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OPT209 Datasheet(PDF) 7 Page - Burr-Brown (TI) |
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OPT209 Datasheet(HTML) 7 Page - Burr-Brown (TI) |
7 / 11 page 7 ® OPT209 APPLICATIONS INFORMATION Figure 1 shows the basic connections required to operate the OPT209. Applications with high-impedance power supplies may require decoupling capacitors located close to the device pins as shown. Output is zero volts with no light and increases with increasing illumination. metal, and differential stages are cross-coupled. Furthermore, the photodiode area is very large relative to the op amp input circuitry making these effects negligible. If your light source is focused to a small area, be sure that it is properly aimed to fall on the photodiode. If a narrowly focused light source were to miss the photodiode area and fall only on the op amp circuitry, the OPT209 would not perform properly. The large (0.090 x 0.090 inch) photodiode area allows easy positioning of narrowly focused light sources. The photodiode area is easily visible—it appears very dark compared to the surrounding active circuitry. The incident angle of the light source also affects the apparent sensitivity in uniform irradiance. For small incident angles, the loss in sensitivity is simply due to the smaller effective light gathering area of the photodiode (proportional to the cosine of the angle). At a greater incident angle, light is diffused by the side of the package. These effects are shown in the typical performance curve “Response vs Incident Angle.” Photodiode current, I D, is proportional to the radiant power or flux (in watts) falling on the photodiode. At a wavelength of 650nm (visible red) the photodiode Responsivity, R I, is approximately 0.45A/W. Responsivity at other wavelengths is shown in the typical performance curve “Responsivity vs Wavelength.” The typical performance curve “Output Voltage vs Radiant Power” shows the response throughout a wide range of radiant power. The response curve “Output Voltage vs Irradiance” is based on the photodiode area of 5.23 x 10–6m2. The OPT209’s voltage output is the product of the photodiode current times the feedback resistor, (I DRF). The internal feedback resistor is laser trimmed to 1M Ω ±2%. Using this resistor, the output voltage responsivity, R V, is approximately 0.45V/ µW at 650nm wavelength. An external resistor can be connected to set a different voltage responsivity. Best dynamic performance is achieved by connecting REXT in series (for RF > 1MΩ), or in parallel (for RF < 1MΩ), with the internal resistor as shown in Figure 2. These connections take advantage of on-chip capacitive guarding of the internal resistor, which improves dynamic performance. For values of R F less than 1MΩ, an external capacitor, CEXT, should be connected in parallel with R F (see Figure 2). This capacitor eliminates gain peaking and prevents instability. The value of CEXT can be read from the table in Figure 2. LIGHT SOURCE POSITIONING The OPT209 is 100% tested with a light source that uniformly illuminates the full area of the integrated circuit, including the op amp. Although all IC amplifiers are light-sensitive to some degree, the OPT209 op amp circuitry is designed to minimize this effect. Sensitive junctions are shielded with ID is proportional to light intensity (radiant power). 1M Ω OPT209 10pF 175 Ω 2 83 5 4 1 V O –15V +15V 0.1µF 0.1µF V O = ID RF R F I D I D (0V) λ FIGURE 1. Basic Circuit Connections. FIGURE 2. Using External Feedback Resistor. EQUIVALENT RF CEXT 100M Ω (1) 10M Ω (1) 1M Ω (1) 330k Ω (1)pF 100k Ω 9pF 33k Ω 25pF ≤20kΩ (2) NOTES: (1) No CEXT required. (2) Not recommended due to possible op amp instability. 1M Ω OPT209 3pF 175 Ω 83 5 4 1 V O = ID RF V– λ V+ R EXT C EXT 2 R F = REXT || 1MΩ For R F < 1MΩ 1M Ω OPT209 175 Ω 5 4 V O = ID RF V– λ V+ 2 R F = REXT + 1MΩ For R F > 1MΩ R EXT |
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