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Related Concept Videos

Second-order Op Amp Circuits01:19

Second-order Op Amp Circuits

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Implementing second-order low-pass filters in audio systems is crucial in refining audio signals by eliminating undesirable high-frequency noise. These filters typically involve second-order op-amp circuits configured as voltage followers, encompassing two nodes with distinct storage elements.
The analysis of such circuits follows a systematic approach, similar to the second-order RLC circuits. In practical scenarios, bulky inductors are rarely employed due to their size and weight. This means...
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Second-Order Circuits01:17

Second-Order Circuits

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Integrating two fundamental energy storage elements in electrical circuits results in second-order circuits, encompassing RLC circuits and circuits with dual capacitors or inductors (RC and RL circuits). Second-order circuits are identified by second-order differential equations that link input and output signals.
Input signals typically originate from voltage or current sources, with the output often representing voltage across the capacitor and/or current through the inductor. For example, in...
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Design Example: Underdamped Parallel RLC Circuit01:17

Design Example: Underdamped Parallel RLC Circuit

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Consider designing an oscillator circuit, a crucial component in various electronic devices and systems. The objective is to create an oscillator circuit with specific characteristics: a damped natural frequency of 4 kHz and a damping factor of 4 radians per second. To accomplish this, a parallel RLC circuit is employed, known for its ability to sustain oscillations at a resonant frequency. In this case, the damping factor is pivotal in achieving the desired performance.
Starting with a fixed...
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Parallel Resonance01:23

Parallel Resonance

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The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
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Linear Approximation in Frequency Domain01:26

Linear Approximation in Frequency Domain

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Linear systems are characterized by two main properties: superposition and homogeneity. Superposition allows the response to multiple inputs to be the sum of the responses to each individual input. Homogeneity ensures that scaling an input by a scalar results in the response being scaled by the same scalar.
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
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Parallel RLC Circuits01:14

Parallel RLC Circuits

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Street lamps equipped with RLC surge protectors are an excellent example of applying circuit analysis in practical scenarios. These surge protectors safeguard the lamp's components against sudden voltage spikes.
A simplified parallel RLC circuit model with a DC input source generating a step response is employed in this context. When the switch is turned on, Kirchhoff's current law is applied, leading to a second-order differential equation.
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Related Experiment Video

Updated: Apr 6, 2026

Microparticle Manipulation by Standing Surface Acoustic Waves with Dual-frequency Excitations
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First and second order derivatives for optimizing parallel RF excitation waveforms.

Kurt Majewski1, Dieter Ritter2

  • 1Siemens AG, CT RTC BAM ORD-DE, 80200 Munich, Germany.

Journal of Magnetic Resonance (San Diego, Calif. : 1997)
|August 2, 2015
PubMed
Summary

This study presents a numerical optimization method for designing radiofrequency (RF) pulses in magnetic resonance imaging (MRI). It simplifies the Bloch equations for faster computation of RF waveforms, improving magnetization control.

Keywords:
Bloch equationHessian matrixInterior-point algorithmParallel transmit excitationRadio frequency pulse designSmall tip angle

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Area of Science:

  • Magnetic Resonance Imaging (MRI)
  • Biophysics
  • Computational Science

Background:

  • Solving Bloch equations for piecewise constant magnetic fields allows explicit magnetization calculation.
  • Excitation pulses can be represented as sequential rotations of initial magnetization.
  • Minimizing magnetization differences requires solving finite-dimensional optimization problems for RF waveforms.

Purpose of the Study:

  • To develop a numerical optimization method for designing parallel RF waveforms.
  • To minimize the difference between achieved and desired magnetization across voxels.
  • To formulate the optimization problem using quaternion calculus and derive its derivatives.

Main Methods:

  • Formulation of the optimization problem in the magnitude least squares variant using quaternion calculus.
  • Specification of first and second order derivatives of the objective function.
  • Development of algorithms for first and second order derivatives, including a small tip angle approximation.

Main Results:

  • A small tip angle approximation was derived via first-order Taylor expansion.
  • Algorithms for first and second order derivatives were developed for the approximation.
  • Computational efforts were precisely quantified using floating-point operation counts.

Conclusions:

  • The numerical optimization method, implemented with an interior-point solver, effectively addresses RF waveform design.
  • The method was applied to literature examples, demonstrating its practical applicability.
  • Quaternion calculus provides an efficient framework for optimizing RF pulses in MRI.