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Product Focus - Silent Switcher Technology


A ‘breakthrough’ in switching regulator design


Christian Kueck looks at how to reduce EMI and improve efficiency using silent switcher designs


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witching regulators replace linear regulators in areas where low heat dissipation and efficiency are valued.


The switching regulator is typically the first active component on the input power bus line, and therefore has a significant impact on the EMI performance of the complete converter circuit. Modern input filter components in surface mount technology have better performance than through-hole parts. However, this improvement is outpaced by the increase in operating switching frequencies of switching regulators. Higher efficiency and low minimum on- and off- times result in higher harmonic content due to the faster switch transitions. For every doubling in switching


frequency the EMI becomes 6dB worse when all other parameters, such as switch capacity and transition times, remain constant. The wideband EMI behaves like a first order high pass with 20dB higher emissions if the switching frequency increases by 10x.


minimum hot loop size. To make layout even more challenging, on a typical planar printed circuit board the magnetic or transformer style coupling between traces above 30MHz will diminish all filter efforts, since the higher the harmonic frequencies are, the more effective unwanted magnetic coupling becomes.


The tried and true solution is to use a shielding box for the complete circuit. Of course, this adds costs, increases required board space, makes thermal management and testing more difficult, and introduces additional assembly costs. Another frequently used method is to slow down the switching edges. This has the undesired effect of reducing the efficiency, increasing minimum on-, off-times, as well as the required dead times, and compromises the potential current control loop speed. With Linear’s new LT8614 Silent Switcher regulator, you have the effect of a shielded box without using a shield and are also able to eliminate the mentioned drawbacks listed above. See Figure 1. The LT8614 has a low IQ


Figure 1: The LT8614 Silent Switcher minimises EMI/EMC emissions while delivering high efficiency at frequencies up to 3MHz


Savvy PCB designers will make the hot loops small and use shielding GND layers as close to the active layer as possible; nevertheless pinout, package construction, thermal design requirements and package sizes needed for adequate energy storage in decoupling components dictate a certain


20 November 2013


of the LT861x series of only 2.5µA operating current. This is the total supply current consumed by the device, in regulation, with no load. It features the same ultralow dropout of this family, which is only limited by the internal top switch. Unlike alternative solutions, the LT8614’s RDSON is not limited by maximum duty cycle and minimum off- times. The part skips its


switch-off cycles in dropout and performs only the minimum required off cycles to keep the internal top switch boost stage voltage sustained, as shown in Figure 6. At the same time, the minimum operating input voltage is 2.9V typical (3.4V max.) and the device can supply a


Components in Electronics


3.3V rail with the part in dropout. The LT8614 is higher efficiency than the LT8610/11 at high currents since its total switch resistance is lower. It can also be synchronised to an external frequency operating from 200KHz to 3MHz. The AC switch losses are low so it can be operated at high switching frequencies without much efficiency loss. In EMI-sensitive applications such as automotive environments, a good balance can be attained and the LT8614 can run either below the AM band for even lower EMI, or above the AM band. In a setup with 700KHz operating switching frequency, the standard LT8614 demo board does not exceed the noise floor in a CISPR25 measurement. The Figure 2 measurements


were taken in an anechoic chamber 12V in 3.3V out at 2A with a fixed switching frequency of 700kHz. To compare the LT8614 Silent Switcher technology against a current state-of-the- art switching regulator, the part was measured against an LT8610. The test was performed in a GTEM cell using the same load, input voltage and the same inductor on the standard demo boards for both parts.


One can see that up to a 20dB improvement is made using the LT8614 Silent Switcher technology compared to the already very good EMI performance of the LT8610, especially in the more difficult to manage higher frequency area. This enables simpler and more compact designs where the LT8614 switching power supply needs less filtering and distance compared to other sensitive systems in the overall design.


In the time domain, the


LT8614 shows very benign behaviour on the switch


Figure 3: Blue trace is the LT8614, purple trace is the LT8610; both 13.5Vin, 3.3V out at 2.2A load


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node edges, as shown in Figure 4. Even at 4ns/div the LT8614 Silent Switcher regulator shows very low ringing (see Ch2 in Figure 3). The LT8610 has a good damped ringing (Ch1, Figure 3) but one can see the higher energy stored in the hot loop compared to the LT8614 in Ch2.


Figure 2: Blue trace is the noise floor; red trace is the LT8614 board at CISPR25 radiated measurement in an anechoic chamber


Figure 5 shows the switch node at 13.2V in. One can see the extremely low deviation from the ideal square wave of the LT8614, shown in Ch2. All time


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