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LM95221 Datasheet(PDF) 14 Page - National Semiconductor (TI) |
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LM95221 Datasheet(HTML) 14 Page - National Semiconductor (TI) |
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14 / 16 page ![]() 3.0 Applications Hints The LM95221 can be applied easily in the same way as other integrated-circuit temperature sensors, and its remote diode sensing capability allows it to be used in new ways as well. It can be soldered to a printed circuit board, and be- cause the path of best thermal conductivity is between the die and the pins, its temperature will effectively be that of the printed circuit board lands and traces soldered to the LM95221’s pins. This presumes that the ambient air tem- perature is almost the same as the surface temperature of the printed circuit board; if the air temperature is much higher or lower than the surface temperature, the actual tempera- ture of the LM95221 die will be at an intermediate tempera- ture between the surface and air temperatures. Again, the primary thermal conduction path is through the leads, so the circuit board temperature will contribute to the die tempera- ture much more strongly than will the air temperature. To measure temperature external to the LM95221’s die, use a remote diode. This diode can be located on the die of a target IC, allowing measurement of the IC’s temperature, independent of the LM95221’s temperature. The LM95221 has been optimized to measure the remote thermal diode with a non-ideality of 1.008 and a series resistance of 2.7 Ω. The thermal diode on the Pentium 4 processor on the 90 nm process has a typical non-ideality of 1.011 and a typical series resistance of 3.33 Ω. Therefore, when measuring this thermal diode with the LM95221 a typical offset of +1.5˚C will be observed. This offset can be compensated for easily by subracting 1.5˚C from the LM95221’s readings. A discrete diode can also be used to sense the temperature of external objects or ambient air. Remember that a discrete diode’s temperature will be affected, and often dominated, by the temperature of its leads. Most silicon diodes do not lend themselves well to this application. It is recommended that a 2N3904 transistor base emitter junction be used with the collector tied to the base. When measuring a diode-connected 2N3904, with an LM95221, an offset of -3.25˚C will be observed. This offset can simply be added to the LM95221’s reading: T 2N3904 = T LM95221 + 3.25˚C 3.1 DIODE NON-IDEALITY 3.1.1 Diode Non-Ideality Factor Effect on Accuracy When a transistor is connected as a diode, the following relationship holds for variables V BE, T and If: where: • q = 1.6x10 −19 Coulombs (the electron charge), • T = Absolute Temperature in Kelvin • k = 1.38x10 −23joules/K (Boltzmann’s constant), • η is the non-ideality factor of the process the diode is manufactured on, • I S = Saturation Current and is process dependent, • I f= Forward Current through the base emitter junction • V BE = Base Emitter Voltage drop In the active region, the -1 term is negligible and may be eliminated, yielding the following equation In the above equation, η and I S are dependant upon the process that was used in the fabrication of the particular diode. By forcing two currents with a very controlled ratio (N) and measuring the resulting voltage difference, it is possible to eliminate the I S term. Solving for the forward voltage difference yields the relationship: The voltage seen by the LM95221 also includes the I FRS voltage drop of the series resistance. The non-ideality factor, η, is the only other parameter not accounted for and de- pends on the diode that is used for measurement. Since ∆V BE is proportional to both η and T, the variations in η cannot be distinguished from variations in temperature. Since the non-ideality factor is not controlled by the tempera- ture sensor, it will directly add to the inaccuracy of the sensor. For the Pentium 4 and Mobile Pentium Processor-M Intel specifies a ±0.1% variation in η from part to part. As an example, assume a temperature sensor has an accuracy specification of ±1˚C at room temperature of 25 ˚C and the process used to manufacture the diode has a non-ideality variation of ±0.1%. The resulting accuracy of the tempera- ture sensor at room temperature will be: T ACC = ± 1˚C+(±0.1% of 298 ˚K) = ±1.4 ˚C The additional inaccuracy in the temperature measurement caused by η, can be eliminated if each temperature sensor is calibrated with the remote diode that it will be paired with. Processor Family η, non-ideality Series R min typ max Pentium II 1 1.0065 1.0173 Pentium III CPUID 67h 1 1.0065 1.0125 Pentium III CPUID 68h/PGA370Socket/Celeron 1.0057 1.008 1.0125 Pentium 4, 423 pin 0.9933 1.0045 1.0368 Pentium 4, 478 pin 0.9933 1.0045 1.0368 Pentium 4 on 0.13 micron process, 2-3.06GHz 1.0011 1.0021 1.0030 3.64 Ω Pentium 4 on 90 nm process 1.011 3.33 Ω Pentium M Processor (Centrino) 1.00151 1.00220 1.00289 3.06 Ω MMBT3904 1.003 AMD Athlon MP model 6 1.002 1.008 1.016 www.national.com 14 |
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