Magnetic field values are often determined by using a device known as a search coil . This technique depends on the measurement of the total charge passing through a coil in a time interval during which the magnetic flux linking the windings changes either because of the coil’s motion or because of a change in the value of B . (a) Show that as the flux through the coil changes from Φ 1 to Φ 2 , the charge transferred through the coil is given by Q = N (Φ 2 − Φ 1 )/ R , where R is the resistance of the coil and N is the number of turns. (b) As a specific example, calculate B when a total charge of 5.00 × 10 −4 C passes through a 100-turn coil of resistance 200 Ω and cross-sectional area 40.0 cm 2 as it is rotated in a uniform field from a position where the plane of the coil is perpendicular to the field to a position where it is parallel to the field.
Magnetic field values are often determined by using a device known as a search coil . This technique depends on the measurement of the total charge passing through a coil in a time interval during which the magnetic flux linking the windings changes either because of the coil’s motion or because of a change in the value of B . (a) Show that as the flux through the coil changes from Φ 1 to Φ 2 , the charge transferred through the coil is given by Q = N (Φ 2 − Φ 1 )/ R , where R is the resistance of the coil and N is the number of turns. (b) As a specific example, calculate B when a total charge of 5.00 × 10 −4 C passes through a 100-turn coil of resistance 200 Ω and cross-sectional area 40.0 cm 2 as it is rotated in a uniform field from a position where the plane of the coil is perpendicular to the field to a position where it is parallel to the field.
Solution Summary: The author explains that the charge transferred through the coil is Q, the resistance of the emf induced in the circuit, and the magnetic flux around the loop.
Magnetic field values are often determined by using a device known as a search coil. This technique depends on the measurement of the total charge passing through a coil in a time interval during which the magnetic flux linking the windings changes either because of the coil’s motion or because of a change in the value of B. (a) Show that as the flux through the coil changes from Φ1 to Φ2, the charge transferred through the coil is given by Q = N(Φ2 − Φ1)/R, where R is the resistance of the coil and N is the number of turns. (b) As a specific example, calculate B when a total charge of 5.00 × 10−4 C passes through a 100-turn coil of resistance 200 Ω and cross-sectional area 40.0 cm2 as it is rotated in a uniform field from a position where the plane of the coil is perpendicular to the field to a position where it is parallel to the field.
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