Large-Signal Characterization of Coupled RF Amplifiers for Parallel Transmit

نویسندگان

  • Michael Twieg
  • Mark A Griswold
چکیده

Target audience: This work is relevant to those interested in parallel transmit amplifiers. Purpose: Previous work has demonstrated the use of high efficiency switch mode power amplifier (SMPA) topologies for miniature on-coil amplifiers aimed at use in parallel transmit coil arrays. Though such amplifiers demonstrate very high efficiency and power density in isolation, there has not yet been any detailed quantification of how these amplifiers behave when the RF coils are coupled to each other, primarily due to their relatively complex behavior. Linear power amplifiers (LPA) are normally assumed to be time invariant, homogeneous, and additive, making them simpler to model using linearized parameters such as transconductance, complex impedance, and scattering parameters. SMPA topologies, such as the Current Mode Class D (CMCD) topology shown in fig 1, are different in that they are inherently periodically-timevarying systems, and they show strong nonlinear behavior. To address these issues, we have developed a method for experimentally quantifying the effective open loop output impedance and power efficiency of coupled power amplifier topologies across their full control space, and we demonstrate its application to the CMCD topology. Methods: CMCD coupling model: The coupling phenomenon observed in coil arrays is due to magnetic and electric fields from one coil element inducing an electromotive force ε in neighboring coils. This work focuses solely on the role of magnetic flux coupling, described by km between two coils with inductances L1 and L2. The ε21 inducted in coil L1 by current IL2 in coil L2 is given by 21 L2 m 1 2 ε =jωI k L L . This ε21 will alter the current in coil L1 according to

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Parallel excitation with an array of transmit coils.

Theoretical and experimental results are presented that establish the value of parallel excitation with a transmit coil array in accelerating excitation and managing RF power deposition. While a 2D or 3D excitation pulse can be used to induce a multidimensional transverse magnetization pattern for a variety of applications (e.g., a 2D localized pattern for accelerating spatial encoding during s...

متن کامل

Robust Parallel Excitation Pulse Design

Introduction Parallel excitation employs multiple transmit channels and coils, each driven by independent waveforms, to afford the pulse designer an additional spatial encoding mechanism, i.e., transmit sensitivity encoding, that complements gradient encoding. However, in contrast to parallel reception, parallel excitation requires individual high-power amplifiers for each transmit channel, whi...

متن کامل

Assessment of the Characteristics of MRI Coils in Terms of RF Non-Homogeneity Using Routine Spin Echo Sequences

Introduction: One of the major causes of image non-uniformity in MRI is due to the existence of  non-homogeneity in RF receive and transmit. This can be the most effective source of error in  quantitative  studies  in  MRI  imaging.  Part  of  this  non-homogeneity  demonstrates  the  characteristics of RF coil and part of it is due to the interaction of RF field with the material being  imaged...

متن کامل

32 Channel Coil Array for Parallel RF Transmission

Introduction: As part of a study that investigates a substantially distributed multi-channel parallel transmit approach, head-size 32-element transmit/receive arrays were developed. The specific goal of the coil development is to facilitate reduction of RF power dissipation in the imaged object / the coil structure, and to facilitate B1 shimming / accelerated parallel excitation for an arbitrar...

متن کامل

Highly Distributed RF Transmission with a 32-Channel Parallel Transmit System

Introduction: When RF signal gets transmitted (Tx) / detected (Rx), the B1 / B1 fields interact with the spin system of the imaged object, forming the basis of MR signal induction / detection. The concomitant E field meanwhile gives rise to RF loss in the object and dictates SAR / noise. An MR system implements / optimizes the RF electromagnetic fields for MR via the currents in an RF coil stru...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 2013