𝔖 Bobbio Scriptorium
✦   LIBER   ✦

A generalized method for characterizing two-dimensional scattering problems with spectral techniques

✍ Scribed by H. Esteban; J. M. López; V. E. Boria; M. Baquero; M. Ferrando


Publisher
John Wiley and Sons
Year
1997
Tongue
English
Weight
133 KB
Volume
14
Category
Article
ISSN
0895-2477

No coin nor oath required. For personal study only.

✦ Synopsis


input voltages that provide useful circuit operation. Figure 4 shows the measured return loss of a typical attenuator chip at Ž 7 GHz. Return loss is similar at other frequencies within the . range of 7᎐18 GHz. The lower left region represents the minimum loss state of the attenuator, with series HEMT on and shunt HEMT off. As V is made less negative to increase 2 the attenuation by the shunt HEMTs, V must be made more 1 negative to maintain low return loss. This is easily understood by considering that the behavior of the HEMT varistor ladder network is closely analogous to a resistive tee or pi network. To achieve very high attenuation, V must be increased 2 toward 0 V, whereas V is kept relatively constant. This can 1 also be understood by the resistor network analogy. Although Ž . high ) 50 dB attenuation is achieved in this region, the phase error is large, in the tens of degrees. Low phase error can, however, be achieved, with the chip operated up to an attenuation of 20᎐30 dB.

Ž . Ž .


📜 SIMILAR VOLUMES


A generalized method for two dimensional
✍ J. M. López; V. E. Boria; M. Baquero; M. Ferrando 📂 Article 📅 1996 🏛 John Wiley and Sons 🌐 English ⚖ 485 KB 👁 2 views

A new method for characreming electrically large scatteren and solring the scattering of multiple objects in two dimensions for TE polarization of the incldent field i s presented. Large objects are dicided into smaller ones. The method of moments and spectral techniques are used to compute a transf

A rapidly convergent iterative method fo
✍ Robert J. Adams; Gary S. Brown 📂 Article 📅 1999 🏛 John Wiley and Sons 🌐 English ⚖ 221 KB 👁 1 views

Figure 3 Comparison of the normalized phase velocity computed w x by using the new expression of and the expression in 1 with r, eff, p the measurements Figure 4 Comparison of the interaction impedance computed by w x using the new expression of and the expression in 1 with the r, eff, p measurement