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Problem
The change in the magnetic dipole moment associated with the orbit, at the end of the time interval of the magnetic field change is a.
−
γ
B
Q
R
2
-\gamma BQR^2
−
γ
B
Q
R
2
b.
−
γ
B
Q
R
2
2
-\gamma \frac{BQR^2}{2}
−
γ
2
B
Q
R
2
c.
γ
B
Q
R
2
2
\gamma \frac{BQR^2}{2}
γ
2
B
Q
R
2
d.
γ
B
Q
R
2
\gamma BQR^2
γ
B
Q
R
2
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