欢迎访问ic37.com |
会员登录 免费注册
发布采购

AD8362-EVAL 参数 Datasheet PDF下载

AD8362-EVAL图片预览
型号: AD8362-EVAL
PDF下载: 下载PDF文件 查看货源
内容描述: 50 Hz至2.7 GHz的60分贝TruPwr⑩探测器 [50 Hz to 2.7 GHz 60 dB TruPwr⑩ Detector]
分类和应用:
文件页数/大小: 36 页 / 699 K
品牌: ADI [ ADI ]
 浏览型号AD8362-EVAL的Datasheet PDF文件第12页浏览型号AD8362-EVAL的Datasheet PDF文件第13页浏览型号AD8362-EVAL的Datasheet PDF文件第14页浏览型号AD8362-EVAL的Datasheet PDF文件第15页浏览型号AD8362-EVAL的Datasheet PDF文件第17页浏览型号AD8362-EVAL的Datasheet PDF文件第18页浏览型号AD8362-EVAL的Datasheet PDF文件第19页浏览型号AD8362-EVAL的Datasheet PDF文件第20页  
AD8362  
4.0  
3.5  
3.0  
2.5  
2.0  
1.5  
1.0  
0.5  
Accordingly, VTGT (and its fractional part VATG) determines the  
output that must be provided by the VGA for the AGC loop to  
settle. Since the scaling parameters of the two squarers are  
accurately matched, it follows that Equation 3 is satisfied only  
when  
2
2
MEAN  
(
VSIG  
)
= VATG  
(4)  
In a formal solution, one would then extract the square root of  
both sides to provide an explicit value for the root-mean-square  
(rms) value. However, it is apparent that by forcing this identity,  
through varying the VGA gain and extracting the mean value  
by the filter provided by the capacitor(s), the system inherently  
establishes the relationship  
0
100µV  
1mV  
10mV  
100mV  
1V  
10V  
RMS INPUT VOLTAGE (100µV TO 3.2V)  
Figure 43. Ideal Response of the AD8362  
rms  
(
VSIG  
)
=VATG  
(5)  
EFFECT OF INPUT COUPLING ON THE INTERCEPT  
VALUE  
Substituting the value of VSIG from Equation 2, we have  
Reductions of VIN due to coupling losses directly affect VZ. In  
high frequency applications, several factors contribute to the  
coupling of the source into the IC, including the board and  
package resonances and attenuation. Any uncertainties in the  
input impedance result in the intercept expressed in power  
terms, which is nominally −57 dBm for a 50 Ω system, being  
less accurately determined than when stated in dBV (that is, in  
pure voltage) terms. On the other hand, the slope VSLP is  
unaffected by all such impedance or coupling uncertainties.  
rms  
[
GOVIN exp  
(
VSET VGNS  
)
]
=VATG  
(6)  
As a measurement device, VIN is the unknown quantity and all  
other parameters can be fixed by design. Solving Equation 6:  
rms  
[
GOVIN VATG  
]
= exp  
(
VSET VGNS  
)
(7)  
so  
VSET =VGNS log  
[
rms  
(VIN  
)
VZ  
]
(8)  
OFFSET ELIMINATION  
The quantity VZ = VATG/GO is defined as the intercept voltage  
because VSET must be 0 when rms (VIN) = VZ.  
To address the small dc offsets that arise in the variable gain  
amplifier, an offset-nulling loop is used. The high-pass corner  
frequency of this loop is internally preset to 1 MHz, sufficiently  
low for most HF applications. When using the AD8362 in LF  
applications, the corner frequency can be reduced as needed by  
the addition of a capacitor from the CHPF pin to ground having  
a nominal value of 200 µF/Hz. For example, to lower the high-  
pass corner frequency to 150 Hz, a capacitance of 1.33 µF is  
required. The offset voltage varies depending on the actual gain  
at which the VGA is operating, and thus, on the input signal  
amplitude.  
When connected as a measurement device, the output of the  
buffer is tied directly to VSET, which closes the AGC loop.  
Making the substitution VOUT = VSET and changing the log  
base to 10, as needed in a decibel conversion, we have  
VOUT =VSLP log10  
[
rms  
(VIN  
)
VZ  
]
(9)  
where VSLP is the slope voltage, that is, the change in output  
voltage for each decade of change in the input amplitude.  
(Note that VSLP = VGNS log (10) = 2.303 VGNS). In the AD8362,  
V
SLP is laser trimmed to 1 V using a 100 MHz test signal.  
Baseline variations of this sort are a common aspect of all  
VGAs, although more evident in the AD8362 because of the  
method of its implementation, which causes the offsets to  
ripple along the gain axis with a period of 6.33 dB. When an  
excessively large value of CHPF is used, the offset correction  
process may lag the more rapid changes in the VGA’s gain,  
which may increase the time required for the loop to fully settle  
for a given steady input amplitude.  
Because a decade corresponds to 20 dB, this slope may also be  
stated as 50 mV/dB. It is later shown how the effective value of  
VSLP may be altered by the user.  
Likewise, the intercept VZ is also laser trimmed to 316 µV  
(−70 dBV). In an ideal system, VOUT would cross zero for an  
rms input of that value. In a single-supply realization of the  
function, VOUT cannot run fully down to ground; here, VZ is  
the extrapolated value. In measurement modes, the output  
ranges from 0.5 V for VIN = 1 mV (input values are stated as  
rms, outputs values as dc), up to a voltage 60 dB × 50 mV/dB =  
3 V above this for VIN = 1 V, that is, to 3.5 V. Figure 43 shows the  
ideal form of Equation 9 scaled as in the AD8362.  
Rev. B | Page 16 of 36  
 
 复制成功!