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LM4701 Datasheet(PDF) 12 Page - National Semiconductor (TI) |
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LM4701 Datasheet(HTML) 12 Page - National Semiconductor (TI) |
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12 / 15 page ![]() Application Information (Continued) the fault condition is temporary, but a sustained fault will cause the device to cycle in a Schmitt Trigger fashion be- tween the thermal shutdown temperature limits of 165˚C and 155˚C. This greatly reduces the stress imposed on the IC by thermal cycling, which in turn improves its reliability under sustained fault conditions. Since the die temperature is directly dependent upon the heat sink used, the heat sink should be chosen such that thermal shutdown will not be reached during normal opera- tion. Using the best heat sink possible within the cost and space constraints of the system will improve the long-term reliability of any power semiconductor device, as discussed in the Determining the Correct Heat Sink Section. DETERMINING MAXIMUM POWER DISSIPATION Power dissipation within the integrated circuit package is a very important parameter requiring a thorough understand- ing if optimum power output is to be obtained. An incorrect maximum power dissipation calculation may result in inad- equate heat sinking causing thermal shutdown and thus lim- iting the output power. Equation (1) exemplifies the theoretical maximum power dis- sipation point of each amplifier where V CC is the total supply voltage. P DMAX = VCC 2/2 π2R L (1) Thus by knowing the total supply voltage and rated output load, the maximum power dissipation point can be calcu- lated. Refer to the graphs of Power Dissipation vs Output Power in the Typical Performance Characteristics section which show the actual full range of power dissipation not just the maximum theoretical point that results from equation (1). DETERMINING THE CORRECT HEAT SINK The choice of a heat sink for a high-power audio amplifier is made entirely to keep the die temperature at a level such that the thermal protection circuitry does not operate under normal circumstances. The thermal resistance from the die (junction) to the outside air (ambient) is a combination of three thermal resistances, θ JC, θCS and θSA. The thermal resistance, θJC (junction to case), of the LM4701 is 2˚C/W. Using Thermalloy Therma- cote thermal compound, the thermal resistance, θ CS (case to sink), is about 0.2˚C/W. Since convection heat flow (power dissipation) is analogous to current flow, thermal resistance is analogous to electrical resistance, and temperature drops are analogous to voltage drops, the power dissipation out of the LM4701 is equal to the following: P DMAX = (TJMAX −TAMB)/θJA (2) where T JMAX = 150˚C, TAMB is the system ambient tempera- ture and θ JA = θJC + θCS + θSA. Once the maximum package power dissipation has been calculated using equation (1), the maximum thermal resis- tance, θ SA, (in ˚C/W) for a heat sink can be calculated. This calculation is made using equation (3) which is derived by solving for θ SA in equation (2). θ SA=[(TJMAX−TAMB)−PDMAX(θJC+θCS)]/PDMAX (3) Again it must be noted that the value of θ SA is dependent upon the system designer’s amplifier requirements. If the ambient temperature that the audio amplifier is to be working under is higher than 25˚C, then the thermal resistance for the heat sink, given all other things are equal, will need to be smaller. SUPPLY BYPASSING The LM4701 has excellent power supply rejection and does not require a regulated supply. However, to improve system performance as well as eliminate possible oscillations, the LM4701 should have its supply leads bypassed with low-inductance capacitors having short leads that are lo- cated close to the package terminals. Inadequate power supply bypassing will manifest itself by a low frequency oscil- lation known as “motorboating” or by high frequency insta- bilities. These instabilities can be eliminated through multiple bypassing utilizing a large tantalum or electrolytic capacitor (10 µF or larger) which is used to absorb low frequency variations and a small ceramic capacitor (0.1 µF) to prevent any high frequency feedback through the power supply lines. If adequate bypassing is not provided, the current in the sup- ply leads which is a rectified component of the load current may be fed back into internal circuitry. This signal causes distortion at high frequencies requiring that the supplies be bypassed at the package terminals with an electrolytic ca- pacitor of 470 µF or more. BRIDGED AMPLIFIER APPLICATION One common power amplifier configuration is shown in Fig- ure 2 and is referred to as “bridged mode” operation. Bridged mode operation is different from the classical single-ended amplifier configuration where one side of the output load is connected to ground. A bridge amplifier design has a distinct advantage over the single-ended configuration, as it provides differential drive to the load, thus doubling output swing for a specified supply voltage. Consequently, theoretically four times the output power is possible as compared to a single-ended amplifier under the same conditions. This increase in attainable output power assumes that the amplifier is not current limited or clipped. A direct consequence of the increased power delivered to the load by a bridge amplifier is an increase in internal power dissipation. For each operational amplifier in a bridge con- figuration, the internal power dissipation will increase by a factor of two over the single ended dissipation. Since there are two amplifiers used in a bridge configuration, the maxi- mum system power dissipation point will increase by a factor of four over the figure obtained by equation (1). This value of P DMAX can be used to calculate the correct size heat sink for a bridged amplifier application, assuming that both IC’s are mounted on the same heatsink. Since the inter- nal dissipation for a given power supply and load is in- creased by using bridged-mode, the heatsink’s θ SA will have to decrease accordingly as shown by equation (3). Refer to the section, Determining the Correct Heat Sink, for a more detailed discussion of proper heat sinking for a given appli- cation. SINGLE-SUPPLY AMPLIFIER APPLICATION The typical application of the LM4701 is a split supply ampli- fier. But as shown in Figure 3, the LM4701 can also be used in a single power supply configuration. This involves using some external components to create a half-supply bias which is used as the reference for the inputs and outputs. Thus, the signal will swing around half-supply much like it swings around ground in a split-supply application. Along with proper circuit biasing, a few other considerations must be accounted for to take advantage of all of the LM4701 functions. www.national.com 12 |
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