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ISL29002 Datasheet(PDF) 8 Page - Intersil Corporation |
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ISL29002 Datasheet(HTML) 8 Page - Intersil Corporation |
8 / 10 page 8 FN7465.2 December 1, 2006 integration is no longer fixed at 32,768, but varies with the chosen integration time, and is limited to 65,536. In order to avoid erroneous lux readings the integration must be short enough not to allow an overflow in the counter register. where: Tint = user defined integration time fosc = 300kHz*100kΩ/REXT. ISL29002’s internal oscillator. Not to be confused with the I2C’s frequency. REXT = user defined external resistor to adjust fosc. 100kΩ recommended. The number of clock cycles in the previous integration period is provided in the third and fourth bytes of data read across the I2C bus. This two-byte value is called the integration counter value. When using one of the three external timing modes, the ISL29002’s resolution varies with the integration time. The resolution is determined by the ratio of the max lux range to the number of clock cycles per integration. The following equations describe the light intensity as a function of sensor reading, integration counter value, and integration time: Tint = Time Interval between external time commands where L is the measured light intensity, Data1 is the sensor reading, Data2 is the integration counter value, T is the integration time, and REXT is external resistor value. Noise Rejection and Integration Time In general, integrating type ADC’s have an excellent noise- rejection characteristics for periodic noise sources whose frequency is an integer multiple of the integration time. For instance, a 60Hz AC unwanted signal’s sum from 0ms to n*16.66ms (n = 1,2...ni) is zero. Similarly, setting the ISL29002’s integration time to an integer multiple of periodic noise signal greatly improves the light sensor output signal in the presence of noise. The integration time, Tint, of the ISL29002 is set by an external resistor REXT. See Equation 3. Design Example 1 Using the ISL29002, determine a suitable integration time, Tint, that will ignore the presence of both 60Hz and 50Hz noise. Accordingly, specify the REXT value. Given that the I2C clock is at fI2C = 10kHz. Solution 1 - Using Internal Timing Tint = n(1/60Hz) = m(1/50Hz). In order to achieve both 60Hz and 50Hz AC rejection, the integration time needs to be adjusted to coincide with an integer multiple of the AC noise cycle times. n/m = 60Hz/50Hz = 6/5. The first instance of integer values at which Tint rejects both 60Hz and 50Hz is when m = 5, and n = 6. Tint = 6(1/60Hz) = 5(1/50Hz) = 100ms From Equation 3: REXT = Tint * (100kΩ/110ms) = 90.9kΩ. By populating REXT =90kΩ, the ISL29002 defaults to 100ms integration time and will reject the presence of both 60Hz and 50Hz power line signals. Solution 2 - Using External Timing From solution 1, the desired integration time is 100ms. Note that the REXT resistor does not determine the integration time when using external timing mode. Instead, the integration and the 16-bit counter starts when an external timing mode command is sent and end when another external timing mode is sent. In other words, the time between two external timing mode command is the integration time. The programmer determines how many clock cycles to wait between two external timing commands. iI2C = fI2C * Tint, where iI2C = number of I 2C cycles iI2C = 10kHz *100ms iI2C = 1,000 I 2C clock cycles. An external timing command 1,000 cycles after another external timing command rejects both 60Hz and 50Hz AC noise signals. IR Rejection Any filament type light source has a high presence of infrared component invisible to the human eye. A white fluorescent lamp, on the other hand has a low IR content. As a result, output sensitivity may vary depending on the light source. Maximum attenuation of IR can be achieved by properly scaling the readings of Diode1 and Diode2. The user obtains data reading from sensor diode 1, D1, which is sensitive to visible and IR, then reading from sensor diode 2, D2 which is mostly sensitive from IR. The graph on Figure 9 shows the effective spectral response after applying Equation 7 of the ISL29002 from 400nm to 1000nm. The equation below describes the method of cancelling IR in internal timing mode. Where: data = lux amount in number of counts less IR presence D1 = data reading of Diode 1 D2 = data reading of Diode 2 n = 1.85. This is a fudge factor to scale back the sensitivity up to ensure Equation 2 is valid. k = 7.5. This is a scaling factor for the IR sensitive Diode 2. T int 65,536 f OSC ------------------ < (EQ. 5) Elux () 50 000lux , R EXT 100 kΩ ⁄ () ------------------------------------------- Data1 Data2 ----------------- ⋅ = (EQ. 6) D3 n D1 kD2 – () = (EQ. 7) ISL29002 |
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