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A straight wire segment of length L makes an angle

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The resolution of length vector of the wire segment is as shown in the figure. L cos θ The y-component of the magnetic force on the current carrying wire is, Id B sin 90° The varying magnetic field is,The y-component of the total magnetic force as follows: dFIdxB The limits for the above integration are 0 to L cos θ , because the x-component is L cos θ Then the y-component of the total magnetic force is, cos Id B Lcose 1B0L cos, θThen calculate the y-component of the total magnetic force as follows: 1B0L cos, θ (5.90 A (2.5T (2.44m (cos 46.0° 4.0214 The force component is along positive y-axis direction.

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