In this class, we discuss about the reason why inductive reactance gets multiplied with 'j' in phasor domain. Similarly, we also discuss about the reason behind the multiplication of capacitive reactance with '-j' in phasor domain.
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L12: Other Theorems: Millman's, Compensation, Tellegen's and Reciprocity
L11: Superposition Theorem (AC and DC Circuits)
L10: Maximum Power Transfer Theorem (AC and DC Circuits)
L9: Norton's Theorem (DC and AC Circuits)
L8: Thevenin's for AC Circuits
L7: Thevenin's Theorem (DC Circuits)
Tutorial Sheet 1: Solution
L6: Inductor and Capacitor in Phasor Domain
L5: Intro to Phasor Domain in AC Circuits
L4: Practice Questions on KCL and KVL
L3: KCL and KVL
L2: Types of Sources
L1: Introduction
Inverters: Full Bridge Inverter and its Advantages
INVERTERS: Harmonic Profile of Square Waveform and Concept of Filters
INVERTERS: Introduction, Half-bridge Inverter
ME Class: Axes Transformation
Transformers: EMF Equation and OC/SC Tests
Transformers: PHASOR DIAGRAM
Transformers: Development of equivalent circuit
Transformers: Non-idealities
3-Phase AC Circuits: TWO WATTMETER METHOD
3-Phase AC Circuits: Relationships with line and phase quantities in star and delta circuits
Three-phase AC circuits: Introduction