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MICRF405 Datasheet(PDF) 31 Page - Micrel Semiconductor |
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MICRF405 Datasheet(HTML) 31 Page - Micrel Semiconductor |
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31 / 46 page ![]() Micrel MICRF405 April 2006 31 M9999-041906 (408) 955-1690 The two first blocks are generating a clock for the modulator. This clock is, together with the user data, used to control a charge pump. The charge pump current is controlled by a DAC. Each time the input data changes state, a charge is then injected into the capacitor to generate a modulation signal. The charge magnitude is controlled by the charging current and by charging time (inversely proportional with modulator clock). To be able to achieve small deviations, it is possible to attenuate the modulation signal. Finally, the signal is filtered to narrow transmitter output spectrum. The procedure is first to determine the settings concerning the data bit rate, then, these values will be used in the calculation of the frequency deviation. Finally, the user must see if the desired values cause the modulator to saturate. Deviation Setting Deviation controlled by user parameters FSKClk_K, MOD_I, and MOD_A, together with physical parameters fXTAL and KVCO. All user parameters can be set in software, and fXTAL (crystal oscillator frequency) is set when designing in the radio chip. KVCO (VCO gain) is a parameter of the radio chip, and is not controllable by the user. The crystal oscillator frequency, fXTAL, is divided by FSKClk_K to generate the modulator clock. Since this modulator clock is controlling the rise and fall times for the modulator, the frequency deviation is inversely proportional to this clock. The relationship is shown in equation (3): XTAL DEV f FSKClk_K f ∝ (3) It is assumed that FSKClk_K will be constant for most applications to keep bit-rate and shaping constant, although this is not a requirement. The primary two controls of frequency deviation are MOD_I and MOD_A. Of these two, MOD_I is the parameter that controls the signal generation, while MOD_A controls attenuation of this signal. The reason for using an attenuator is to be able to generate small deviations at high values of FSKClk_K. The relationship is shown in equation (4). A MOD DEV I MOD f _ 2 _ ∝ (4) Finally, the VCO gain is given by equation (5). () () FreqBand FreqBand f Const Const K C VCO − − ⋅ ⋅ + = 3 3 2 1 (5) where: Const1 9 10 6324 . 30 × − Const2 7 . 54 fC: Carrier frequency of the radio. FreqBand: Frequency band. 0: 315MHz, 1: 433MHz and 2: 900MHz. In equation (5), it is evident that the VCO gain is dependent of carrier frequency. MOD_I is probably the best parameter to alter if counteracting this effect if necessary. Combining equations (3), (4), and (5) gives us an expression for the frequency deviation: () () FreqBand FreqBand f Const Const I MOD f f C A MOD XTAL DEV − − ⋅ ⋅ + ⋅ ⋅ = 3 3 2 _ FSKClk_K 2 1 _ (6) Observe that equation (6) gives single-sided- deviation. Peak-to-peak deviation is twice this value. Shaping The modulation waveform will be shaped due to the charging and discharging of a capacitor. The waveform looks like a Gaussian filtered signal with a Bandwidth ⋅Period-product, BT, given by: FSKn BT 2 = (7) where: BT: Shaping factor. It is evident from this that a low FSKn gives a low shaping factor, and is thus preferred if it is possible to choose FSKn freely. In addition to this, it is possible to smooth the modulator output in a programmable low-pass filter. This filter is controlled by the parameter MOD_F. The parameter should be set according to equation (8). BR F MOD 3 10 150 _ × ≤ (8) Modulator Saturation The modulator output voltage is generated by a capacitor that is being charged. This means that there is a risk of saturating the modulator if the charge received by the capacitor is too large. Use equation (9) to determine the maximum value of MOD_I that can be used. 1 10 28 _ 6 + ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ × ⋅ ≤ − FSKClk_K f I MOD XTAL (9) If it turns out that the MOD_I-range is too small for your requirements, try increasing FSKn and decreasing FSKClk_K accordingly. |
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