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LOG102 数据表(PDF) 6 Page - Texas Instruments |
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LOG102 数据表(HTML) 6 Page - Texas Instruments |
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6 / 13 page ![]() www.ti.com LOG102 6 SBOS211A 14 I 1 I 2 1 10 8 11 3 12 7 4 5 6 V+ 9 V– 10 µF Amplifier A 4 not being used. C C 10 µF LOG102 V OUT R 2 V LOGOUT V OUT = G • VLOGOUT R 1 1000pF 1000pF Unused amplifiers should have positive inputs grounded and negative inputs tied to their respective outputs. FIGURE 1. Basic Connections with Output Gain Factor of the LOG102. APPLICATION INFORMATION The LOG102 is a true logarithmic amplifier that uses the base-emitter voltage relationship of bipolar transistors to compute the logarithm, or logarithmic ratio of a current ratio. With two uncommitted on-chip operational amplifiers, the LOG102 provides design flexibility and simplicity. Figure 1 shows the basic connections required for operation of the LOG102 with a gain factor. In order to reduce the influence of lead inductance of power supply lines, it is recommended that each supply be bypassed with a 10 µF tantalum capacitor in parallel with a 1000pF ceramic capaci- tor, as shown in Figure 1. Connecting the capacitors as close to the LOG102 as possible will contribute to noise reduction as well. INPUT CURRENT RANGE To maintain specified accuracy, the input current range of the LOG102 should be limited from 1nA to 1mA. Input currents outside of this range may compromise LOG102 performance. Input currents larger than 1mA result in increased nonlinearity. An absolute maximum input current rating of 10mA is included to prevent excessive power dissipation that may damage the logging transistor. On ±5V supplies the total input current (I 1 + I2) is limited to 1.1mA. Due to compliance issues internal to the LOG102, to accommodate larger total input currents, supplies should be increased. Currents smaller than 1nA will result in increased errors due the input bias currents of op amps A1 and A2 (typically 5pA). The input bias currents may be compensated for, as shown in Figure 2. The input stages of the amplifiers have FET inputs, with input bias current doubling every 10 °C, which makes the nulling technique shown practical only where the temperature is fairly stable. FIGURE 2. Bias Current Nulling. V– R 1' > 1M Ω I 2 I 1 R 2' 10k Ω R 1 1M Ω R 2 10k Ω V+ 14 1 9 10 5 V OUT 6 V– V+ C C LOG102 2N2905 I REF R REF 2N2905 +15V –15V I REF = 6V R REF 3.6k Ω 6V IN834 FIGURE 3. Temperature Compensated Current Source. SETTING THE REFERENCE CURRENT When the LOG102 is used to compute logarithms, either I1 or I2 can be held constant and becomes the reference current to which the other is compared. VLOGOUT is expressed as: VLOGOUT = (1V) • log (I1/I2) (1) IREF can be derived from an external current source (such as shown in Figure 3), or it may be derived from a voltage source with one or more resistors. When a single resistor is used, the value may be large depending on IREF. If IREF is 10nA and +2.5V is used: RREF = 2.5V/10nA = 250MΩ A 1 + R 2 R 1 +5V R 3 V REF = 100mV R 3 >> R2 I REF – V OS 14 FIGURE 4. T Network for Reference Current. A voltage divider may be used to reduce the value of the resistor (as shown in Figure 4). When using this method, one must consider the possible errors caused by the amplifier’s input offset voltage. The input offset voltage of amplifier A1 has a maximum value of 1.5mV, making VREF a suggested value of 100mV. |
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