Difference between revisions of "T pad"

Latest revision as of 13:50, 10 December 2011

The T pad is a specific type of attenuator circuit in electronics whereby the topology of the circuit is formed in the shape of the letter "T".

Attenuators are used in electronics to reduce the level of a signal. They are also referred to as pads due to their effect of padding down a signal by analogy with acoustics. Attenuators have a flat frequency response attenuating all frequencies equally in the band they are intended to operate. The attenuator has the opposite task of an amplifier. The topology of an attenuator circuit will usually follow one of the simple filter sections. However, there is no need for more complex circuitry, as there is with filters, due to the simplicity of the frequency response required.

Circuits are required to be balanced or unbalanced depending on the geometry of the transmission lines they are to be used with. For radio frequency applications, the format is often unbalanced, such as coaxial. For audio and telecommunications, balanced circuits are usually required, such as with the twisted pair format. The T pad is intrinsically an unbalanced circuit. However, it can be converted to a balanced circuit by placing half the series resistances in the return path. Such a circuit is called an H-section, or else an I section because the circuit is formed in the shape of a serifed letter "I".

Terminology

An attenuator is a form of a two-port network with a generator connected to one port and a load connected to the other. In all of the circuits given below it is assumed that the generator and load impedances are purely resistive (though not necessarily equal) and that the attenuator circuit is required to perfectly match to these. The symbols used for these impedances are;

<math>Z_1 \,\!</math> the impedance of the generator

<math>Z_2 \,\!</math> the impedance of the load

Popular values of impedance are 600Ω in telecommucations and audio, 75Ω for video and dipole antennae, 50Ω for RF

The voltage transfer function, A, is,

<math>A = \frac{V_\mathrm {out}}{V_\mathrm {in}}</math>

While the inverse of this is the loss, L, of the attenuator,

<math>L = \frac{V_\mathrm {in}}{V_\mathrm {out}}</math>

The value of attenuation is normally marked on the attenuator as its loss, L_dB, in decibels (dB). The relationship with L is;

<math>L_\mathrm{dB} = 20 \log L \,\!</math>

Popular values of attenuator are 3dB, 6dB, 10dB, 20dB and 40dB.

However, it is often more convenient to express the loss in nepers,

<math> L = e^\gamma \,</math>

where <math>\gamma \,</math> is the attenuation in nepers (one neper is approximately 8.7 dB).

Impedance and loss

The values of resistance of the attenuator's elements can be calculated using image parameter theory. The starting point here is the image impedances of the L section in figure 2. The image impedance of the input is,

<math>Z_\mathrm {i T} = \sqrt {Z^2 + \frac{Z}{Y}}</math>

and the image admittance of the output is,

<math>Y_\mathrm {i \Pi} = \sqrt {Y^2 + \frac{Y}{Z}}</math>

The loss of the L section when terminated in its image impedances is,

<math>L_\mathrm {L1} = \sqrt{Z_\mathrm {i T} Y_\mathrm {i \Pi}} \ e^{\gamma_\mathrm L}</math>

where the image parameter transmission function, γ_L is given by,

<math>\gamma_\mathrm L=\sinh^{-1}{\sqrt{ZY}}</math>

The loss of this L section in the reverse direction is given by,

<math>L_\mathrm {L2}=\sqrt{Z_\mathrm {i \Pi} Y_\mathrm {i T}} \ e^{\gamma_\mathrm L}</math>

For an attenuator, Z and Y are simple resistors and γ becomes the image parameter attenuation (that is, the attenuation when terminated with the image impedances) in nepers. A T pad can be viewed as being two L sections back-to-back as shown in figure 3. Most commonly, the generator and load impedances are equal so that Z₁ = Z₂ = Z₀ and a symmetrical T pad is used. In this case, the impedance matching terms inside the square roots all cancel and,

<math>L_\mathrm T = L_\mathrm {L1} L_\mathrm {L2} = e^{2 \gamma_\mathrm L} = e^{\gamma_\mathrm T} \,</math>

Substituting Z and Y for the corresponding resistors,

<math>\gamma_\mathrm T = 2 \gamma_\mathrm L = 2 \sinh^{-1}{\sqrt{\frac{R_1}{2R_2}}} \,</math>

<math>Z_0 = \sqrt {{R_1}^2 + 2R_1 R_2}</math>

These equations can easily be extended to non-symmetrical cases.

Resistor values

The equations above find the impedance and loss for an attenuator with given resistor values. The usual requirement in a design is the other way around – the resistor values for a given impedance and loss are needed. These can be found by transposing and substituting the last two equations above;

<math> R_1 = Z_0 \tanh \left ( \frac {\gamma_ \mathrm T}{2} \right )</math>

<math> R_2 = \frac {{Z_0}^2 -{R_1}^2}{2R_1} </math>

See also

• Π pad
• L pad

References

• Matthaei, Young, Jones, Microwave Filters, Impedance-Matching Networks, and Coupling Structures, pp.41-45, 4McGraw-Hill 1964.
• Redifon Radio Diary, 1970, pp.49–60, William Collins Sons & Co, 1969.