Reactance voltage is a term often used in the context of transformers and other inductive devices. It refers to the voltage that develops across the inductive reactance of a transformer when an alternating current (AC) flows through its windings. To understand how reactance voltage is developed in transformers, let's break down the key concepts:
Inductive Reactance: Transformers consist of coils of wire (windings) wound around a core. When an AC voltage is applied to the primary winding, it creates a changing magnetic field around the winding. This changing magnetic field induces a voltage in the secondary winding according to Faraday's law of electromagnetic induction. Additionally, the varying current in the primary winding creates a self-induced voltage due to the inductance of the winding itself. This self-induced voltage opposes any changes in current and is known as inductive reactance.
Phasor Diagram: To analyze the development of reactance voltage, phasor diagrams are often used. A phasor diagram is a graphical representation that helps visualize the relationships between voltage and current in AC circuits. In a transformer, the primary and secondary windings are represented by phasors that are 90 degrees out of phase due to the transformer's inductive nature.
Lagging Current: When an AC voltage is applied to the primary winding of a transformer, the resulting current lags the voltage due to the inductive nature of the winding. This lagging current creates a voltage drop across the inductive reactance, which is proportional to the rate of change of current with respect to time (di/dt). This voltage drop across the reactance contributes to the development of reactance voltage.
Reactance Voltage Magnitude: The magnitude of the reactance voltage depends on factors such as the inductance of the winding, the rate of change of current, and the frequency of the AC source. A higher frequency or a faster-changing current will lead to a larger reactance voltage.
In summary, reactance voltage develops in transformers due to the inductive reactance of the windings. When an AC voltage is applied, it induces a varying magnetic field and a corresponding voltage across the secondary winding. Simultaneously, the changing current in the primary winding generates a self-induced voltage due to the inductive reactance. This reactance voltage opposes changes in current and leads to a phase shift between voltage and current. Phasor diagrams are useful tools for understanding the relationships between these voltages and currents in AC circuits, including transformers.