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INA337 Datasheet(PDF) 10 Page - Texas Instruments |
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INA337 Datasheet(HTML) 10 Page - Texas Instruments |
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10 / 14 page ![]() INA337, INA338 10 SBOS222A www.ti.com Following this design procedure for R1 produces the maxi- mum possible input stage gain for best accuracy and lowest noise. Circuit layout and supply bypassing can affect performance. Minimize the stray capacitance on pins 1 and 8. Use recom- mended supply bypassing, including a capacitor directly from pin 7 to pin 4 (V+ to V–), even with dual (split) power supplies (see Figure 1). DYNAMIC PERFORMANCE The typical characteristic “Gain vs Frequency” shows that the INA337 has nearly constant bandwidth regardless of gain. This results from the bandwidth limiting from the recom- mended filters. NOISE PERFORMANCE Internal auto-correction circuitry eliminates virtually all 1/f noise (noise that increases at low frequency) in gains of 100 or greater. Noise performance is affected by gain-setting resistor values. Follow recommendations in the “Setting Gain” section for best performance. Total noise is a combination of input stage noise and output stage noise. When referred to the input, the total mid-band noise is: VnV Hz nV Hz G N =+ 33 800 / / (3) The output noise has some 1/f components that affect performance in gains less than 10. See typical characteristic “Input-Referred Voltage Noise vs Frequency.” High-frequency noise is created by internal auto-correction circuitry and is highly dependent on the filter characteristics chosen. This may be the dominant source of noise visible when viewing the output on an oscilloscope. Low cutoff frequency filters will provide lowest noise. Figure 2 shows the typical noise performance as a function of cutoff frequency. Applications sensitive to the spectral characteristics of high- frequency noise may require consideration of the spurious frequencies generated by internal clocking circuitry. “Spurs” occur at approximately 90kHz and its harmonics (see typical characteristic “Input Referred Ripple”) which may be reduced by additional filtering below 1kHz. Insufficient filtering at pin 5 can cause nonlinearity with large output voltage swings (very near the supply rails). Noise must be sufficiently filtered at pin 5 so that noise peaks do not “hit the rail” and change the average value of the signal. Figure 2 shows guidelines for filter cutoff frequency. HIGH-FREQUENCY NOISE C2 and CO form filters to reduce internally generated auto- correction circuitry noise. Filter frequencies can be chosen to optimize the tradeoff between noise and frequency response of the application, as shown in Figure 2. The cutoff frequen- cies of the filters are generally set to the same frequency. Figure 2 shows the typical output noise for four gains as a function of the –3dB cutoff frequency of each filter response. Small signals may exhibit the addition of internally generated auto-correction circuitry noise at the output. This noise, combined with broadband noise, becomes most evident in higher gains with filters of wider bandwidth. INPUT BIAS CURRENT RETURN PATH The input impedance of the INA337 is extremely high— approximately 1010 Ω. However, a path must be provided for the input bias current of both inputs. This input bias current is approximately ±0.2nA. High input impedance means that this input bias current changes very little with varying input voltage. Input circuitry must provide a path for this input bias current for proper operation. Figure 3 shows provisions for an input bias current path in a thermocouple application. Without a bias current path, the inputs will float to an undefined poten- tial and the output voltage may not be valid. FIGURE 2. Total Output Noise vs Filter Cutoff Frequency. 100 1 10 1k 10k Required Filter Cutoff Frequency (Hz) 1k 100 10 1 G = 10 G = 1 G = 100 G = 1000 INA337 Thermocouple 5 FIGURE 3. Providing Input Bias Current Return Path. |
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