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Integrated analog front end for ultrasound applications
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The News - Semiconductor news
Written by Bogdan   

Integrated analog front end for ultrasound applications

Texas Instruments  new AFE5805 analog front end provides the lowest power consumption and lowest noise in an ultra-small 15 mm x 9 mm package. It is the first device in TI’s new AFE58xx family that integrates multiple high-performance analog components providing superior image quality for a wide range of ultrasound equipment.

The AFE5805 is a complete analog front-end device specifically designed for ultrasound systems that require low power and small size.

The AFE5805 consists of eight channels, including a low-noise amplifier (LNA), voltage-controlled attenuator (VCA), programmable gain amplifier (PGA), low-pass filter (LPF), and a 12-bit analog-to-digital converter (ADC) with low voltage differential signaling (LVDS) data outputs.

The LNA gain is set for 20dB gain, and has excellent noise and signal handling capabilities, including fast overload recovery. VCA gain can vary over a 46dB range with a 0V to 1.2V control voltage common to all channels of the AFE5805.

The PGA can be programmed for gains of 20dB, 25dB, 27dB, and 30dB. The internal low-pass filter can also be programmed to 10MHz or 15MHz.

Image

The LVDS outputs of the ADC reduce the number of interface lines to an ASIC or FPGA, thereby enabling the high system integration densities desired for portable systems. The ADC can either be operated with internal or external references. The ADC also features a signal-to-noise ratio (SNR) enhancement mode that can be useful at high gains.

The AFE5805 is available in a 15mm × 9mm, 135-ball BGA package that is Pb-free (RoHS-compliant) and green. It is specified for operation from 0°C to +70°C.

 

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A new PIC was born ! Welcome PIC32 :)
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The News - Semiconductor news
Written by Bogdan   

 PIC32

Microchip Technology Inc. announced the PIC32 family of 32-bit microcontrollers (MCUs). The PIC32 family adds more performance and more memory while maintaining pin, peripheral and software compatibility with Microchip’s 16-bit MCU/DSC families. To further ease migration and protect tool investments, the PIC32 family is fully supported by Microchip’s free MPLAB® Integrated Development Environment (IDE). The MPLAB IDE offers unprecedented compatibility by supporting Microchip’s complete portfolio of 8-, 16- and 32-bit devices.

“As a world leader in embedded-control solutions, Microchip is introducing the PIC32 family to build on the success of our vast 8- and 16-bit portfolio and offer customers a seamless migration path that bridges product families,” said Ganesh Moorthy, executive vice president of Microchip. “We provide designers with the most compatible environment in the industry for developing systems with 8-, 16-, and 32-bit MCUs!”

Consumers’ desire for ever-more engaging end products is driving system requirements for increased memory capacity, performance and functionality. Launching with seven general-purpose members, the PIC32 family operates at up to 72 MHz and offers ample code- and data-space capabilities with up to 512 KB Flash and 32 KB RAM. The PIC32 family also includes a rich set of integrated peripherals, significantly reducing total design complexity and cost. Examples include a variety of communication peripherals, a 16-bit Parallel Master Port supporting additional memory and displays, as well as a single-supply on-chip voltage regulator.

“Microchip brings a new perspective to the ever-growing 32-bit microcontroller market, born of their tremendous success in the 8-bit market,” said Tom Starnes, processor analyst at semiconductor market research firm Objective Analysis. “The peripheral-compatible PIC32 family should bring comfort to Microchip’s customers, knowing that the headroom is available as their applications evolve.”

The PIC32 family is based on the industry-standard MIPS32® architecture, with its leading combination of high performance, low power consumption, fast interrupt response and extensive industry tool support. The high-performance MIPS32 M4K® core can achieve best-in-class 1.5 DMIPS/MHz operation, due to its efficient instruction-set architecture, 5-stage pipeline, hardware multiply/accumulate unit and up to 8 sets of 32 core registers. To reduce system cost, the PIC32 supports MIPS16e™ 16 bit ISA—enabling code-size reductions of up to 40%.

“In the hands of the architects at Microchip, the MIPS architecture will do well in 32-bit MCUs,” said Max Baron, principal analyst at In-Stat. “Microchip gets a great architecture, while MIPS gets to be part of a series of MCUs from a company that is very successful in the MCU market. It’s a win-win for both companies.”

 

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Wheatstone bridge
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Electronics lessons - General electronics
Written by Sergiu   

Wheatstone bridge

A Wheatstone bridge is a measuring instrument invented by Samuel Hunter Christie in 1833 and improved and popularized by Sir Charles Wheatstone in 1843. It is used to measure an unknown electrical resistance by balancing two legs of a bridge circuit, one leg of which includes the unknown component. Its operation is similar to the original potentiometer except that in potentiometer circuits the meter used is a sensitive galvanometer.

Wheatstone's bridge circuit diagram.
Wheatstone's bridge circuit diagram.

In the circuit at right, Rx is the unknown resistance to be measured; R1, R2 and R3 are resistors of known resistance and the resistance of R2 is adjustable. If the ratio of the two resistances in the known leg (R2 / R1) is equal to the ratio of the two in the unknown leg (Rx / R3), then the voltage between the two midpoints will be zero and no current will flow between the midpoints. R2 is varied until this condition is reached. The current direction indicates if R2 is too high or too low.

Detecting zero current can be done to extremely high accuracy (see Galvanometer). Therefore, if R1, R2 and R3 are known to high precision, then Rx can be measured to high precision. Very small changes in Rx disrupt the balance and are readily detected.

If the bridge is balanced, which means that the current through the galvanometer Rg is equal to zero, the equivalent resistance of the circuit between the source voltage terminals is:

R1 + R2 in parallel with R3 + Rx

R_E = {{(R_1 + R_2) \cdot (R_3 + R_x)}\over{R_1 + R_2 + R_3 + R_x}}

Alternatively, if R1, R2, and R3 are known, but R2 is not adjustable, the voltage or current flow through the meter can be used to calculate the value of Rx, using Kirchhoff's circuit laws (also known as Kirchhoff's rules). This setup is frequently used in strain gauge and Resistance Temperature Detector measurements, as it is usually faster to read a voltage level off a meter than to adjust a resistance to zero the voltage.

Derivation

First, we can use the first Kirchhoff rule to find the currents in junctions B and D:

I_3\ - I_x\ - I_g\ =\ 0
I_1\ + I_g\ - I_2\ =\ 0

Then, we use Kirchhoff's second rule for finding the voltage in the loops ABD and BCD:

I_3 \cdot R_3 + I_g \cdot R_g - I_1 \cdot R_1 = 0
I_x \cdot R_x - I_2 \cdot R_2 - I_g \cdot R_g = 0

The bridge is balanced and Ig = 0, so we can rewrite the second set of equations:

I_3 \cdot R_3 = I_1 \cdot R_1
I_x \cdot R_x = I_2 \cdot R_2

Then, we divide the equations and rearrange them, giving:

R_x = {{R_2 \cdot I_2 \cdot I_3 \cdot R_3}\over{R_1 \cdot I_1 \cdot I_x}}

From the first rule, we know that I3 = Ix and I1 = I2. The desired value of Rx is now known to be given as:

R_x = {{R_3 \cdot R_2}\over{R_1}}

If all four resistor values and the supply voltage (Vs) are known, the voltage across the bridge (V) can be found by working out the voltage from each potential divider and subtracting one from the other. The equation for this is:

V = {{R_x}\over{R_3 + R_x}}V_s - {{R_2}\over{R_1 + R_2}}V_s

This can be simplified to:

V = \left({{R_x}\over{R_3 + R_x}} - {{R_2}\over{R_1 + R_2}}\right)V_s

The Wheatstone bridge illustrates the concept of a difference measurement, which can be extremely accurate. Variations on the Wheatstone bridge can be used to measure capacitance, inductance, impedance and other quantities, such as the amount of combustible gases in a sample, with an explosimeter. The Kelvin Double bridge was one specially adapted for measuring very low resistances. This was invented in 1861 by William Thomson, Lord Kelvin.

The concept was extended to alternating current measurements by James Clerk Maxwell in 1865 and further improved by Alan Blumlein in about 1926.

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