Name: single-diode ac to dc conversion
Uploaded: 2024-07-08T13:20:20.000Z
Duration: 1 min 20 s
Channel: JoVE

Um circuito retificador de diodo converte a tensão CA em uma tensão CC unidirecional usando configurações de meia onda ou onda completa.
Considere um circuito retificador de meia onda que consiste em um diodo, resistor e sinal senoidal de entrada em combinação em série.
Durante os semiciclos positivos do sinal de entrada, quando a tensão excede ou é igual à queda de tensão do diodo, ele se torna polarizado para frente, permitindo que a corrente flua.
A tensão de saída é então determinada subtraindo a queda de tensão do diodo da tensão de entrada.
Por outro lado, durante o meio ciclo negativo, a tensão de entrada é menor que a queda de tensão do diodo e o diodo permanece não condutor, resultando em uma tensão de saída zero.
Apesar da tensão de entrada mudar de polaridade com um valor médio de zero, a saída permanece unidirecional com um valor médio consistente devido à retificação.
A tensão inversa de pico representa a tensão reversa máxima que um diodo pode suportar sem danos.
Em um retificador de meia onda, isso ocorre durante semiciclos negativos, quando a tensão de entrada atinge seu pico na direção negativa.
Assim, a tensão inversa de pico é igual ao pico da tensão de entrada, mas com polaridade invertida.

retificador de meia onda

Um retificador de meia onda é um circuito fundamental em eletrônica, projetado para converter a tensão de corrente alternada (CA) em uma tensão unidirecional. Ele utiliza a forma mais simples de retificação de diodo, onde o circuito compreende um único diodo em série com um resistor de carga e uma fonte de alimentação CA.
<img alt="Figure 1" src="/files/ftp_upload/15719/15719_Figure_1.svg" style="height: 150px;">
A operação de um retificador de meia onda é baseada no princípio de que os diodos permitem o fluxo de corrente em apenas uma direção. Durante os semiciclos positivos da entrada CA, o diodo é polarizado diretamente à medida que a tensão de entrada excede o limite do diodo. Conseqüentemente, a corrente flui através do circuito e uma tensão de saída se desenvolve no resistor de carga. Esta tensão de saída é a tensão de entrada menos a queda de tensão direta do diodo.
Por outro lado, durante os semiciclos negativos, o diodo é polarizado reversamente. A tensão de entrada não é suficiente para superar a barreira de potencial inerente do diodo, tornando o diodo não condutor. Conseqüentemente, não há fluxo de corrente e a tensão de saída cai para zero. Esta retificação resulta em uma corrente contínua pulsante (CC) que flui apenas durante os semiciclos positivos do sinal CA de entrada.
Um parâmetro crucial para diodos em circuitos retificadores é a tensão inversa de pico (PIV). Esta é a tensão máxima que o diodo pode suportar em condições de polarização reversa sem sofrer ruptura. Em um retificador de meia onda, o PIV é essencialmente o valor de pico da tensão CA de entrada, mas com polaridade oposta. É vital que o diodo escolhido possa suportar o PIV esperado para evitar danos e garantir a longevidade do circuito.
<img alt="Equation 1" src="/files/ftp_upload/15719/15719_Equation_1.svg" style="height: 30px;">

Retificador de Meia Onda

Um circuito retificador de diodo converte a tensão CA em uma tensão CC unidirecional usando configurações de meia onda ou onda completa.
Considere uma meia onda ...

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KEY TERMS AND CONCEPTS

TERMOS E CONCEITOS-CHAVE

Half wave rectifier

single-diode ac to dc conversion

Single-diode AC to DC conversion uses a half-wave rectifier to change alternating current into a unidirectional voltage. The circuit is simple. It uses one diode in series with a load resistor and an AC power source.

The diode controls the current because it allows flow in only one direction. During the positive half-cycles of the AC input, the diode is forward-biased. When the input voltage is greater than the diode threshold, current flows and an output voltage appears across the load resistor. That output is the input voltage minus the diode's forward voltage drop.

During the negative half-cycles, the diode is reverse-biased. The input voltage cannot overcome the diode's internal barrier, so the diode does not conduct. As a result, no current flows and the output voltage falls to zero. The circuit therefore produces a pulsating DC signal that appears only during the positive half-cycles of the AC input.

Diode selection also matters in rectifier circuits because of peak inverse voltage, or PIV. PIV is the maximum reverse voltage a diode can withstand without breakdown. In a half-wave rectifier, the PIV is essentially the peak value of the input AC voltage with opposite polarity. The diode must handle this reverse voltage to avoid damage and help the circuit last longer.

Single-Diode AC to DC Conversion

the ideal diode

Ideal Diode I-V Curve and Rectification

An ideal diode is a simple model of a semiconductor diode used to show how current moves through circuits. A diode has two terminals. The anode is positive, and the cathode is negative. In this model, current can flow only in one direction. When a positive voltage is applied to the anode relative to the cathode, the diode is forward-biased. In that state, it conducts current. When the cathode is at a higher potential than the anode, the diode is reverse-biased. It then blocks current and acts...

diode: forward bias

Diode Current in Forward Bias

Diode current in forward bias depends on how the p-type and n-type regions are connected to a battery. When the p-type region is tied to the positive terminal and the n-type region to the negative terminal, the diode is forward-biased. This setup lowers the potential barrier inside the diode and lets current move easily from the p-type side to the n-type side. The current-voltage behavior of a forward-biased diode is described by its I-V characteristics. These characteristics depend on the...

diode: reverse bias

Diode Reverse Current and Breakdown

A diode in reverse bias blocks current flow and widens its depletion region. In this setup, the positive terminal of the power source connects to the n-type material, and the negative terminal connects to the p-type material. The reverse connection also raises the barrier potential, so current stays very small. The small reverse current is called leakage current. It comes mainly from minority charge carriers. At room temperature, once the reverse voltage is above the thermal voltage, the...

zener diodes

Zener Diode Voltage Regulation

Zener diodes are semiconductor devices used to hold voltage steady in reverse bias. In reverse breakdown, current flows into the cathode and makes it positive relative to the anode. This behavior is different from a conventional diode and is the reason Zener diodes are useful in voltage regulation. A Zener diode has a nearly vertical current-voltage, or I-V, curve above a threshold called the knee current. That shape lets it keep a fairly stable voltage over a wide range of currents.

modeling of diode forward characteristics

modeling-of-diode-forward-characteristics

Diode Forward Bias: I-V Curve and Models

Diode forward bias is analyzed with the current-voltage, or I-V, curve and two common circuit models. These models help describe how a diode behaves when current flows in the forward direction. They are useful for electronic circuit design and analysis. The exponential diode model is used when the source voltage rises above 0.5 volts. At that point, the diode current increases exponentially above the saturation current. The I-V curve shows this nonlinear response as the forward voltage...

small-signal diode model

Diode Bias and Small-Signal Response

Diode bias and small-signal response describe how a diode behaves when a steady DC voltage and a tiny changing signal act on the same circuit. The DC bias sets the diode’s operating point, or Q point. Around that point, the diode current and voltage follow an exponential I-V relationship. A small time-varying signal can be added on top of the DC bias to study how the diode responds to small changes. When the signal voltage is much smaller than the thermal voltage, the diode’s behavior can be...

modeling of diode reverse characteristics

modeling-of-diode-reverse-characteristics

Zener Diode Load-Line Modeling

Zener diode load-line modeling shows how a reverse-biased diode sets a steady voltage in a circuit. Zener diodes use reverse breakdown in a controlled way, so they can hold a fixed voltage across their terminals. This makes them useful for voltage regulation. When the reverse voltage rises above the Zener voltage, or VZ, the diode enters the breakdown region. In this region, the current-voltage, or I-V, curve becomes nearly vertical after the knee current, IZ, is reached. That means the...

half wave rectifier

Single-diode AC to DC conversion uses a half-wave rectifier to change alternating current into a unidirectional voltage. The circuit is simple. It uses one diode in series with a load resistor and an AC power source. The diode controls the current because it allows flow in only one direction. During the positive half-cycles of the AC input, the diode is forward-biased. When the input voltage is greater than the diode threshold, current flows and an output voltage appears across the load...

full wave rectifier

AC to DC Conversion with Full-Wave Rectifiers

A full-wave rectifier converts alternating current, or AC, into direct current, or DC. It is more efficient than a half-wave rectifier. The circuit usually uses a center-tapped transformer, two diodes, and a load resistor. The center-tapped transformer is the key part of the circuit. Its secondary winding is split into two equal voltages with opposite polarities. That split lets the rectifier use both halves of the AC input waveform. During the positive half-cycle of the AC signal, diode D1...

bridge rectifier

AC to DC Conversion with Bridge Diodes

A bridge rectifier converts alternating current (AC) into direct current (DC) using four diodes arranged in a bridge layout. It is used to turn both halves of the AC waveform into a single-direction output. That makes it an important part of many electronics circuits. During the positive half-cycle, diodes D1 and D2 conduct. Current then flows through the load resistor R. At the same time, D3 and D4 are reverse-biased, so they do not conduct. The action switches during the negative half-cycle.

clipper circuit

Dual Diode Wave Clipping

Dual diode wave clipping uses diodes and biasing batteries to reshape an AC signal. A clipper circuit is a wave-shaping device that changes waveform parts without changing the whole signal. It is commonly used in television and radar communication systems to improve waveform modulation in transmitters and receivers. A dual-clipper setup uses two ideal diodes, two biasing batteries, and a resistor connected in parallel. The circuit works by responding to the phase of the input AC signal. The...

clamper circuit

DC Restorer for Waveform Level Shifting

A clamper circuit, or DC restorer, shifts a waveform up or down by adding a DC level. It is a special form of rectifier circuit. In this setup, the output is taken across the diode instead of across the capacitor. The circuit works well with square wave inputs and other pulse signals. The diode direction lets the capacitor charge to the most negative peak of the input signal. After that, the diode stops conducting. The capacitor then holds that voltage at a steady value. As a result, the...

voltage doubler circuit

How a Voltage Doubler Raises AC Output

A voltage doubler circuit raises the output voltage by using a clamping section and a rectifier section. The clamping section includes a capacitor, C1, and a diode, D1. The rectifier section includes a second diode, D2, and a capacitor, C2. The circuit starts working when a sinusoidal input signal enters the clamping section. Under ideal conditions, this stage clamps the positive peaks at zero volts. It also lets the negative peak reach a magnitude that is twice the input amplitude. That...

schottky barrier diode

Fast Switching in Schottky Diodes

Schottky barrier diodes use a metal-semiconductor junction to control current flow. They are built by combining a metal layer with a moderately doped n-type semiconductor. This contact creates the Schottky barrier, which gives the diode its one-way current behavior. When the metal touches the semiconductor, charge transfer occurs. The Fermi levels of the two materials align, and a depletion region forms near the contact area. In an n-type semiconductor, this region contains uncompensated...

key terms and concepts

Learn how a half-wave rectifier uses one diode and a load resistor to convert AC into pulsating DC, including forward bias, reverse bias, and PIV.

Single-Diode AC to DC Conversion | JoVE K12

JoVE Core Electrical Engineering offers easy-to-understand animated videos that cover fundamental concepts of electric circuits along with circuit analysis techniques. It incorporates first-order and second-order circuits using operational amplifiers and circuit transformation concepts. The inclusion of practical design examples and real-world applications through scientist-in-action videos adds significant educational value, making complex concepts accessible.

electrical engineering

Single-Diode AC to DC Conversion

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