System Architecture - Frontend

In this problem we look at the paper written by Shafer, The Influence of Front-End Hardware on Digital Ultrasonic Imaging and get to know a bit more on the system Front-End.

Related materials:

by Lasse Løvstakken (lasse.lovstakken@ntnu.no) 12.11.2013

Contents

Front-end overview

Transmit chain

% Bipolar (+1,-1) or tripolar (+1,0,-1), arbitrary waveform generators
% (state of the art)
%* *What benefit could you have from transmitting an accurately defined
%pulse?*

% * Only emit in the transducer band, minimum waste of energy to heat
% * No emission of second harmonic (for harmonic imaging)
% * Advanced: multi-pulse transmission (MLT), pulse inversion (cancellation
% techniques)
% It acts as a band pass filter, smoothing out sharp edges and turning the
% input into a tapered sinusoidal shape
% * Ringing in the pulse means that you degrade the axial resolution
% * Insufficient amplitude means that you degrade penetration and also reduce
% the ability to do harmonic imaging
% * Transmitting outside the transducer band increases heating at the probe
% surface, this is very often a limiting factor which needs to be minimized

Receive chain

% Weak echoes, low voltage (micro-Volt). Need to bring the signal up to
% standard levels
% Pulse is attenuated as it propagates into the tissue
% * The dynamic range is the relative difference between the weakest and
% strongest echos. Due to depth dependent attenuation the dynamic range can
% be ~100dB.
% * The final dynamic range is determined by the resolution of the
% A/D-converter, e.g. 12 bit => 12*6dB = 72dB theoretical dynamic range.
% * Some extra dynamic range can also be gained through oversampling and in
% the coherent summation (lowers the noise floor).

What are the typical requirements of the analog-to-digital converter in an ultrasound system?

% * Low-end: 12 bit 40MHz
% % High-end: 14 bit, 62.5MHz
% * There is a mismatch in electrical impedance between the cable and
% transducer elements, leading to suboptimal transfer of signal energy
% * By tuning out this mismatch (typically capacitive) through the addition
% of a coil (inductance), a more “effective” system is achieved, e.g.
% improved signal-to-noise.
% * Most important on receive side to maximize SNR
% * Noise introduced by amplifiers and A/D-converters limits SNR and
% detectability
% * The limited dynamic range of A/D converters used infers that signal
% compression is needed (through depth-dependent preamplification)
% * The number of channels sets a lower limit on the F-number / aperture
% that can be achieved, i.e. influences lateral resolution.

Transucer

% Piezo-composites, e.g. PZT
% The acoustical impedance is the (complex) relationship between pressure and (particle) velocity
% Because it is very high (stiff) compared to the tissue, causing a
% mismatch that results in reflected waves at the interface, i.e. an
% inefficient transfer of energy.
% * The properties of the tissue, namely: density and speed of sound
% * The transducer load is also determined by the area of the transducer
% surface, which determines the effective mass that needs to be moved
% By introducing (quarter-wave) matching layers in between the
% piezo-element and tissue, which has an impedance in between the two, Zm =
% sqrt(Zpiezo*Ztissue)

Phased-array systems

% * That both focusing and (continuous) steering is done electronically,
% resulting in a sector image format
% * Fine steering delays are needed
% The pitch needs to be sufficiently small to avoid grating lobes, i.e.
% less than lambda/2 for a steering angle of +-45deg.
% * Smaller elements require more channels
% * Transmit delay quantization must be sufficiently small, i.e. the clock
% rate of transmit beamformer must be sufficiently high
% * Smaller elements means higher electrical impedance for each piezo-element,
% electrical impedance matching may be more crucial
% * Element directivity is given by the element width. The directivity
% pattern needs to be sufficiently wide to allow for large steering angles,
% typically +-45 deg for lambda/2 pitch probes.
% * The limited discretization of delay values can lead to the same delay
% value applied to multiple elements
% * This means that these elements effectively appear as one large element,
% leading to what appears as grating lobes, often also called quantization
% sidelobes due to their origin.
% * Mostly a problem for fine steering such as in phased-array operation