as follows:
where ISS = 10 μA and VSS = 1 V. MOSFET and TIMER
Selection Thermal and Power
Considerations Recall that the hot-swap controller initiates the TIMER at a minimum sense voltage of 92 mV. For this calculation, we need to know the maximum possible dc current that can flow without tripping the TIMER. Assume the worst-case VREGMIN of 97 mV. Then,
Assuming that the MOSFET's maximum RDSON is 2 milliohms, the power is
The MOSFET’s thermal resistance at ambient temperature will be specified in the data sheet. The footprint size and additional copper will have an effect on this value. Assume
As the MOSFET is required to dissipate 2.1 W, a worst-case temperature rise of 126°C above ambient can be expected:
One way to reduce this number is to use two or more MOSFETs in parallel. This will effectively reduce the RDSON and thus the power dissipation in the MOSFETs. With two MOSFETs, a maximum temperature rise of 32°C per MOSFET will be incurred, assuming current is divided evenly between the devices (some tolerance should be allowed). The following shows the power in each MOSFET:
With this temperature rise and an assumed ambient temperature of TA = 30°C, a maximum case temperature of 62°C can be expected for each MOSFET.
MOSFET SOA Considerations
Before comparing
this to the MOSFET SOA graphs, we need to consider the temperature derating
of the MOSFET, since the SOA graph is based on data at ambient case temperature,
TC = 25°C. First calculate the power dissipation
at
where RthJC is specified in MOSFET data sheet. Now perform the same calculation for TC = 62°C:
Thus, a derating factor of 1.42 is calculated as follows:
This needs to be applied to the SOA graph, of the MOSFET in Figure 3. The diagonal lines that represent the time maximum power is applied need to be moved downward to reflect the adjusted power ratings. We earlier used the 1-ms line as an example to illustrate how the curves work. For example, take a point on that line—say (20 A, 40 V); the power at that point is 800 W. Applying the derating formula:
At 40 V, the corresponding current for derated power is 14 A. Plotting this point on the SOA graph establishes a point on the new 62°C-derated 1-ms line. New 10-ms and 100-μs lines can be established in the same way. The new lines are shown in red in Figure 6.
Figure 6. SOA plot including 62°C-derated power limits. Selecting the
TIMER Capacitor Recall that the estimated time to charge the load was approximately 850 μs. As the soft-start time is established by a linear ramp, it takes longer (than with a step change) to charge the load capacitors. To estimate the total volume of charge, assume that half the SS time is to be added to the calculated time if using soft start; thus add half the SS time (50 μs) to 850 μs, resulting in a total time of approximately 900 μs. If the MOSFET chosen has a large gate charge (e.g., ≥80 nC), this may be further reduced, as discussed earlier. If the time to charge the load is less than the maximum SOA time, the MOSFET is suitable. In this case, the criterion is met (0.9 ms < 2 ms). A TIMER value of less than 2 ms should be sufficient to protect the MOSFET—and greater than 0.9 ms to charge the load. If a conservative value of 1 ms is selected, the capacitance can be calculated as follows:
where ITIMER = 60 μA and VTIMER = 1.3 V,
When using paralleled MOSFETs, the calculations for TIMER selection will not change. It is critical that the TIMER and short-circuit protection be designed with a single MOSFET in mind. The reason is that the VGSTH can differ significantly among a population of MOSFETs, so a single MOSFET may be required to handle a large proportion of current during regulation. Hot-Swap Design
Complete
Figure 7. Completed reference design.
Copyright 1995-
Analog
Devices, Inc. All rights reserved. |
||||||