熱門工具
- 1環(huán)型天線計算器
- 2運算放大器低通濾波器計算器
- 3飛行器機翼弦長估算工具
- 4Trap 天線設(shè)計方法及計算工具
- 5微帶線計算工具 | Microstrip Line Calculator
- 6RF Trap衰減器計算 | RF Trap With Attenuators Calculator
- 7同軸線計算工具 | Coaxial Line Calculator
- 85級微帶低通濾波器設(shè)計 | 5-section Distributed LPF Calculator
- 9PI衰減器計算器 (回波) | PI Attenuator Calculator
- 10J型發(fā)射天線尺寸在線計算器
有源工具
完整的RF放大器設(shè)計與分析計算器
To use the calculator, enter in the amp’s S-parameters. The characteristic impedance used in the S-parameter measurements. The frequency at which you will use the amplifier, the source’s and load’s impedance, and whether you want high pass or low pas networks on the L-Matching networks.
Remember that the S-parameters are a function of how the amplifier is biased. Some times you can read or extrapolate the parameter’s off transistor datasheets for a given bias point. However, if these are not available then you must measure the S-parameters using a vector network analyzer (VNA).
The calculator will return the Rollet Stability Factor (K). If K is greater than one, then amplifier is stable for any combination of load and source impedance. However, it it is less than one then there may exist certain combinations for load and source impedance which are less than one, which could cause the amplifier to be unstable, e.g. oscillate.
The returned maximum allowable gain (MAG) for the RF amplifier. The MAG is the highest gain you could expect to achieve from a conjugately matched amplifier.
The purpose of the matching networks is transform the desired load and source impedances such they generate the calculated load and source impedances (GammaL/S).
The calculated load and source impedances, are the impedances that would be see looking into the input of the conjugately-matched amplifier. For example on the input side, it is the impedance seen looking into the input of an amplifier, which has it’s output perfectly matched, or the observed output impedance of the amplifier, when the input is perfectly matched.
The suggested L-networks will transform the input and output impedances so that they perfectly match the given source and load impedances. Please note that the L-Networks are just suggestions, there are many other ways to match two impedances, such as three element PI and T networks, and broadband transformers. The disadvantage with L-networks is that they have a fixed Q, which is a function of the ratio of the resistive parts of the two impedances which are being matched. Three element matches give more flexibility in the choice of Q. Networks with many elements can be designed which give any desired Q. The Q is important because it determines the bandwidth of the network. For a broad band amplifier, you want the smallest possible Q. These are typically done with the use of a Smith chart. There are also cases when you don’t want a perfect match, for example you want an amplifier that has lower gain.
CALCULATOR INPUTS | |
Zo= (ohms) | F= MHz |
Source and Load Impedances | |
ZS= j | ZL= j |
Source and Load L-Matching Networks | |
Source: Low Pass High Pass | Load: Low Pass High Pass |
S-Parameters (Rectangular Or Polar(Degrees)) | |
S11= | |
S12= | |
S21= | |
S22= | |
|
|
CALCULATOR RESULTS |
|
Rollet Stability Factor (K) | |
K= | |
Maximum Allowable Gain | |
MAG= (Gain) (Db) | |
Conjugate Input and Output Reflection Coefficients | |
GAMAL (Polar) | |
GAMAS (Polar) | |
Input and Output Impedances Looking into Amp | |
ZSM j | |
ZLM j | |
L-Network Matching Components | |
Source | Load |
C=pf, L=nH | C=pf, L=nH |
Qs= | QL= |
Parallel leg of L-network near amp | Parallel leg of L-network near amp |
Equations:
Ds=S11S22 - S12S21
K=(1+|Ds|^2-|S11|^2-|S22|^2)/(2|S21||S12|)
B1=1+|S11|^2 - |S22|^2 - |Ds|^2
MAG= |S21|/|S21|(Kqrt(K^2-1) -> if B is negative use +, otherwise -.
Load Reflection Coefficient:
GAMAL