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LM4951 Datasheet(PDF) 13 Page - Texas Instruments |
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LM4951 Datasheet(HTML) 13 Page - Texas Instruments |
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13 / 22 page ![]() LM4951 www.ti.com SNAS244N – AUGUST 2004 – REVISED MAY 2013 TJMAX = PDMAX-MONOBTLθJA + TA (5) Equation (5) gives the maximum junction temperature TJMAX. If the result violates the LM4951's 150°C, reduce the maximum junction temperature by reducing the power supply voltage or increasing the load resistance. Further allowance should be made for increased ambient temperatures. The above examples assume that a device is operating around the maximum power dissipation point. Since internal power dissipation is a function of output power, higher ambient temperatures are allowed as output power or duty cycle decreases. If the result of Equation 2 is greater than that of Equation (3), then decrease the supply voltage, increase the load impedance, or reduce the ambient temperature. Further, ensure that speakers rated at a nominal 8 Ω do not fall below 6 Ω. If these measures are insufficient, a heat sink can be added to reduce θJA. The heat sink can be created using additional copper area around the package, with connections to the ground pins, supply pin and amplifier output pins. Refer to the Typical Performance Characteristics curves for power dissipation information at lower output power levels. POWER SUPPLY VOLTAGE LIMITS Continuous proper operation is ensured by never exceeding the voltage applied to any pin, with respect to ground, as listed in the Absolute Maximum Ratings section. POWER SUPPLY BYPASSING As with any power amplifier, proper supply bypassing is critical for low noise performance and high power supply rejection. Applications that employ a voltage regulator typically use a 10µF in parallel with a 0.1µF filter capacitors to stabilize the regulator's output, reduce noise on the supply line, and improve the supply's transient response. However, their presence does not eliminate the need for a local 1.0µF tantalum bypass capacitance connected between the LM4951's supply pins and ground. Do not substitute a ceramic capacitor for the tantalum. Doing so may cause oscillation. Keep the length of leads and traces that connect capacitors between the LM4951's power supply pin and ground as short as possible. Connecting a larger capacitor, CBYPASS, between the BYPASS pin and ground improves the internal bias voltage's stability and improves the amplifier's PSRR. The PSRR improvements increase as the bypass pin capacitor value increases. Too large, however, increases turn-on time and can compromise the amplifier's click and pop performance. The selection of bypass capacitor values, especially CBYPASS, depends on desired PSRR requirements, click and pop performance (as explained in the section, SELECTING EXTERNAL COMPONENTS), system cost, and size constraints. MICRO-POWER SHUTDOWN The LM4951 features an active-low micro-power shutdown mode. When active, the LM4951's micro-power shutdown feature turns off the amplifier's bias circuitry, reducing the supply current. The low 0.01µA typical shutdown current is achieved by applying a voltage to the SHUTDOWN pin that is as near to GND as possible. A voltage that is greater than GND may increase the shutdown current. There are a few methods to control the micro-power shutdown. These include using a single-pole, single-throw switch (SPST), a microprocessor, or a microcontroller. When using a switch, connect the SPST switch between the shutdown pin and VDD. Select normal amplifier operation by closing the switch. Opening the switch applies GND to the SHUTDOWN pin activating micro-power shutdwon.The switch and internal pull-down resistor ensures that the SHUTDOWN pin will not float. This prevents unwanted state changes. In a system with a microprocessor or a microcontroller, use a digital output to apply the active-state voltage to the SHUTDOWN pin. SELECTING EXTERNAL COMPONENTS Input Capacitor Value Selection Two quantities determine the value of the input coupling capacitor: the lowest audio frequency that requires amplification and desired output transient suppression. As shown in Figure 1, the input resistor (Ri) and the input capacitor (Ci) produce a high pass filter cutoff frequency that is found using Equation 6. fc = 1/2πRiCi (6) Copyright © 2004–2013, Texas Instruments Incorporated Submit Documentation Feedback 13 Product Folder Links: LM4951 |
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