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LTC3422 Datasheet(PDF) 13 Page - Linear Technology |
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LTC3422 Datasheet(HTML) 13 Page - Linear Technology |
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13 / 16 page ![]() LTC3422 13 3422fa APPLICATIO S I FOR ATIO conduct heat away from the LTC3422 and into the copper plane with as much area as possible. In the event that the junction temperature gets too high, the peak current limit will automatically be decreased. If the junction tempera- ture continues to rise, the LTC3422 will go into thermal shutdown and all switching will stop until the internal temperature drops. VIN > VOUT Operation The LTC3422 will maintain voltage regulation when the input voltage is above the output voltage. This is achieved by terminating the switching of the synchronous P-chan- nel MOSFET and applying VIN statically on the gate. This will ensure the volt • seconds of the inductor will reverse during the time current is flowing to the output. Since this mode will dissipate more power in the LTC3422, the maximum output current is limited in order to maintain an acceptable junction temperature and is given by: I T VV OUT MAX A IN OUT () – •( . ) – = + () 125 43 1 5 where TA = ambient temperature. For example at VIN = 4.5V, VOUT = 3.3V and TA = 85°C, the maximum output current is 345mA. Short Circuit The LTC3422 output disconnect feature allows output short circuit while maintaining a maximum internally set current limit. However, the LTC3422 also incorporates internal features such as current limit foldback and ther- mal shutdown for protection from an excessive overload or short circuit. During a prolonged short circuit the current limit folds back to 0.75A typical should VOUT drop below approximately 666mV. This 0.75A current limit remains in effect until VOUT exceedsapproximately800mV, at which time the steady-state current limit is restored. Closing the Feedback Loop The LTC3422 utilizes current mode control with internal adaptive slope compensation. Current mode control elimi- nates the 2nd order filter due to the inductor and output capacitor exhibited in voltage mode controllers, thus simplifying it to a single pole filter response. The product of ‘the modulator control to output DC gain’ and ‘the error amp open-loop gain’ gives the DC gain of the system: GG G V V G V I G DC CONTROL OUTPUT EA REF OUT CONTROL OUTPUT IN OUT EA = = ≈ _ _ •• • ; 2 2000 The output filter pole is given by: ƒFILTER POLE OUT OUT OUT I VC _ •• = π where COUT is the output filter capacitor. The output filter zero is given by: ƒFILTER ZERO ESR OUT RC _ •• • = π 1 2 where RESR is the capacitor equivalent series resistance. A troublesome feature of the boost regulator topology is the right-half plane zero (RHP), given by: ƒRHPZ IN OUT OUT V IL V = π 2 2• • • • At heavy loads this gain increase with phase lag can occur at a relatively low frequency. The loop gain is typically rolled off before the RHP zero frequency. The typical error amplifier compensation is shown in Figure 3. The equations for the loop dynamics are as follows: ƒ ƒ ƒ POLE C ZERO ZC POLE ZC eC RC RC 1 1 1 1 2 2 1 220 6 1 2 1 2 ≈ π ≈ π ≈ π •• • •• • •• • which is extremely close to DC |
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