The reactance is:
X L = 2 π f L X_L = 2\pi fL X L = 2 π f L where f f f is the frequency, and L = 40 m H = 0.04 H L = 40mH = 0.04H L = 40 m H = 0.04 H is the inductance of the inductor. Thus, for different frequencies obtain:
X L = 2 π ⋅ 0 ⋅ 0.04 = 0 Ω X L = 2 π ⋅ 60 ⋅ 0.04 ≈ 15.1 Ω X L = 2 π ⋅ 500 ⋅ 0.04 ≈ 125.7 Ω X_L =2\pi\cdot 0\cdot 0.04 = 0\Omega\\
X_L =2\pi\cdot 60\cdot 0.04 \approx 15.1\Omega\\
X_L =2\pi\cdot 500\cdot 0.04 \approx 125.7\Omega X L = 2 π ⋅ 0 ⋅ 0.04 = 0Ω X L = 2 π ⋅ 60 ⋅ 0.04 ≈ 15.1Ω X L = 2 π ⋅ 500 ⋅ 0.04 ≈ 125.7Ω The impedance is:
Z = R 2 + X L 2 Z = \sqrt{R^2 + X_L^2} Z = R 2 + X L 2 where R = 25 Ω R = 25\Omega R = 25Ω is the resistance of the inductor. Thus, for different X L X_L X L from the previous step obtain:
Z = 2 5 2 + 0 2 = 25 Ω Z = 2 5 2 + 15. 1 2 ≈ 29.2 Ω Z = 2 5 2 + 125. 7 2 ≈ 128.1 Ω Z = \sqrt{25^2 + 0^2} = 25\Omega\\
Z = \sqrt{25^2 + 15.1^2} \approx 29.2\Omega\\
Z = \sqrt{25^2 + 125.7^2} \approx 128.1\Omega Z = 2 5 2 + 0 2 = 25Ω Z = 2 5 2 + 15. 1 2 ≈ 29.2Ω Z = 2 5 2 + 125. 7 2 ≈ 128.1Ω
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