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NE5517 Datasheet(PDF) 10 Page - NXP Semiconductors

Part # NE5517
Description  Dual operational transconductance amplifier
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Manufacturer  PHILIPS [NXP Semiconductors]
Direct Link  http://www.nxp.com
Logo PHILIPS - NXP Semiconductors

NE5517 Datasheet(HTML) 10 Page - NXP Semiconductors

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Philips Semiconductor
Product data
NE5517/NE5517A/
AU5517
Dual operational transconductance amplifier
2002 Dec 06
10
V+
11
D4
Q6
Q7
2,15
D2
Q4
Q5
D3
–INPUT
4,13
+INPUT
3,14
AMP BIAS
INPUT
1,16
Q2
Q1
D1
V–
6
Q10
D6
Q11
VOUTPUT
5,12
Q9
Q8
D5
Q14
Q15
Q16
R1
D7
D8
Q3
7,10
Q12
Q13
8,9
SL00313
Figure 8. Circuit Diagram of NE5517
+VS
ID
IB
I5
Q4
1/2ID
IS
IS
1/2ID
–VS
I4
I5
D3
D2
I
D
2
* I
S
I
D
2
) I
S
I
0 +
I
5 *
I
4
I
0 +
2I
S
I
B
I
D
SL00314
Figure 9. Linearizing Diode
Stereo Amplifier With Gain Control
Figure 11 shows a stereo amplifier with variable gain via a control
input. Excellent tracking of typical 0.3 dB is easy to achieve. With
the potentiometer, RP, the offset can be adjusted. For AC-coupled
amplifiers, the potentiometer may be replaced with two 510
resistors.
Modulators
Because the transconductance of an OTA (Operational
Transconductance Amplifier) is directly proportional to IABC, the
amplification of a signal can be controlled easily. The output current
is the product from transconductance
×input voltage. The circuit is
effective up to approximately 200 kHz. Modulation of 99% is easy to
achieve.
Voltage-Controlled Resistor (VCR)
Because an OTA is capable of producing an output current
proportional to the input voltage, a voltage variable resistor can be
made. Figure 13 shows how this is done. A voltage presented at the
RX terminals forces a voltage at the input. This voltage is multiplied
by gM and thereby forces a current through the RX terminals:
RX=
R
) R
A
gM
) R
A
where gM is approximately 19.21 µMHOs at room temperature.
Figure 14 shows a Voltage Controlled Resistor using linearizing
diodes. This improves the noise performance of the resistor.
Voltage-Controlled Filters
Figure 15 shows a Voltage Controlled Low-Pass Filter. The circuit is
a unity gain buffer until XC/gM is equal to R/RA. Then, the frequency
response rolls off at a 6dB per octave with the –3 dB point being
defined by the given equations. Operating in the same manner, a
Voltage Controlled High-Pass Filter is shown in Figure 16. Higher
order filters can be made using additional amplifiers as shown in
Figures 17 and 18.
Voltage-Controlled Oscillators
Figure 19 shows a voltage-controlled triangle-square wave
generator. With the indicated values a range from 2 Hz to 200 kHz is
possible by varying IABC from 1 mA to 10 µA.
The output amplitude is determined by IOUT × ROUT.
Please notice the differential input voltage is not allowed to be above
5 V.
With a slight modification of this circuit you can get the sawtooth
pulse generator, as shown in Figure 20.


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