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TS615IPWT 数据表(PDF) 25 Page - STMicroelectronics

部件名 TS615IPWT
功能描述  DUAL WIDE BAND OPERATIONAL AMPLIFIER WITH HIGH OUTPUT CURRENT
PDF  27 Pages
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制造商  STMICROELECTRONICS [STMicroelectronics]
网页  http://www.st.com
标志 STMICROELECTRONICS - STMicroelectronics

TS615IPWT 数据表(HTML) 25 Page - STMicroelectronics

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TS615
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INCREASING THE LINE LEVEL BY USING AN
ACTIVE IMPEDANCE MATCHING
With a passive matching, the output signal ampli-
tude of the driver must be twice the amplitude on
the load. To go beyond this limitation an active
matching impedance can be used. With this tech-
nique, it is possible to keep a good impedance
matching with an amplitude on the load higher
than the half of the output driver amplitude. This
concept is shown in figure 74 for a differential line.
Figure 74 : TS615 as a differential line driver with
an active impedance matching
Component Calculation
Let us consider the equivalent circuit for a single
ended configuration, Figure75.
Figure 75 : Single ended equivalent circuit
Let us consider the unloaded system. Assuming
the currents through R1, R2 and R3
as respectively:
As Vo° equals Vo without load, the gain in this
case becomes :
The gain, for the loaded system will be (eq1):
As shown in figure76, this system is an ideal gen-
erator with a synthesized impedance as the inter-
nal impedance of the system. From this, the out-
put voltage becomes:
with Ro the synthesized impedance and Iout the
output current. On the other hand Vo can be ex-
pressed as:
By identification of both equations (eq2) and
(eq3),
the
synthesized
impedance
is,
with
Rs1=Rs2=Rs:
Figure 76 : Equivalent schematic. Ro is the
synthesized impedance
R4
R2
Vi
Vi
Vo
Vo
RL
100
1:n
Hybrid
&
Transformer
GND
Vcc+
10
µ
100n
100n
100n
1k
1k
Rs1
Rs2
10n
1
µ
R3
R5
Vo°
Vo°
GND
Vcc+
Vcc+
+
_
+
_
GND
1/2
R1
1/2
R1
Vcc/2
1/2RL
1/2R1
R2
R3
+
_
Vi
Vo
Rs1
-1
Vo°
1/2RL
1/2R1
R2
R3
+
_
Vi
Vo
Rs1
-1
Vo°
2Vi
R1
---------
Vi
Vo
°
()
R2
--------------------------- and
Vi
Vo
+
()
R3
------------------------
,
G
Vo noload
()
Vi
---------------------------------
1
2R2
R1
-----------
R2
R3
--------
++
1
R2
R3
--------
------------------------------------
==
GL
Vo with load
()
Vi
--------------------------------------
1
2
---
1
2R2
R1
-----------
R2
R3
--------
++
1
R2
R3
--------
------------------------------------ eq1
()
,
==
Vo
ViG
()
RoIout
()
=
eq2
()
,
Vo
Vi 1
2R2
R1
-----------
R2
R3
--------
++


1
R2
R3
--------
------------------------------------------------
Rs1Iout
1
R2
R3
--------
----------------------- eq3
()
,
=
Ro
Rs
1
R2
R3
--------
----------------- eq4
()
,
=
Ro
Vi.Gi
Iout
1/2
RL



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