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प्रत्यावर्ती धारा की अति उच्च आवृत्ति पर संघारित्र एक शुद्ध चालक की भाँति व्यवहार करता है क्यों?

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धारितीय प्रतिघात XC\(\frac{1}{2\pi fc}\) से स्पष्ट है कि XC ∝ \(\frac{1}{f}\)

अत: अति उच्च आवृत्ति के लिए XC → 0

अतः संधारित्र शुद्ध चालक की भाँति व्यवहार करेगा।

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