A rotating-coil generator has peak emf E0=NBAωE0=NBAω. If only angular speed ωω is tripled (N, B, A unchanged), peak emf
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Chapter 13: Electromagnetic Induction and Alternating Currents (Set-4)
A circular loop is rotated in a uniform magnetic field; magnetic flux through the loop varies as A Constant only
Continue readingChapter 13: Electromagnetic Induction and Alternating Currents (Set-3)
A rectangular coil enters a uniform magnetic field region with constant speed; induced emf depends mainly on A Coil resistance
Continue readingChapter 13: Electromagnetic Induction and Alternating Currents (Set-2)
When coil turns faster in a uniform field, the induced emf amplitude mainly A Decreases always B Becomes zero C
Continue readingChapter 13: Electromagnetic Induction and Alternating Currents (Set-1)
In electromagnetic induction, induced emf appears mainly due to change in which quantity A Magnetic flux B Electric potential C
Continue readingChapter 12: Magnetism and Magnetic Effects of Current (Set-5)
A long straight wire carries current I. At a point P, distance from wire becomes half and current becomes half.
Continue readingChapter 12: Magnetism and Magnetic Effects of Current (Set-4)
For a circular loop (radius R, current I), magnetic field on axis at distance x is A μ0I/2xμ0I/2x B μ0I/2πxμ0I/2πx
Continue readingChapter 12: Magnetism and Magnetic Effects of Current (Set-3)
When observation point lies on extension of current element direction, Biot–Savart law gives field contribution as A Zero value B
Continue readingChapter 12: Magnetism and Magnetic Effects of Current (Set-2)
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Continue readingChapter 12: Magnetism and Magnetic Effects of Current (Set-1)
In Biot–Savart law, magnetic field contribution mainly depends on A Current element direction B Total charge only C Square of
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