Thus, the impedance in rectangular form is the sum of the resistive components for the real portion, plus the sum of the reactances for the imaginary (\(j\)) portion. By copying the \(X_L\) vector and...Thus, the impedance in rectangular form is the sum of the resistive components for the real portion, plus the sum of the reactances for the imaginary (\(j\)) portion. By copying the \(X_L\) vector and then shifting it down and next to \(X_C\), the difference between the two reactive components can be seen (purple component directly above the \(X_L\) copy).
Thus, the impedance in rectangular form is the sum of the resistive components for the real portion, plus the sum of the reactances for the imaginary (\(j\)) portion. By copying the \(X_L\) vector and...Thus, the impedance in rectangular form is the sum of the resistive components for the real portion, plus the sum of the reactances for the imaginary (\(j\)) portion. By copying the \(X_L\) vector and then shifting it down and next to \(X_C\), the difference between the two reactive components can be seen (purple component directly above the \(X_L\) copy).
