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EL4451C 参数 Datasheet PDF下载

EL4451C图片预览
型号: EL4451C
PDF下载: 下载PDF文件 查看货源
内容描述: 宽带可变增益放大器的增益2 [Wideband Variable-Gain Amplifier, Gain of 2]
分类和应用: 放大器
文件页数/大小: 12 页 / 303 K
品牌: ELANTEC [ ELANTEC SEMICONDUCTOR ]
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EL4451C  
Wideband Variable-Gain Amplifier, Gain of 2  
360X or less. Alternatively, a small capacitor  
across R can be used to create more of a fre-  
Applications Information  
F
The EL4451 is a complete two-quadrant multipli-  
er/gain control with 70 MHz bandwidth. It has  
three sets of inputs; a differential signal input  
quency-compensated divider. The value of the ca-  
pacitor should scale with the parasitic capaci-  
tance at the FB input. It is also practical to place  
small capacitors across both the feedback and the  
gain resistors (whose values maintain the desired  
gain) to swamp out parasitics. For instance, two  
10pF capacitors across equal divider resistors for  
a maximum gain of 4 will dominate parasitic ef-  
fects and allow a higher divider resistance.  
V
IN  
, a differential gain-controlling input V  
,
GAIN  
and another differential input which is used to  
complete a feedback loop with the output. Here is  
a typical connection:  
The REF pin can be used as the output’s ground  
reference, for DC offsetting of the output, or it  
can be used to sum in another signal.  
Gain-Control Characteristics  
The quantity V  
in the above equations is  
2, even though the exter-  
GAIN  
s
s
bounded as 0  
V
GAIN  
4451-2  
nally applied voltages exceed this range. Actual-  
ly, the gain transfer function around 0 and 2V is  
‘‘soft’’; that is, the gain does not clip abruptly  
The gain of the feedback divider is  
R
G
e
H
.
below the 0%-V voltage nor above the  
GAIN  
a
R
G
R
F
100%-V  
applied to V  
level. An overdrive of 0.3V must be  
GAIN  
The transfer function of the part is  
a
to obtain truly 0% or 100%.  
GAIN  
e
c
a
b
b
c
b
b
(V  
GAIN  
a
))  
V
A
O
(((V  
IN  
)
(V  
)) ((V  
GAIN  
)
OUT  
IN  
Because the 0%- or 100%- V levels cannot  
GAIN  
b
(V  
REF  
V
)).  
FB  
be precisely determined, they are extrapolated  
from two points measured inside the slope of the  
gain transfer curve. Generally, an applied V  
V
is connected to V  
OUT  
c
V
through a feedback  
. A is the open-  
OUT O  
FB  
network, so V  
e
H
FB  
GAIN  
loop gain of the amplifier, and is approximately  
600. The large value of A drives  
b
range of 0.5V to 2.5V will assure the full nu-  
merical span of 0  
a
O
s
s
V
GAIN  
2.  
a
b
b
c
a
b
b
a
b
((V  
IN  
)
(V  
IN  
)) ((V  
GAIN  
)
(V  
GAIN  
))  
(V  
V
FB  
)
REF  
x
0.  
The gain control has a small-signal bandwidth  
equal to the V channel bandwidth, and over-  
load recovery resolves in about 20 nsec.  
Rearranging and substituting for V  
a
IN  
FB  
e
a
b
b
c
b
a
V
(((V  
IN  
)
(V  
)) ((V  
GAIN  
)
(V  
))  
V
)/H,  
REF  
OUT  
IN  
GAIN  
or  
V
Input Connections  
e
c
a
(V  
IN  
V
V
)/H  
REF  
OUT  
GAIN  
The input transistors can be driven from resistive  
and capacitive sources, but are capable of oscilla-  
tion when presented with an inductive input. It  
takes about 80nH of series inductance to make  
the inputs actually oscillate, equivalent to four  
Thus the output is equal to the difference of the  
’s times the difference of V and offset  
V
IN  
by V  
GAIN’S  
, all gained up by the feedback divider  
REF  
ratio. The EL4451 is stable for a direct connec-  
tion between V and FB, and the divider may  
OUT  
inches of unshielded wiring or 6 of unterminat-  
×
be used for higher output gain, although with the  
traditional loss of bandwidth.  
ed input transmission line. The oscillation has a  
characteristic frequency of 500 MHz. Often plac-  
ing one’s finger (via a metal probe) or an oscillo-  
scope probe on the input will kill the oscillation.  
Normal high-frequency construction obviates  
any such problems, where the input source is rea-  
sonably close to the input. If this is not possible,  
one can insert series resistors of around 51X to  
de-Q the inputs.  
It is important to keep the feedback divider’s im-  
pedance at the FB terminal low so that stray ca-  
pacitance does not diminish the loop’s phase  
margin. The pole caused by the parallel imped-  
ance of the feedback resistors and stray capaci-  
tance should be at least 150 MHz; typical strays  
of 3 pF thus require a feedback impedance of  
7