| 数据搜索系统,热门电子元器件搜索 |
|
LM4850MM 数据表(PDF) 12 Page - National Semiconductor (TI) |
|
|
|
|||||||||||||||||||||||||||||
LM4850MM 数据表(HTML) 12 Page - National Semiconductor (TI) |
|
12 / 20 page ![]() Application Information (Continued) amplifier’s closed-loop gain without causing excessive out- put signal clipping, please refer to the Audio Power Ampli- fier Design section. A bridge configuration, such as the one used in LM4850, also creates a second advantage over single-ended amplifi- ers. Since the differential outputs, BTL OUT- and BTL OUT+, are biased at half-supply, no net DC voltage exists across the load. This eliminates the need for the output coupling capacitor that a single supply, single-ended amplifier con- figuration requires. Eliminating an output coupling capacitor in a single-ended configuration forces the half-supply bias voltage across the load. This increases internal IC power dissipation and may cause permanent loudspeaker damage. POWER DISSIPATION Whether the power amplifier is bridged or single-ended, power dissipation is a major concern when designing the amplifier. Equation 2 states the maximum power dissipation point for a single-ended amplifier operating at a given supply voltage and driving a specified load. P DMAX =(VDD) 2/(2 π2 R L): Single-Ended (2) However, a direct consequence of the increased power de- livered to the load by a bridge amplifier is an increase in internal power dissipation. Equation 3 states the maximum power dissipation point for a bridge amplifier operating at the same given conditions. P DMAX = 4x(VDD) 2/(2 π2 R L): Bridge Mode (3) The LM4850 is designed to drive either two single-ended loads simultaneously or one mono bridged-tied load. In SE mode, the maximum internal power dissipation is 2 times that of Equation 2. In BTL mode, the maximum internal power dissipation is the result of Equation 3. Even with this substantial increase in power dissipation, the LM4850 does not require heatsinking. The power dissipation from Equation 3 must not be greater than the power dissipation predicted by Equation 4: P DMAX =(TJMAX -TA)/ θ JA (4) For the package MTC14, θ JA = 150˚C/W, and for the pack- age MUA10A, θ JA = 194˚C/W. T JMAX = 150˚C for the LM4850. Depending on the ambient temperature, T A,ofthe surroundings, Equation 4 can be used to find the maximum internal power dissipation supported by the IC packaging. If the result of Equation 3 is greater than that of Equation 4, then either the supply voltage must be decreased, the load impedance increased, or the ambient temperature reduced. For the typical application of a 5V power supply, and an 8 Ω bridged load, the maximum ambient temperature possible without violating the maximum junction temperature is ap- proximately 55˚C for package MTC14. This assumes the device operates at maximum power dissipation and uses surface mount packaging. Internal power dissipation is a function of output power. If typical operation is not around the maximum power dissipation point, operation at higher ambi- ent temperatures is possible. Refer to the Typical Perfor- mance Characteristics curves for power dissipation infor- mation for different output power levels. POWER SUPPLY BYPASSING As with any power amplifier, proper supply bypassing is critical for low noise performance and high power supply rejection. The capacitor location on both the bypass and power supply pins should be as close to the device as possible. The value of the pin bypass capacitor, C B, directly affects the LM4850’s half-supply voltage stability and PSRR. The stability and supply rejection increase as the bypass capacitor’s value increases Typical applications employ a 5V regulator with a 10µF and a 0.1µF bypass capacitors which aid in supply filtering. This does not eliminate the need for bypassing the supply nodes of the LM4850. The selection of bypass capacitors, especially C B, is thus dependent upon desired PSRR requirements, click and pop performance, system cost, and size constraints. SHUTDOWN FUNCTION In order to reduce power consumption while not in use, the LM4850 features amplifier bias circuitry shutdown. This shut- down function is activated by applying a logic high to the SHUTDOWN pin. The trigger point is 2.0V minimum for a logic high level, and 0.8V maximum for a logic low level. It is best to switch between ground and the supply, V DD,to ensure correct shutdown operation. By switching the SHUT- DOWN pin to V DD, the LM4850 supply current draw will be minimized in idle mode. Whereas the device will be disabled with shutdown voltages less than V DD, the idle current may be greater than the typical value of 44µA. In either case, the SHUTDOWN pin should be tied to a fixed voltage to avoid unwanted state changes. In many applications, a microcontroller or microprocessor output is used to control the shutdown circuitry. This provides a quick, smooth shutdown transition. Another solution is to use a single-pole, single-throw switch in conjunction with an external pull-up resistor. When the switch is closed, the SHUTDOWN pin is connected to ground and enables the amplifier. If the switch is open, the external pull-up resistor, R PU2 will disable the LM4850. This scheme guarantees that the SHUTDOWN pin will not float, thus preventing unwanted state changes. HP-IN FUNCTION The LM4850 features a headphone control pin, HP-IN, that enables the switching between BTL and SE modes. A logic-low to HP-IN activates the BTL mode, while a logic-high activates the SE mode. Figure 2 shows the implementation of the LM4850’s head- phone control. The voltage divider formed by R PU1 and RD1 sets the voltage at HP-IN to be approximately 50mV with no headphones plugged into the system. This logic-low voltage at the HP-IN pin enables the BTL mode When a set of headphones is plugged into the system, the headphone jack’s contact pin is disconnected from the signal pin. This also interrupts the voltage divider set up by the resistors R PU1 and RD1. Resistor RPU1 applies VDD to the HP-IN pin, switching the LM4850 out of BTL mode and into SE mode. The amplifier then drives the headphones, whose impedance is in parallel with resistors R D1 and RD2. Resis- tors R D1 and RD2 have negligible effect on the output drive capability since the typical impedance of headphones is 32 Ω. www.national.com 12 |
|
|
链接网址 |
| ALLDATASHEET是否为您带来帮助? [ DONATE ] |
关于 Alldatasheet | 广告服务 | 联系我们 | 隐私政策 | 数据表链接 | 链接交换 | 制造商名单 All Rights Reserved©Alldatasheet.com |
| Russian : Alldatasheetru.com | Korean : Alldatasheet.co.kr | Spanish : Alldatasheet.es | French : Alldatasheet.fr | Italian : Alldatasheetit.com Portuguese : Alldatasheetpt.com | Polish : Alldatasheet.pl | Vietnamese : Alldatasheet.vn Indian : Alldatasheet.in | Mexican : Alldatasheet.com.mx | British : Alldatasheet.co.uk | New Zealand : Alldatasheet.co.nz |
|
Family Site : ic2ic.com |
icmetro.com |