Name: second-order op amp low-pass filters
Uploaded: 2024-04-11T12:48:44.000Z
Duration: 1 min 19 s
Channel: JoVE

オーディオ信号の望ましくない高周波ノイズを除去するために、2次ローパスフィルタを使用するオーディオシステムについて考えてみましょう。
このセットアップには、電圧フォロワ構成の2次オペアンプ回路と、2つのストレージ要素で構成される2つのノードが含まれています。
これらのノードにキルヒホッフの現在の法則を適用すると、2つの微分方程式が得られます。
さらに、帰還コンデンサの両端の電圧は、抵抗の電圧から他のコンデンサの電圧を差し引いたものに等しくなります。
これらの方程式を利用して、最初のノードのKCL方程式からコンデンサ電圧を除去できます。
結果は、2 次特性微分方程式です。
この微分方程式の解には、過渡応答と定常状態応答の両方が含まれます。
過渡応答は時間とともに消散し、過減衰、過小減衰、および臨界減衰のシナリオにおけるソースフリー回路のソリューションに似ています。
回路が定常状態になると、コンデンサや抵抗に電流が流れなくなり、理想的なオペアンプの入力端子が電流の流入を防ぎます。その結果、定常状態の応答はソース電圧と一致します。
入力ソース電圧を排除すると、純粋な過渡応答が得られます。

利益相反は宣言されていません。

2 次オペアンプ回路

Second-order Op Amp Circuits

オーディオ システムに 2 次ローパス フィルターを実装することは、望ましくない高周波ノイズを除去してオーディオ信号を洗練する上で非常に重要です。 これらのフィルターには通常、電圧フォロワとして構成された 2 次のオペアンプ回路が含まれ、異なる記憶素子を備えた 2 つのノードが含まれます。

このような回路の解析は、2 次 RLC 回路と同様の体系的なアプローチに従います。 実際のシナリオでは、サイズと重量のため、かさばるインダクタが使用されることはほとんどありません。 これは、ここで主に RC 二次オペアンプ回路に焦点を当てていることを意味します。RC 2 次オペアンプ回路は、フィルターや発振器などのデバイスに広範な用途があります。

ノードにキルヒホッフの電流法則を適用すると、2 つの微分Figureが現れます。 さらに、回路コンポーネント間の電圧関係を観察することによって、2 次の特性微分Figureが推定されます。 このFigureは、過渡応答と定常状態応答の両方を表しています。

<img alt="Equation1" src="/files/ftp_upload/15103/15103_PT_Equation_1.svg" style="text-align: center; height: 34px;">

過渡応答は時間の経過とともに徐々に減少し、ソースフリー回路で見られるソリューションと類似しており、過減衰、過小減衰、臨界減衰シナリオの特性を示します。 回路が定常状態に達すると、コンデンサと抵抗器は電流を流さなくなり、理想的なオペアンプ入力端子が電流の流れをブロックします。 したがって、定常状態の応答は電源電圧と一致します。

特に、入力電源電圧を除去すると、純粋な過渡応答が得られます。 これらの 2 次オペアンプ回路は、オーディオ品質を向上させるためにさまざまな用途に使用でき、さまざまなオーディオ処理システムにおいて極めて重要です。 さまざまなダンピングシナリオの下での動作を理解することは、オーディオ信号の最適な改善を達成するのに役立ちます。

オーディオ信号の望ましくない高周波ノイズを除去するために、2次ローパスフィルタを使用するオーディオシステムについて考えてみましょう。
この設定は...

Education

JoVE Core

Electrical Engineering

電気工学

Unit 1

ユニット1

First and Second-Order Circuits

一次および二次回路

KEY TERMS AND CONCEPTS

主要な用語と概念

second-order op amp low-pass filters

Second-order op-amp low-pass filters remove unwanted high-frequency noise from audio signals. They are used in audio systems to refine sound quality. These filters are often built as voltage followers and have two nodes with storage elements.

The circuit analysis follows the same basic method used for second-order RLC circuits. In practice, bulky inductors are usually avoided because of their size and weight. For that reason, the focus here is on RC second-order op-amp circuits, which are common in filters and oscillators.

Applying Kirchhoff's current law at the nodes gives two differential equations. A second-order characteristic differential equation is then found from the voltage relationships across the circuit parts. That equation describes both the transient response and the steady-state response.

The transient response fades over time. It can show overdamped, underdamped, or critically damped behavior, much like the solutions for source-free circuits. When the circuit reaches steady state, the capacitors and resistors no longer carry current, and the ideal op-amp input terminals block current flow. As a result, the steady-state response matches the source voltage.

If the input source voltage is removed, the circuit shows a pure transient response. These second-order op-amp circuits are important in audio processing systems because they help improve audio quality. Knowing how the circuit behaves under different damping conditions helps explain how the filter shapes the signal.

Second-Order Op Amp Low-Pass Filters

first-order circuits

First-Order Circuits in Flashing Lamps

First-order circuits use a resistor and one energy storage element, either a capacitor or an inductor. They are common in electronic systems and are described by a first-order differential equation that links the input and output signals. One important example is the RC circuit, which uses a resistor and a capacitor. In a relaxation oscillator such as a neon lamp circuit, the capacitor starts charging when voltage is applied. At first, the lamp behaves like an open circuit. When the capacitor...

rc circuit without source

RC Capacitor Discharge After Power Loss

An RC circuit discharges after the DC source is removed. If the capacitor was fully charged first, its initial voltage, V0, provides the energy that drives the source-free circuit. Kirchhoff’s current law is applied at the top node of the circuit. The current terms for the resistor and capacitor are then substituted, which leads to a first-order differential equation. Rearranging, integrating, and taking the exponential gives the natural response of the circuit. The integration constant in...

rc circuit with source

RC Circuit Charging After a DC Step

An RC circuit with a DC source shows how a capacitor charges after a sudden voltage step. The applied source is treated as a unit step function, and the capacitor voltage is the step response of the circuit. This response describes how the circuit reacts right after the input changes. A capacitor cannot change its voltage instantly. So, immediately after the switch closes at t=0, the capacitor voltage stays at its initial value. Kirchhoff’s current law is then applied at that moment and...

rl circuit without source

RL Circuit Decay After Source Removal

An RL circuit begins to decay after the DC source is removed. At that moment, the circuit becomes source-free. If the inductor has an initial current, I0, it also stores initial energy. That stored energy drives the natural response of the circuit. Kirchhoff’s voltage law is applied around the loop. The inductor voltage and resistor voltage are substituted into the equation. This gives a first-order differential equation for the current. Rearranging the terms produces a logarithmic form, which...

rl circuit with source

RL Step Response Under a DC Source

An RL circuit connected to a DC source has a step response that changes over time. The response has two parts: the transient response and the steady-state response. The transient response is the short-lived reaction that happens right after the source is applied. During the transient phase, the current changes exponentially. If the circuit starts with current in the inductor, that current decays toward zero as time goes on. At this stage, the inductor acts like a short circuit, so the source...

design example: frog muscle response

RL Circuit and Frog Leg Current Response

An RL circuit is used to model the frog leg’s response to electrical stimulation. In this setup, the student studies how current changes in a resistor-inductor circuit can trigger muscle contraction. The circuit provides a way to control and measure the electrical impulses involved in the experiment. When the switch is closed, the frog’s leg shows a brief contraction. At steady state, the inductor acts like a short circuit. That lets current bypass the resistor and produces a mild, short...

second-order circuits

RLC Damping and Resonant Frequency

Second-order circuits use two energy storage elements, such as a capacitor and an inductor, to shape how current and voltage change over time. These circuits include RLC circuits, along with RC and RL circuits that have two capacitors or two inductors. Their behavior is described by second-order differential equations that connect the input signal to the output signal. The input usually comes from a voltage source or a current source. The output is often the voltage across the capacitor, the...

series rlc circuit without source

Natural Response of a Source-Free RLC Circuit

A source-free RLC circuit is a series circuit with a resistor, inductor, and capacitor, but no external energy source. It begins with the energy already stored in the capacitor and inductor. That stored energy drives the circuit at first. The circuit is described by a second-order differential equation. This equation shows how the resistor, inductor, and capacitor interact over time. The resistor removes energy from the circuit, so the solution has an exponential form. When the exponential...

types of responses of series rlc circuits

types-of-responses-of-series-rlc-circuits

Damping in Series RLC Circuit Responses

A source-free series RLC circuit shows three response patterns based on damping. The circuit is described by a second-order differential equation. Its complete solution is made from two distinct solutions. Those solutions depend on the roots, which are written in terms of the damping factor and the resonant frequency. When the damping factor is greater than the resonant frequency, both roots are real and negative. This gives an overdamped response. The circuit output decays slowly over time. <br...

series rlc circuit with source

Forced Response in a Series RLC Circuit

A series RLC circuit with a DC source can model an automobile ignition system. The circuit shows how a battery can produce the high voltage needed for a spark. In this case, the input DC voltage acts like a forcing step function. Applying Kirchhoff's voltage law leads to a second-order differential equation. A second-order differential equation is an equation with a term for the second derivative. The form of this equation is very similar to the one used for a source-free RLC circuit, so the...

parallel rlc circuits

Parallel RLC Step Response in Surge Protectors

Parallel RLC circuits help explain how a surge protector works in a street lamp. The circuit model uses a DC input source that creates a step response when the switch is turned on. This setup shows how the lamp’s components can be protected from sudden voltage spikes. When the switch closes, Kirchhoff’s current law is applied to the parallel RLC circuit. That leads to a second-order differential equation. The solution has two parts: a transient response and a steady-state response. The...

second-order op amp circuits

Second-order op-amp low-pass filters remove unwanted high-frequency noise from audio signals. They are used in audio systems to refine sound quality. These filters are often built as voltage followers and have two nodes with storage elements. The circuit analysis follows the same basic method used for second-order RLC circuits. In practice, bulky inductors are usually avoided because of their size and weight. For that reason, the focus here is on RC second-order op-amp circuits, which are...

design example: underdamped parallel rlc circuit

design-example-underdamped-parallel-rlc-circuit

Oscillator Design with a Parallel RLC Circuit

A parallel RLC circuit can be designed to work as an oscillator with underdamped behavior. This example targets a damped natural frequency of 4 kHz and a damping factor of 4 radians per second. A fixed resistance of 200 Ω is used as the starting point for the design. The first step is to find the capacitance. The damping factor is the reciprocal of twice the product of resistance and capacitance. Using that relationship, the needed capacitance value can be calculated from the given resistance...

key terms and concepts

Learn how second-order op-amp low-pass filters reduce audio noise, form characteristic equations, and show damping behavior in RC circuits.

Second-Order Op Amp Low-Pass Filters | JoVE K12

JoVE Core 電気工学 は、電気回路の基本概念と回路解析テクニックを網羅したアニメーションビデオシリーズです。オペアンプと回路変換および 1 次・ 2 次回路の概念を網羅しています。実験を撮影した実写動画では、設計例や現代社会での応用が含まれており、複雑な概念も分かりやすく学習いただけます。

electrical engineering

Second-Order Op Amp Low-Pass Filters

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