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MICRF230 Datasheet(PDF) 12 Page - Micrel Semiconductor |
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MICRF230 Datasheet(HTML) 12 Page - Micrel Semiconductor |
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12 / 20 page ![]() Micrel, Inc. MICRF230 MICRF230, ensure that the power level remains constant throughout the transmit burst. The value of AGC impacts the period between the TTGD, which is defined as the time when signal is first applied, to the pulse width at DO, within 10% of the steady state value. The optimal value of AGC depends on the setting of the D4 and D3 bits. A smaller AGC value does not always result in a shorter TTGD. This is due to the loop dynamics, the fast discharge current being 600µA, and the charge current being only 1.5µA. For example, if SEL0 = SEL1 = 0, the low pass filter bandwidth is set to a minimum and the AGC capacitance is too small. The TTGD will be longer than if AGC capacitance is properly chosen. This is because when the RF signal first appears, the fast discharge period will reduce VAGC very fast, lowering the gain of the mixer and IF amplifier. Since the low pass filter bandwidth is low, it takes too long for the AGC comparator to see a reduced level of the audio signal, and cannot stop the discharge current. This causes an undershoot in AGC voltage and a corresponding overshoot in RSSI voltage. Once the AGC undershoots, it takes a long time for it to charge back up because the current available is only 1.5µA. Table 2 lists the recommended minimum AGC values for different SEL0 and SEL1 settings to insure that the voltage on AGC does not undershoot. Table 2. Minimum Suggested AGC Values SEL0 SEL1 AGC value 0 0 4.7 μF 0 1 2.2 μF 1 0 1 μF 1 1 1 μF Figure 4 illustrates what occurs if AGC is too small for a given bandwidth setting. In this instance, SEL0 = 1, SEL1 = 0, AGC = 0.47 μF, and the RF input level is stepped from no signal to −100dBm. RSSI voltage is shown in place of AGC voltage because RSSI is a buffered version of AGC with an inversion and amplification. Probing AGC directly can affect the loop dynamics through resistive loading from a scope probe, especially in the state where only 1.5 μA is available, whereas probing RSSI does not. When the RF signal is first applied, RSSI voltage overshoots due to the fast discharge current on AGC, and the loop is too slow to stop this fast discharge current in time. Since the voltage on AGC is too low, the audio signal level is lower than the slicing threshold (voltage on CTH), and DO pin is low. Once the fast discharge current stops, only the small 1.5µA charge current is available in settling the AGC loop to the correct level, causing the recovery from AGC undershoot/RSSI overshoot condition to be slow. As a result, TTGD is about 9.1ms. It is recommended that Tantalum caps or high voltage ceramic caps are used for AGC to minimize capacitor leakage current which may affect the performance of the AGC. Figure 4. RSSI Overshoot and Slow TTGD (9.1ms) Figure 5 shows the behavior with a larger capacitor on AGC pin (2.2 μF), SEL0:SEL1 = 10. In this case, V AGC does not undershoot (RSSI does not overshoot), and TTGD is relatively short at 1ms. Figure 5. Proper TTGD (1ms) with Sufficient AGC Reference Oscillator The reference oscillator in the MICRF230, shown in Figure 6, uses a basic Pierce crystal oscillator April 15, 2015 12 Revision 2.0 |
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