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What is the relationship between impedance and admittance?

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Impedance and admittance are related concepts in electrical engineering, particularly in AC circuit analysis.

1. **Impedance (Z)**: Impedance is a measure of how much a circuit resists the flow of alternating current (AC). It combines both resistance (R) and reactance (X), and is generally represented as a complex number: \( Z = R + jX \), where \( j \) is the imaginary unit.

2. **Admittance (Y)**: Admittance is the reciprocal of impedance. It measures how easily a circuit allows AC to flow through it. Admittance is also a complex quantity and is given by: \( Y = \frac{1}{Z} \). In terms of its components, admittance can be written as \( Y = G + jB \), where \( G \) is the conductance (the real part) and \( B \) is the susceptance (the imaginary part).

The relationship between impedance and admittance is:

\[ Y = \frac{1}{Z} \]

and vice versa:

\[ Z = \frac{1}{Y} \]

So, if you know the impedance of a circuit, you can find the admittance by taking its reciprocal, and if you know the admittance, you can find the impedance similarly.
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Impedance and admittance are fundamental concepts in electrical engineering, particularly in the analysis of AC circuits. They are mathematical inverses of each other and are used to describe how circuits respond to alternating current (AC).

### Impedance

Impedance (\( Z \)) is a measure of how much a circuit resists the flow of AC. It combines both resistance (\( R \)) and reactance (\( X \)) into a single complex quantity. Impedance is expressed as:

\[ Z = R + jX \]

where:
- \( R \) is the real part representing resistance (measured in ohms, \( \Omega \)).
- \( X \) is the imaginary part representing reactance (measured in ohms, \( \Omega \)).
- \( j \) is the imaginary unit (\( j = \sqrt{-1} \)).

### Admittance

Admittance (\( Y \)) is the measure of how easily a circuit allows AC to pass through it. It is the reciprocal of impedance. Admittance is also a complex quantity and is expressed as:

\[ Y = \frac{1}{Z} = G + jB \]

where:
- \( G \) is the real part representing conductance (measured in siemens, \( S \)).
- \( B \) is the imaginary part representing susceptance (measured in siemens, \( S \)).

### Relationship Between Impedance and Admittance

The relationship between impedance and admittance is given by the following formulas:

1. **Inversion**: Admittance is the reciprocal of impedance:
   \[ Y = \frac{1}{Z} \]

2. **Polar Form**: If impedance is expressed in polar form as \( Z = |Z| \angle \theta \), where \( |Z| \) is the magnitude and \( \theta \) is the phase angle, then admittance is expressed as:
   \[ Y = \frac{1}{|Z| \angle \theta} = \frac{1}{|Z|} \angle (-\theta) \]
   The magnitude of admittance is the reciprocal of the magnitude of impedance, and the phase angle of admittance is the negative of the phase angle of impedance.

3. **Rectangular Form**: In rectangular form, if impedance is \( Z = R + jX \), then admittance can be calculated as:
   \[ Y = \frac{1}{R + jX} \]
   To find \( Y \), you multiply the numerator and denominator by the complex conjugate of the denominator:
   \[ Y = \frac{R - jX}{R^2 + X^2} \]
   Here, the real part \( G \) (conductance) is \( \frac{R}{R^2 + X^2} \), and the imaginary part \( B \) (susceptance) is \( -\frac{X}{R^2 + X^2} \).

In summary, impedance and admittance are interconnected through the reciprocal relationship, and both provide valuable insights into the behavior of AC circuits. Impedance describes how a circuit opposes AC, while admittance describes how readily the circuit allows AC to pass.
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