參數(shù)資料
型號: ATF-38143-TR1
元件分類: 小信號晶體管
英文描述: L BAND, GaAs, N-CHANNEL, RF SMALL SIGNAL, HEMFET
封裝: PLASTIC, SC-70, 4 PIN
文件頁數(shù): 12/12頁
文件大?。?/td> 540K
代理商: ATF-38143-TR1
9
PRELIMINARY DATA
This preliminary data is provided to assist you in the evaluation of product(s) currently under development and targeted for market release
shortly. Until Hewlett-Packard releases this product for general sales, HP reserves the right to alter prices, specifications, features,
capabilities, functions, release dates, and remove availability of the product(s) at any time.
Noise Parameter Applications Information
Fmin values at 2GHz and higher are based on measurements while the Fmins below 2 GHz have been extrapolated. The
Fmin values are based on a set of 16 noise figure measurements made at 16 different impedance using an ATN NP5 test
system. From these measurements, a true Fmin is calculated. Fmin represents the true minimum noise figure of the
device when the device is presented with an impedance matching network that transforms the source impedance,
typically 50
, to an impedance represented by the reflection coefficient Γ
o. The designer must design a matching
network that will present
Γ
o to the device with minimal associated circuit losses. The noise figure of the completed
amplifier is equal to the noise figure of the device plus the losses of the matching network preceding the device. The
noise figure of the device is equal to Fmin only when the device is presented with
Γ
o. If the reflection coefficient of the
matching network is other than
Γ
o , then the noise figure of the device will be greater than Fmin based on the following
equation.
NF = Fmin + 4 Rn
|
Γs - Γo |2
Zo
(|1 +
Γo|2) (1 - |Γs|2)
Where Rn/Zo is the normalized noise resistance,
Γ
o is the optimum reflection coefficient required to produce Fmin and Γ
s is the reflection coefficient of the source impedance actually presented to the device.
The losses of the matching networks are non-zero and they will also add to the noise figure of the device creating a
higher amplifier noise figure. The losses of the matching networks are related to the Q of the components and associated
printed circuit board loss.
Γo is typically fairly low at higher frequencies and increases as frequency is lowered. Larger
gate width devices will typically have a lower
Γ
o as compared to narrower gate width devices. Typically for FETs , the
higher
Γ
o usually infers that an impedance much higher than 50 is required for the device to produce Fmin. At VHF
frequencies and even lower L Band frequencies, the required impedance can be in the vicinity of several thousand ohms.
Matching to such a high impedance requires very hi-Q components in order to minimize circuit losses. As an example at
900 MHz, when air-wound coils (Q>100)are used for matching networks, the loss can still be up to 0.25 dB which will
add directly to the noise figure of the device. Using multi-layer molded inductors with Qs in the 30 to 50 range results in
additional loss over the air-wound coil. Losses as high as 0.5 dB or greater add to the typical 0.15 dB Fmin of the device
creating an amplifier noise figure of nearly 0.65 dB. A discussion concerning calculated and measured circuit losses and
their effect on amplifier noise figure is covered in Hewlett Packard Application 1085.
相關(guān)PDF資料
PDF描述
ATF-38143-TR2 L BAND, GaAs, N-CHANNEL, RF SMALL SIGNAL, HEMFET
ATF-38143-BLK L BAND, GaAs, N-CHANNEL, RF SMALL SIGNAL, HEMFET
ATF-38143-TR2G X BAND, GaAs, N-CHANNEL, RF SMALL SIGNAL, HEMFET
ATF-38143-BLKG X BAND, GaAs, N-CHANNEL, RF SMALL SIGNAL, HEMFET
ATF-38143-TR1G X BAND, GaAs, N-CHANNEL, RF SMALL SIGNAL, HEMFET
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