Pre-lab EM-9 The magnetic field of a solenoid The magnetic field along the axis of a solenoid can be viewed as generated by many single current loops. The total field can be calculated by integrating the field generated by all of the single current loops. The axial component of the field as a function of distance x from the midpoint of a solenoid can be expressed as Honl B = L+2x L-2x (1) 2 D2 +(L+2x) D +(L-2x)) where L is the length, Dis the diameter of the solenoid, n is the number of turns per unit length on the solenoid, and7 is the current in the solenoid. At the midpoint of the solenoid, x 0, the magnetic field is Be = Honl- (2) VD2 +L2 If the solenoid is long and thin, L>>D, then B = He nl is true for most points inside the solenoid. If the solenoid is short, and L and D are comparable, then the magnetic field inside the solenoid would vary with position. B po nl is true only for the points at or near the center of the solenoid. Immediately outside the wall of the solenoid, the magnetic field is zero. The magnetic field at and near the openings of the solenoid varies with position. Given the diameter of the solenoid D 1.0 cm, length L-20 cm, n=4000 turn/m, and I=1.0 A, use Eq. (1) to calculate the magnetic field at the following positions: Be = D=1.0 cm, L= 20 cm D+(L+2x) (cm') D+(L-2x) (cm) x(cm) (L +2x) (cm) (L-.2x) (cm) B (mT) 7. 10 Sample calculation of B (x) for x= Scm
Pre-lab EM-9 The magnetic field of a solenoid The magnetic field along the axis of a solenoid can be viewed as generated by many single current loops. The total field can be calculated by integrating the field generated by all of the single current loops. The axial component of the field as a function of distance x from the midpoint of a solenoid can be expressed as Honl B = L+2x L-2x (1) 2 D2 +(L+2x) D +(L-2x)) where L is the length, Dis the diameter of the solenoid, n is the number of turns per unit length on the solenoid, and7 is the current in the solenoid. At the midpoint of the solenoid, x 0, the magnetic field is Be = Honl- (2) VD2 +L2 If the solenoid is long and thin, L>>D, then B = He nl is true for most points inside the solenoid. If the solenoid is short, and L and D are comparable, then the magnetic field inside the solenoid would vary with position. B po nl is true only for the points at or near the center of the solenoid. Immediately outside the wall of the solenoid, the magnetic field is zero. The magnetic field at and near the openings of the solenoid varies with position. Given the diameter of the solenoid D 1.0 cm, length L-20 cm, n=4000 turn/m, and I=1.0 A, use Eq. (1) to calculate the magnetic field at the following positions: Be = D=1.0 cm, L= 20 cm D+(L+2x) (cm') D+(L-2x) (cm) x(cm) (L +2x) (cm) (L-.2x) (cm) B (mT) 7. 10 Sample calculation of B (x) for x= Scm
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