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LMH6672LD Datasheet(PDF) 12 Page - National Semiconductor (TI) |
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LMH6672LD Datasheet(HTML) 12 Page - National Semiconductor (TI) |
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12 / 14 page ![]() Application Notes Thermal Management The LMH6672 is a high-speed, high power, dual operational amplifier with a very high slew rate and very low distortion. For ease of use, it uses conventional voltage feedback. These characteristics make the LMH6672 ideal for applica- tions where driving low impedances of 25-100 Ω such as xDSL and active filters. A class AB output stage allows the LMH6672 to deliver high currents to low impedance loads with low distortion while consuming low quiescent supply current. For most op-amps, class AB topology means that internal power dissipation is rarely an issue, even with the trend to smaller surface mount packages. However, the LMH6672 has been designed for applications where high levels of power dissipation may be encountered. Several factors contribute to power dissipation and conse- quently higher junction temperatures. These factors need to be well understood if the LMH6672 is to perform to specifi- cations in all applications. This section will examine the typical application that is shown on the front page of this data sheet as an example. (Figure 1) Because both amplifiers are in a single package, the calculations will for the total power dissipated by both amplifiers. There are two separate contributors to the internal power dissipation: 1. The product of the supply voltage and the quiescent current when no signal is being delivered to the external load. 2. The additional power dissipated while delivering power to the external load. The first of these components appears easy to calculate simply by inspecting the data sheet. The typical quiescent supply current for this part is 6.2mA per amplifier, therefore, with a (6 volt supply, the total power dissipation is: P D =VS x2xlQ = 12 x (12.4x10 -3) = 149 mW (V S =VCC +VEE) With a thermal resistance of 172˚C/W for the SOIC package, this level of internal power dissipation will result in a junction temperature (T J) of 26˚C above ambient. Using the worst-case maximum supply current of 18mA and an ambient of 85˚C, a similar calculation results in a power dissipation of 216 mW, or a T J of 122˚C. This is approaching the maximum allowed T J of 150˚C be- fore a signal is applied. Fortunately, in normal operation, this term is reduced, for reasons that will soon be explained. The second contributor to high T J is the power dissipated internally when power is delivered to the external load. This cause of temperature rise is more difficult to calculate, even when the actual operating conditions are known. To maintain low distortion, in a Class AB output stage, an idle current, I Q, is maintained through the output transistors when there is little or no output signal. In the LMH6672, about 4.8 mA of the total quiescent supply current of 12.4 mA flows through the output stages. Under normal large signal conditions, as the output voltage swings positive, one transistor of the output pair will conduct the load current, while the other transistor shuts off, and dissipates no power. During the negative signal swing this situation is reversed, with the lower transistor sinking the load current while the upper transistor is cut off. The current in each transistor will approximate a half wave rectified version of the total load current. Because the output stage idle current is now routed into the load, 4.8mA can be subtracted from the quiescent supply current when calculating the quiescent power when the out- put is driving a load. The power dissipation caused by driving a load in a DSL application, using a 1:2 turns ratio transformer driving 20 mW into the subscriber line and 20mW into the back termi- nation resistors, can be calculated as follows: P DRIVER =PTOT –(PTERM +PLINE) where P DRIVER is the LMH6672 power dissipation P TOT is the total power drawn from the power supply P TERM is the power dissipated in the back termination resis- tors P LINE is the power sent into the subscriber line At full specified power, P TERM =PLINE = 20mW, PTOT =VS xI S. In this application, V S = 12V. I S =IQ +AVG |IOUT|. I Q = the LMH6672 quiescent current minus the output stage idle current. I Q = 12.4 - 4.8 = 7.6mA A VG |IOUT| for a full-rate ADSL CPE application, using a 1:2 turns ratio transformer, is = 28.28mA RMS. For a Gaussian signal, which the DMT ADSL signal approxi- mates, A VG |IOUT|= = 22.6mA. Therefore, P TOT = (22.6mA + 7.6mA) x 12V = 362mW and P DRIVER is 362-40 = 322mW. In the SOIC package, with a θ JA of 172˚C/W, this causes a temperature rise of 55˚C. With an ambient temperature at the maximum recommended 85˚C, the T J is at 140˚C, well below the specified 150˚C maximum. Even if we assume the absolute maximum I S over tempera- ture of 18mA, when we scale up the I Q proportionally to 7mA, the P DRIVER only goes up by 41mW causing a 62˚C rise to 147˚C. Although very few CPE applications will ever operate in an environment as hot as 85˚C, if a lower T J is desired or the LMH6672 is to be used in an application where the power dissipation is higher, the PSOP package provides a much lower θ JA of only 58.6˚C/W. Using the same P DRIVER as above, we find that the tempera- ture rise is only 19˚ and 21˚C, resulting in T J’s in an 85˚C ambient of 104˚C and 106˚C respectively. Circuit Layout Considerations National Semiconductor suggests the following evaluation boards as a guide for high frequency layout and as an aid in device testing and characterization. Since the exposed PAD (or DAP) of the PSOP and LLP package is internally floating, the footprint for DAP could be connected to ground plane in PCB for better heat dissipation. Device Package Evaluation Board PN LMH6672MA 8-Pin SOIC CLC730036 LMH6672LD 8-Pin LLP CLC730114 LMH6672MR 8-Pin PSOP CLC730121 These free evaluation boards are shipped when a device sample request is placed with National Semiconductor. www.national.com 12 |
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