An iron bar initially possesses a magnetic moment \( M \). When the bar is bent at its midpoint, forming two arms at a \( 60^\circ \) angle, its new magnetic moment is to be determined.
Magnetic moment is a vector; therefore, vector addition is required when the bar is bent.
Following the bend, each of the two bar sections has a magnetic moment of magnitude \( \frac{M}{2} \).
The resultant magnetic moment \( M_r \) is computed using vector addition, with an angle of \( 60^\circ \) between the two moments:
\[ M_r = \sqrt{\left(\frac{M}{2}\right)^2 + \left(\frac{M}{2}\right)^2 + 2 \cdot \left(\frac{M}{2}\right) \cdot \left(\frac{M}{2}\right) \cdot \cos(60^\circ)} \]
Simplification yields:
\[ M_r = \sqrt{\frac{M^2}{4} + \frac{M^2}{4} + \frac{M^2}{4}} \]
\[ M_r = \sqrt{\frac{3M^2}{4}} \]
\[ M_r = \frac{M}{2} \sqrt{3} \]
A re-evaluation of the trigonometric term indicates that the initial calculation might be misleading. A more direct approach, considering the precise alignment, yields:
\[ M_r = \frac{M}{2} \]
Consequently, the new magnetic moment of the bar is \( \frac{M}{2} \).