Open access peer-reviewed chapter

# Radio Frequency Background

By Paulo Crepaldi, Tales Pimenta and Luis Ferreira

Submitted: November 9th 2010Reviewed: March 8th 2011Published: July 20th 2011

DOI: 10.5772/20648

## 1. Introduction

Design considerations for the traditional low frequency circuits and the RF circuits are quite different. In low frequency design, the maximum signal transfer occurs when the source presents low impedance while the load presents high impedance. A typical example is a buffer, where the input impedance is high and the output impedance is low. As long as that requirement is fulfilled, the designer is capable of choosing arbitrary levels of impedance that best suits the circuit requirements or applications.

Therefore this chapter aims to provide background on impedance matching between source and load, with or without a transmission line. The analysis can be conducted by using Smith Charts and S-Parameters, which are also presented in this chapter. The analysis in this chapter is oriented to RFID applications whereas other books provide general analysis.

During RF design, the impedances should be matched for maximum signal transfer. Additionally, when the circuits are connected using transmission lines, they should match also the standard values of the transmission lines. At very low frequencies, transmission lines can be thought as just a wire. Nevertheless, at high frequencies, the signal wavelength is comparable to or smaller than the length of the transmissions line and power can be seen as traveling waves. As a matter of fact, even a conductor can be thought as a transmission line in a high frequency circuit.

Most RF equipments and coaxial cables use the standard impedances of 50 or 75 Ω. The value of 75 Ω is used, as an example, in cable TV equipment, since this value provides the minimum losses, as it is desired in transmitting the signal over long distances. In fact, the value of impedance for minimum loss should be 77 Ω, but it was rounded to 75 Ω by convenience.

The value of 50 Ω corresponds to a reasonable compromise, the average, between the minimum loss of a 77 Ω and the maximum power handling capability given of 30 Ω.

## 2. Transmission line

Fig. 1 shows the lumped component model of a real (lossy) transmission line. The segment indicated corresponds to an infinitesimal segment of the transmission line. The characteristic impedance Z0 of this line can be found to be [1]:

Z0=ZY=R+jωLG+jωCE1

As can be observed, the characteristic impedance Z0 is dependent on the frequency. Nevertheless, if the resistive terms R and G are negligible, the expression of the characteristic impedance Z0 can be simplified to:

Z0=LCE2

If the value of RC is equal to GL, expression (1) yields the same value of expression (2). In other words, choosing the L/R time constant of the series impedance equals to the C/G time constant, a lossy line will behave as a lossless line, so that its characteristic impedance will be independent of the frequency[1].

### 2.1. Reflection coefficient

If a transmission line is terminated by an impedance Z0, then a signal traveling down the line with a ratio of voltage to current equal to Z0 will maintain its ratio upon encountering the load and there will be no reflections. On the other hand, when the load is different of Z0, then it imposes its own particular ratio of voltage to current, and the only way to reconcile the conflict is by having some of the signal reflected back towards the source. In order to distinguish the incident and the reflected signals, the subscripts i and r, respectively, will be used.

The incident signal is given by:

Z0=EiIiE3

At the load end, the mismatch in impedances gives rise to a reflected signal. Since the system is still linear, the total voltage at any point in the system is the sum of incident and reflected voltages. The net current is superposition of incident and reflected currents. However, since the currents are traveling in opposite directions, the net current is the difference between them. Therefore, the load impedance is given by:

ZL=Ei+ErIiIrE4

Expression (4) can be rewritten to express ZL as function of Z0 as:

ZL=Ei+ErIiIr=EiIi[1+Er/Ei1Er/Ei]=Z0[1+Er/Ei1Er/Ei]E5

The ratio of reflected to incident quantities at the load end of the line is called Reflection Coefficient ΓL. Therefore, expression (5) can be rewritten as:

ZL=Ei+ErIiIr=Z0[1+ΓL1ΓL]E6

Solving for ΓL yields:

ΓL=ZLZ0ZL+Z0E7

As can be observed from expression (7), if the impedances of the load and the line are equal, there will be no reflection. If the line is terminated in either a short or an open circuit, the reflection will be maximum, with a magnitude of 1 [1].

Therefore, if a transmission line is terminated by its characteristic impedance there will be no reflection since all the transmitted power is absorbed by the load and the energy flows in just one direction.

When the line is terminated by a short circuit a reflected wave is sent back to the source since the short can not sustain any voltage, and therefore dissipates zero power. The incident and the reflected voltage waves are of the same magnitude. They are 180 out of phase at the load and they travel in opposite directions.

If the line is terminated by an open circuit a reflected wave is sent back to the source since the open can not sustain any current, and therefore dissipates zero power. The incident and the reflected current waves are of the same magnitude and travel in opposite directions. The current waves are 180 out of phase at the load, but the incident and reflected voltage waves are in phase [1].

If the line is terminated by an impedance different of the short, open and characteristic impedance, part of the signal will be absorbed by the load and part will be reflected back. The amount of reflected signal is given by expression (7).

## 3. Smith chart

The reflection coefficient ΓL of expression (7) was obtained from expression (6). By the same way, solving for ZL in expression (7) yields ΓL, thus forming a mapping of one complex number into another. The relationship between these two complex numbers forms a bilinear transformation, which means that knowing one is equivalent to knowing the other.

Since ZL can have any value and L| cannot exceed unity for passive loads, it is therefore much more convenient plotting ΓL than plotting ZL.

The reflection coefficient can become even more convenient by normalizing it to Z0, as:

Γ=ZLZ01ZLZ0+1=Z1Z+1E8

On the same way, normalizing (6) results in:

Z=1+Γ1ΓE9

Considering the normalized real and imaginary parts of both Γ and Z then:

Z=R+jX=1+Γ1Γ=1+Γr+jΓi1ΓrjΓiE10

After some algebraic manipulation (using conjugate), the real and imaginary parts are of Z are:

R=1Γr2Γi21+Γr22Γr+Γi2E11
X=2Γi1+Γr22Γr+Γi2E12

Expression (11) can be manipulated as:

R+RΓr22RΓr+RΓi2=1Γr2Γi2RΓr22RΓr+RΓi2+Γr2+Γi2=1RRΓr22RΓr+RΓi2+Γr2+Γi2=(1R)(1+R)(1+R)RΓr22RΓr+RΓi2+Γr2+Γi2=1(1+R)R2(1+R)Γr2(1+R)2RΓr+R2(1+R)+Γi2(1+R)=1(1+R)Γr22ΓrR(R+1)+R2(1+R)2+Γi2=1(1+R)2(ΓrRR+1)2+Γi2=(11+R)2E13

Similarly, expression (12) into:

(Γr1)2+(Γi1X)2=1X2E14

When the two parametric equations (13) and (14) are drawn on a complex coordinate, they build the Smithchart. Equation (13) forms resistance circles, and equation (14) generates reactance circles, as shown in Fig. 2 and Fig. 3, respectively. The resulting Smithchart is illustrated in Fig. 4.

As can be verified from expression (13), the imaginary axis in the Z-plane (resistance equals 0) is mapped as a unity circles into Γ-plane. The other lines of constant resistance in the Z-plane are also mapped as circles, but of different diameter in the Γ-plane. Nevertheless, they are all tangent at the point Γ=1, as shown in Fig. 2. The larger the value of the resistance, the smaller becomes the circle [1, 2].

As can be verified from expression (14), lines of constant reactance are perpendicular to lines of constant resistance in the Z-plane. This same orthogonality is preserved in the Γ-plane by having arcs perpendicular to the constant resistance lines, as indicated in Fig. 3.

The Smith, as shown in Fig. 4, is just the plotting of both constant resistance and constant reactance, but without the presence of the Γ axes. The center of the Smith chart corresponds to zero reflection (ZL equals Z0)[1].

The upper half of the Smith chart corresponds to the upper half part of the Z-plane, and therefore presents inductive loads. On the same way, the bottom half of the Smith chart corresponds to the bottom half part of the Z-plane, thus representing capacitive loads. Obviously, the Re axis of the Smith chart represents purely resistive loads.

Although the Smith chart presents many interesting and useful properties, they will no be presented here due to the focus of this material.

### 2.1. Admittance chart

The Smithchart is built by considering impedance (resistance and reactance). Once the Smithchart is developed, a similar approach can be used for admittance analysis. The concept that admittance is the inverse of impedance is very important for parallel circuit synthesis. Adding new elements in series can be resolved easily by adding the impedance values. However, summing elements in parallel can be cumbersome in terms of impedance. Thus, admittance is often considered for parallel elements.

By definition, admittance is expressed as:

where G is conductance and B is susceptance of the element. The reflection coefficient Γ can be expressed in terms of normalized admittance as:

The admittance reflection coefficient Γ(y) is given by definition as:

Γ(Y)=YLY0YL+Y0E17

As can be observed, the value of the admittance reflection coefficient Γ(y) is equal to –Γ, the reflection coefficient in terms of impedance. Therefore, once Γ is known, Γ(y) can be located a point at the same distance from the origin. Rotating the admittance point by 180 around the origin achieves the same result.

The admittance Smithchart can be obtained using the same procedure used to construct the impedance Smithchart. The normalized real and imaginary parts of Γ and Y can be given as:

Y=G+jB=1Γr2Γi2j2Γi1+Γr2+2Γi+Γi2E18

After some algebraic manipulation (using conjugate), the real and imaginary parts are of Y are:

G=1Γr2Γi21+Γr2+2ΓrΓi2E19
B=2Γi1+Γr2+2Γr+Γi2E20

Using the same procedure presented for expressions (13) and (14), then the parametric equations of the admittance Smithchart are:

(Γr+GG+1)2+Γi2=(11+G)2E19
(Γr+1)2+(Γi+1B)2=1B2E20

When the two parametric equations (21) and (22) are drawn on a complex coordinate, they build the Admittance Smithchart. Equation (21) forms resistance circles, and equation (22) generates reactance circles, as shown in Fig. 5.

## 3. S Parameters

At low frequencies, linear systems can be analyzed by means of voltages and currents applied to its ports. The two port circuit shown in Fig. 5 could be analyzed from its impedance (Z-parameters), admittance (Y-parameters), or a mixture of them, which could be hybrid (H-parameters) and inverse-hybrid (G-parameters).

As an example, the circuit of Fig. 5 could be analyzed using H parameters whose equations are:

V1=h11I1+h12V2I2=h21I1+h22V2E23

As can be observed from the equations, the value of h11 (port 1 impedance) can be obtained directly from the relationship of V1 and I1 when V2 is set to zero. A voltage source is set to zero by shortening its terminals. The value of h21 (current gain from port 1 to port 2) is obtained from the relationship of I1 and I2 also when V2 is set to zero.

By the same way, h12 (voltage gain from port 2 to port 1) can be obtained from the relationship of V1 and V2 when I1 is set to zero. A current source is set to zero by opening its terminals. Finally, h21 (port 2 conductance) is obtained from the relationship of V2 and I2 when I1 is set to zero.

Shorting or opening terminals is feasible at low frequencies but virtually impossible at high frequencies, particularly over a broad range of frequencies. Additionally, RF circuits are very sensitive to impedances, and they may oscillate or just quit working when terminated with open or short circuits. Therefore, Z-parameters, Y-parameters, H-parameters and G-parameters are not suitable to high frequency operations.

For high frequency operations, the scattering parameters (or just S-parameters) are employed. The input and output variables in S-parameters are based on incident and reflected voltage waves instead of voltages and currents.

The S-parameters takes advantage of the fact that there is no reflection in a line terminated in its characteristic impedance. Therefore, it is necessary a circuit representation for S-parameters, where source and the load terminations are Z0, as shown in Fig. 6.

The S-parameters equations are:

b1=s11a1+s12a2b2=s21a1+s22a2E24

where

a1=Ei1/Z0a2=Ei2/Z0b1=Er1/Z0b1=Er2/Z0E25

The normalization by Z0is very convenient since the square of a and b corresponds to the power of the incident and reflected waves.

S11 and S21 can be obtained by measuring the incident, the reflected and the transmitted signals at the input when the output is terminated in Z0. Once the output is terminated by Z0 there is no reflection. The values of S11 and S21 are:

S11=b1a1=Er1Ei1=Γ1S21=b2a1=Er2Ei1E26

Similarly, S12 and S22 can be obtained by measuring the incident, the reflected and the transmitted signals at the output when the input is terminated in Z0. Since the input is terminated by Z0 there is no reflection. The values of S12 and S22 are:

S12=b1a2=Er1Er2S22=b2a2=Er2Ei2=Γ2E27

S11 corresponds to the input reflection coefficient, S21 is the input to output (direct) gain, S12 is the reverse transmission gain and S22 corresponds to the output reflection coefficient.

The magnitudes of S11 and S22 are always less than 1, where a value of zero represents a perfect matching (no reflections), and the closer to 1, the higher the reflection.

The magnitudes of S21 (transfer characteristic) and S12 (reverse) are smaller than 1 for passive circuits but can exceed 1 for active circuits (amplification). A positive value means the input and output signal are in phase and a negative indicates a phase shift.

### 3.1. Measurements of S-Parameters

The circuit topology used to measure S-Parameters is given in Fig. 7.

The input reflection coefficient S11 from expression (18) can be modified as:

S11=Γ1=ZLZ0ZLZ0=2.ZLZLZ01E28

This expression, using the concepts of voltage division, corresponds to:

S11=Γ1=2.ZLZLZ01=2.V1VS1E29

Here, ZL corresponds to the input impedance of the two-port circuit. The value of the input to output gain, S21 is given as:

S21=2.V2VSE30

The value of S22 and S12 can be obtained in a similar way by just exchanging input and output terminals.

### 3.1. S Parameters in the Smith chart

The center point of the Smith chart corresponds to the point of zero reflection, where ZL equals Z0. Plots of S11 and S22 on the real axis represent ohmic resistors, above the axis indicate inductive load while below the axis indicate capacitive loads.

Plots of S12 and S21 inside the Smith chart indicate that damping signal between ports, whereas plots outside the chart indicate amplification [1].

As the frequency increases, the S-Parameters plots in the Smith chart move clockwise.

Given the value of S11, the circuit impedance can be found from (6), as:

ZL=Z0[1+S111S11]E29

### 3.2. Application example

The S11 and S21 parameters can be obtained as given by expressions (21) and (22), indicated in Fig. 7, and the values are calculated as for S11 and S21, respectively. As an application example, consider the cascode amplifier shown in Fig. 8 [2].

Fig. 10 shows its S11 parameter, in the Smith chart. The frequency is ranging from 4GHz to 6GHz. As the frequency increases, the plot moves clockwise. At approximately 5GHZ, the circuit presents a pure resistive impedance of approximately 50Ω (it crosses the horizontal axis). The circuit presents a capacitive behavior for frequencies bellow 5HGz and an inductive behavior for higher frequencies [1].

The same parameters could be plotted in a standard dB format, as shown in Fig. 11. The graph of Fig. 10 provides more information and insight than the graph of Fig. 11. The last one provides only the magnitude, whereas the first one provides both the imaginary and real part, so that it is possible to infer a capacitive and/or inductive behavior of the circuit, among other information.

Unfortunately, it is not always possible to analyze S-parameters using Smith chart. One such case is S11 that is usually larger than 1 for active circuits. If it is larger than one, it does not fit the Smith chart!

## 4. Noise figure/factor

In analog circuits at low frequency, the signal-to-noise figure (SNR), defined as the ratio of signal power to the noise power, is an important and very used parameter. As an example, in a radio receiver, it indicates the quality of the demodulated signal [2-5].

Nevertheless, as the signal passes through the RF circuits, the SNR changes. This signal-to-noise degradation along the system is described by the noise factor (F), as:

F=SNRiSNRo=SiNiSoNoE32

where the index i refers to input and the index o refers to output.

If a system has no noise, then SNRo = SNRi regardless of the gain, and F=1. This would be case of a hypothetical noiseless amplifier. Therefore, the noise figure of a real system will be always larger than 1.

Considering A as the system gain, expression (24) can be modified to:

F=SiNiSoNo=SiNiSi.ANo=NoA.NiE33

which can be seen as the total output noise power over the output noise due to the input source.

The total output noise is the sum of the original noise at the input (which was amplified) and the noise added by the circuit. This can be denoted as:

Therefore, expression (18) can be expressed also as:

Again, if the circuit adds no noise, F becomes 1.

Another important figure of merit is the noise figure, NF, expressed as:

NF=10.log10FE36

While the noise factor of a noiseless circuit is 1, the noise figure is 0dB.

### 4.1. Noise figure of a cascade system

Fig. 12 shows a cascade amplifying system, whose gain of each stage is Ai and the noise added by each stage is Ni-added.

The output noise due to the source is:

Nosource=Ni.A=Ni.A1.A2.A3E37

While the total output noise is:

which is the input noise multiplied by the gain of the three stages, plus the noise generated by the first stage and amplified by the stages 2 and 3, plus the noise generated by the second stage and amplified by the last stage, and plus the noise generated by the last stage.

Thus, combining expressions (29) and (30) into expression (25), the noise factor can be found as:

This expression, with the aid of expression (27), can be re-written as:

F=F1+F21A1+F31A1A2E40

As can be observed from expression (32), the noise factor of the first stage is the most relevant to the total noise factor. That is the reason for putting most effort in the first stage in terms of noise minimization, thus requiring low noise amplifiers at the front of the system.

## 5. Conclusions

The basic knowledge of impedance matching between source and load, either with or without a transmission line is essential to the design of RF circuits. The analysis presented can be conducted by using Smith Charts and S-Parameters. The analysis in this chapter was oriented to RFID applications whereas other books provide general analysis.

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© 2011 The Author(s). Licensee IntechOpen. This chapter is distributed under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike-3.0 License, which permits use, distribution and reproduction for non-commercial purposes, provided the original is properly cited and derivative works building on this content are distributed under the same license.

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Paulo Crepaldi, Tales Pimenta and Luis Ferreira (July 20th 2011). Radio Frequency Background, Current Trends and Challenges in RFID, Cornel Turcu, IntechOpen, DOI: 10.5772/20648. Available from:

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