SSI2144 FATKEYS FOUR-POLE VOLTAGE CONTROLLED FILTER

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SSI FATKEYS FOUR-POLE VOLTAGE CONTROLLED FILTER The SSI reprises the SSM0 of legacy chipmaker Solid State Micro Technology, which many believe to be the best-sounding analog synthesis filter IC ever produced. Based on Dave Rossum s patented classic improved ladder topology, the SSI allows rich tonal characteristics that showcase the very best attributes of subtractive synthesis. The SSI uses the same internal circuit as the SSM0 but incorporates improvements by the original designer and takes advantage of modern process technology. Features include a minimum,000 to sweep range, on-chip control of resonance, differential inputs, high control rejection, and minimized external components. The SSI will operate on supplies as low as ±V, and improvements include lower noise, significantly better control feedthrough, and more consistent unit-to-unit performance of the resonance control. Pin connections were revised for PCB layout ease. Most importantly, the SSI preserves the coveted sonic character of the SSM0. FEATURES Classic Analog Synthesis Timbre On-Chip Resonance Circuit Improved for More Consistent Control and Performance ±V to ±V Operation Pin Connections Optimized for PCB Layout Differential Inputs Large Sweep Range - Typical 0,000 to Low Feedthrough on Both Control Ports -Pin SSOP Package with Minimal External Components CB CA CB V+ CA CB CA CB CA V+ g ms g ms SIG IN FREQ CTRL CA CB CA SSI TOP VIEW Q CTRL CA CB CA SIG IN- SIG IN+ C C C C g ms g mq A o CB CB GND FREQ CTRL e-v fc I fc 00Ω I Q g ms PIN CONNECTIONS -LEAD SSOP (JEDEC MO--AB) Q CTRL FUNCTIONAL BLOCK DIAGRAM The SSI is distributed exclusively by CruzTOOLS, Inc. and it s authorized resellers PO Box 0, Standard, CA USA Phone 0--0, www.soundsemiconductor.com Sound Semiconductor and Fatkeys are trademarks of Sound Semiconductor Rev..0. January 0 0 Sound Semiconductor M 0 Sound Semiconductor

SPECIFICATIONS (VS = ±V, T A = C; using Figure circuit unless otherwise noted) FATKEYS FOUR-POLE VOLTAGE CONTROLLED FILTER Page Parameter Symbol Conditions Min Typ Max Units POWER SUPPLY Supply Voltage Range Supply Current - Positive Supply Current - Negative FILTER SECTION Frequency Sweep Range Frequency Control Sensitivity Frequency Control Input Bias Current Frequency Control Input Range Frequency Control Feedthrough Frequency Control Offset Voltage Maximum Available Control Current RESONANCE (Q) SECTION Q Current Input Range Q Current at Oscillation Q Control Feedthrough SIGNAL INPUTS Input Bias Current Differential Input Signal Range SIGNAL PUT Maximum Output Signal Current Dynamic Range Output Offset V S I CC I EE V FC I Q V FC and Q CNTRL at ground V FC and Q CNTRL at ground ±V IN =GND; -0mV V FC +0mV Untrimmed V FC = -0mV -0mV V FC +0mV 0 < I Q < 00 I B V IN Either Input, V FC = 0, Iq = 0 Clipping I OMAX DR I OS Noise floor to % THD, A Wtd V IN+ = V IN- = V FC = 0, I Q = 0 ±.0. :000: -0-0 - - 00.0. 0:000: - -0 0 0 0 0 00-0 0 ±0 ±00 ±00 ±.. - +0 + 00 00 0-0 V ma ma mv/oct mv db mv db 0 na mv ±0 db ABSOLUTE MAXIMUM RATINGS Supply Voltage ±V Storage Temperature Range - C to +0 C Operating Temperature Range -0 C to + C Lead Temperature Range (Soldering, sec) 0 C ORDERING INFORMATION Part Number Package Type Container SSISS-TU -Lead SSOP*, Tube Packing 0 SSISS-RT -Lead SSOP*, Tape and Reel 000 *Compliant to JEDEC MO--AB. Please order in full container multiples. USING THE SSI Signal Inputs Figure shows typical connection of the SSI as a four-pole lowpass filter in electronic music systems. Differential inputs allow the convenience of directly connecting two oscillators. To prevent cancellation of in-phase signals, a db attenuation of the SIG IN- input is accomplished using the resistor values shown. If only one input is needed, the unused input pin should be connected to ground via a resistor. The SSI differential input signal level is nominally ±0mV and clips at ±0mV. The resistor values in Figure result in ±V being the nominal input signal level. Frequency Control The Control Summer adds voltages from various sources such as the panel frequency control, ADSR, LFO, etc. Any number of signals can be mixed through resistors to the summing node of the op amp. For best control rejection, the Control Summer and input attenuator should be designed such that maximum swing to the Frequency Control (pin ) matches extremes of the intended sweep range when the Control Summer is driven to the op amp s full output voltage swing. With values shown in Figure, ±0mV at the Frequency Control pin corresponds to a 00: sweep range using ±V supplies. A frequency offset adjustment is necessary in polyphonic systems for consistent cutoff fequency across voices, or programmable systems where repeatable performance from a given control voltage is desired. Resonance (Q) Control The Q Control (pin ) is a current input summing node at ground. Minimum resonance occurs at zero current. Oscillation will occur when current into the Q Control reaches approximately 00, equating to.v using the resistor value of.kω in Figure. Figures shows typical squarewave response at various Q current intervals.

Page.kΩ V+ NOTES: All resistors are % and capacitors % NPO *Optional temperature-compensating resistor - see text Optional - improves Q stability and amplitude over frequency sweep SIG IN- 0kΩ.kΩ 0pF / TL0.nF SSI Q CONTROL.kΩ Ω nf kω* kω Fc Fc Fcx FREQ CONTROL 0kΩ kω 0kΩ 0kΩ / TL0 V/OCT 0kΩ CONTROL SUMMER +V 0kΩ -V FREQ OFFSET ADJUST Figure : Typical Application Circuit Q = 0 Q = Q = Q = 00 Figure : Square Wave Response vs. Q Current +V Q CTRL Ω.kΩ kω REVERSE AUDIO nf Figure : Recommended Q Control Potentiometer Circuit

Page Due to response of the Q circuit (see SSI Filter Characteristics below), ideal potentiometer feel is achieved with a reverse audio taper (0% at 0%; i.e. Bourns PDB series) configuration as shown in Figure. If accurate musical intervals during oscillation are desired, the V/OCT trim and a temperature compensating resistor (such as the Panasonic ERA-VJV) are necessary. If such intervals aren t important, substitute % kω in the Control Summer feedback network and % kω in place of the temperature compensating resistor. The temperature compensating resistor should be physically as close to the SSI as possible to maintain good thermal coupling. Signal Output Figure shows direct connection to a current input SSI VCA from the SSI s output (pin ). In this case, no intervening op amp is required. A µf cap blocks any DC offset present at Pin, so no further offset adjustment is neccesary to maintain the SSI s specified control feedthrough. The input to the SSI should also be AC coupled when this circuit is used. VCA CV IN 0pF SSI µf kω / SSI 0.kΩ.kΩ Ω / TL0 VCA Figure : Direct Connection of SSI to a SSI VCA SSI FILTER CHARACTERISTICS Figures and show behavior of the SSI filter and Q circuits. In Figure, the solid line shows response of the filter with the Q control at ground. In this case, the filter comprises four real poles, each producing db of attenuation at the cutoff frequency. As voltage is applied to the Fc input, cutoff frequency will vary exponentially in response to the control voltage. The Q circuit provides negative feedback around the filter. As Q control current is increased, gain at DC and frequencies below cutoff are proportionately decreased, and gain at the cutoff frequency is increased as shown in the dotted line of Figure. At higher frequencies, an approximate db/octave rolloff will be maintained. When feedback exceeds db, loop gain at cutoff exceeds unity and the filter oscillates with a pure sinewave at the cutoff frequency. This waveform can therefore become a very useful tone source in electronic music systems. The SSI s Q control circuit has been improved over the SSM0. It accurately applies the current supplied to the Q input summing node (which is maintained at a ground potential) to the feedback amplifier, eliminating process dependent variations in the gain of the Q control circuit. Figure shows resonance, measured as the height of the resonant peak above the low frequency gain, as a function of Q Control current. Note that the slope is more flat at lower current, then increases rapidly as oscillation is approached. To compensate for this variation in slope, the reverse audio taper potentiometer circuit in Figure above is recommended. Figure shows the corrected response; the rightmost portion of the rotation represents the region of oscillation.

Page 0 0 Amplitude SSI Filter Response Resonance (db) 0 0 0 Increasing Q Control 0 Frequency Figure : Filter and Q Response 0 00 00 00 Q Control Current () Figure : Resonance Peak Height vs. Q Current 0 Resonance (db) 0 0 0 0 0 Q Pot Rotation (%) Figure : Q Response Using Reverse Audio Pot APPLICATION INFORMATION SUB-AUDIO FREQUENCY CUTOFF CONSIDERATIONS In most fixed signal-path synthesizers, cutoff frequency is limited to the audio range. Modular systems, however, may allow sub-audio cutoffs. The SSI and its predecessor SSM0 can exhibit undesirable behavior when voltage at the Frequency Control (Pin ) exceeds approximately mv. Current in the ladder becomes smaller than the output amplifier s bias current, causing the common-mode voltage of the output stage to suddenly drop. Under these conditions, the filter no longer passes any signal and the output transitions to an unrelated fixed voltage. Normal operation resumes once the control voltage is reduced to approximately mv, and may be accompanied by an audible thump. Note that actual control voltage levels at which these transitions occur may vary slightly from part-to-part or batch-to-batch. A network attached to both C pins provides a simple solution. Place a pair of matched low leakage diodes (or diode-connected transistors, as shown) with cathodes connected to CA and CB (Pins and ). Tie the anodes together and to a diode connected to ground, and bias this point with a resistor to the negative supply. The bias current magnitude is relatively unimportant. This circuit will prevent the output stage common-mode voltage from dropping, allowing the filter to gracefully degrade in performance at extremely low cutoff frequencies. See Figure.

Page IN BCM CA CB MΩ Figure : Sub-Audio Filter Cutoff Application Circuit CIRCUMVENTING Q CONTROL PASSBAND ATTENUATION As described in the preceeding Filter Characteristics section, both the SSM0 and the SSI demonstrate increasing attenuation of the passband as Q is increased. Many synthesizer enthusiasts consider this to be part of its signature sound, but in some applications the designer may wish to mitigate the characteristic. Figures and show alternate solutions. Both schemes route input and output signals to the input of an external Q VCA that uses one-half of an LM00 Transconductance Amplifier, with its I C (bias) pin becoming the Q control, replacing the internal Q VCA of the SSI. As Q is increased, the filter input signal is proportionately increased to offset DC gain reduction from negative feedback. As a result, DC gain is held constant. In essence the negative feedback at DC will be zero regardless of Q VCA gain, preventing any DC gain change. The TL0 s inverting output is summed with the non-inverted signal input and applied to the Q VCA input yielding zero negative feedback signal at DC. Figure uses one-half of a non-linearized LM00 as the Q VCA. The values of R, R, R, and R are chosen to accurately mimic the SSI s internal Q amplifier. Consequently, a control current of approximately to the I C input of the LM00 results in oscillation. With the values shown, the DC gain of the filter remains contant at approximately unity over the Q control range. Increasing R s value will proportionally reduce DC gain at high Q currents; omitting it will cause the circuit behave virtually identical to the SSI. This circuit is recommended if the vintage SSM0 sound is desired. I C LM00 V D NC Ω R.kΩ R V+ Q CONTROL kω REVERSE AUDIO D N D AUDIO.kΩ R.kΩ pf / TL0.kΩ R.kΩ Ω R SSI kω.kω FREQ CONTROL To Control Summer and Offset Trim as Needed kω Figure : Non-Linearized Q VCA

Page Figure takes advantage of the LM00 s linearizing diodes which allows R to be set to zero. Other values are chosen such that a ma control current to the Ic input of the LM00 gives oscillation and maintains constant DC gain over the Q range. As with Figure, increasing R will proportionately reduce DC gain at high Q currents. Use this circuit to minimize distortion in the Q VCA. In both cases, the designer must supply the Q control as a current to the LM00 s I C input pin. The circuits shown use the same Reverse Audio taper pot previously recommended, and assume ±V supplies. Diodes D and D (any general purpose signal diode will do) provide thermal compensation for the variation in input voltage at the I C pin, and therfore should be physically close to the LM00. Designers familiar with the LM00 may choose to use other schemes to supply I C. I C LM00 V D.kΩ R.kΩ R V+ Q CONTROL kω REVERSE AUDIO D N D AUDIO.kΩ R.kΩ pf / TL0.kΩ R.kΩ.kΩ R SSI kω.kω FREQ CONTROL To Control Summer and Offset Trim as Needed kω Figure : Linearized Q VCA TYPICAL PERFORMANCE GRAPHS Figure Application Circuit at V S = ±V, f = khz unless otherwise noted THD+N vs. Frequency V IN = +dbu, Hz - 0kHz Filter THD+N vs. Amplitude f = khz, <Hz - khz Filter FATKEYS Trademark Usage Sound Semiconductor customers are encouraged, but not required, to use the Fatkeys trademark in their product and promotional literature. A royalty-free license is provided for use of the mark to those who purchase the SSI from Sound Semiconductor and it s authorized distributors. Proper attribution of the mark includes Fatkeys from Sound Semiconductor or if Fatkeys is used separately, a trademark symbol ( ) must accompany it and the text Fatkeys is a trademark of Sound Semiconductor provided at a reasonable location on the same page as first use of the mark.