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A wire, carrying a current \( i \), is kept in the \( \mathrm{XY}- \) plane along the curve \( y=A \sin \left(\frac{2 \pi}{\lambda} x\right) \). A magnetic field \( B \) exists in the z-direction. The magnitude of the magnetic force on the portion of the wire between \( x=0 \) and \( x=\lambda \) is
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