link to page 10 link to page 10 link to page 10 link to page 10 link to page 10 AD633Data Sheet Likewise, Figure 16 shows how to implement a divider using a This arrangement forms the basis of voltage-controlled integrators multiplier in a feedback loop. The transfer function for the and oscillators as is shown later in this section. The transfer divider is function of this circuit has the form 1 X1 X2Y1Y2 10 E W V (6) I (7) E O R 10 V X R10kΩLINEAR AMPLITUDE MODULATOR+15V+15V The AD633 can be used as a linear amplitude modulator with no 0.1µF0.1µF external components. Figure 19 shows the circuit. The carrier E1X1+VXS8R and modulation inputs to the AD633 are multiplied to produce 10kΩ72X2W 7E a double sideband signal. The carrier signal is fed forward to the 2AD633JN63Y1Z 6AD711 Z input of the AD633 where it is summed with the double 0.1µF3 sideband signal to produce a double sideband with the carrier 44Y2–VS 50.1µF output. +15V–15V–15VE -015 0.1µFW' = –10V 86 EXMODULATION +1 X1+VS 8 007 INPUT Figure 16. Connections for Division ±EEM –2 X2W 7W =M1+EC sin ωtAD633JN10VVARIABLE SCALE FACTORCARRIER3 Y1Z 6INPUT In some instances, it may be desirable to use a scaling voltage EC sin ωt4 Y2–VS 5 other than 10 V. The connections shown in Figure 17 increase 0.1µF 18 0 6- the gain of the system by the ratio (R1 + R2)/R1. This ratio is –15V 78 00 limited to 100 in practical applications. The summing input, S, Figure 19. Linear Amplitude Modulator can be used to add an additional signal to the output, or it can VOLTAGE-CONTROLLED, LOW-PASS AND HIGH- be grounded. PASS FILTERS+15V Figure 20 shows a single multiplier used to build a voltage- 0.1µF+1 X1+V controlled, low-pass filter. The voltage at Output A is a result of S8XINPUT(X1 – X2)(Y1 – Y2) R1 + R2 filtering ES. The break frequency is modulated by EC, the control –2 X2W 7W =+ SAD633JNR110VR1 input. The break frequency, f2, equals +3 Y1Z 61kΩ ≤ R1, R2 ≤ 100kΩYINPUT E –4 Y2–VR2S5 f C (8) 2 0.1µF 10 ( 2 RC ) S 6 -01 and the roll-off is 6 dB per octave. This output, which is at a 786 –15V 00 high impedance point, may need to be buffered. Figure 17. Connections for Variable Scale Factor dBf2 f1CURRENT OUTPUT0f+15V The voltage output of the AD633 can be converted to a current –6dB/OCTAVEOUTPUT B output by the addition of a resistor, R, between the W and Z pins of 0.1µFOUTPUT A1 X1+VS 8 the AD633 as shown in Figure 18. CONTROLINPUT E1 + TC1P2 X2W 7OUTPUT B =+15V1 + TAD633JN2PRSIGNAL13 Y1Z0.1µF6OUTPUT A =INPUT ES0.1µF1 + T2P+1 X1+VS 8CX4 Y2–V1S5RT == RCINPUT1(X1 – X2)(Y1 – Y2)1ω–12 X2W 7IO = 9 AD633JNR10V1 01 10RC–15V 6- T2 ==+3 Y1Z 61kΩ ≤ R ≤ 100kΩω2EC 078 Y 0 INPUT Figure 20. Voltage-Controlled, Low-Pass Filter –4 Y2–VS 50.1µF 7 1 0 The voltage at Output B, the direct output of the AD633, has the 6- –15V 78 same response up to frequency f 00 1, the natural breakpoint of RC Figure 18. Current Output Connections filter, and then levels off to a constant attenuation of f1/f2 = 10/EC 1 f (9) 1 2 RC Rev. K | Page 10 of 20 Document Outline FEATURES APPLICATIONS FUNCTIONAL BLOCK DIAGRAM GENERAL DESCRIPTION PRODUCT HIGHLIGHTS TABLE OF CONTENTS REVISION HISTORY SPECIFICATIONS ABSOLUTE MAXIMUM RATINGS THERMAL RESISTANCE ESD CAUTION PIN CONFIGURATIONS AND FUNCTION DESCRIPTIONS TYPICAL PERFORMANCE CHARACTERISTICS FUNCTIONAL DESCRIPTION ERROR SOURCES APPLICATIONS INFORMATION MULTIPLIER CONNECTIONS SQUARING AND FREQUENCY DOUBLING GENERATING INVERSE FUNCTIONS VARIABLE SCALE FACTOR CURRENT OUTPUT LINEAR AMPLITUDE MODULATOR VOLTAGE-CONTROLLED, LOW-PASS AND HIGH-PASS FILTERS VOLTAGE-CONTROLLED QUADRATURE OSCILLATOR AUTOMATIC GAIN CONTROL (AGC) AMPLIFIERS MODEL RESULTS EXAMPLES OF DC, SIN, AND PULSE SOLUTIONS USING MULTISIM EXAMPLES OF DC, SIN, AND PULSE SOLUTIONS USING PSPICE EXAMPLES OF DC, SIN, AND PULSE SOLUTIONS USING SIMETRIX EVALUATION BOARD OUTLINE DIMENSIONS ORDERING GUIDE