Two forces of equal magnitude \( F \) act at some angle \( \theta \) between them, and it is given that their resultant also has magnitude \( F \). Rather than deriving the angle algebraically, test each candidate angle directly using the resultant magnitude formula \( R = \sqrt{2F^2(1+\cos\theta)} \).
- Option \( 30^\circ \): Substituting, \( \cos(30^\circ) \approx 0.866 \), giving \( R = \sqrt{2F^2(1.866)} \approx 1.93F \), which is much larger than \( F \); this angle does not satisfy the condition.
- Option \( 60^\circ \): Substituting, \( \cos(60^\circ) = 0.5 \), giving \( R = \sqrt{2F^2(1.5)} = \sqrt{3}\,F \approx 1.73F \), still larger than \( F \); this does not satisfy the given equality either.
- Option \( 90^\circ \): Substituting, \( \cos(90^\circ) = 0 \), giving \( R = \sqrt{2F^2(1)} = \sqrt{2}\,F \approx 1.41F \), which is again larger than \( F \), so this angle also fails to match.
- Option \( 120^\circ \): Substituting, \( \cos(120^\circ) = -0.5 \), giving \( R = \sqrt{2F^2(1-0.5)} = \sqrt{2F^2(0.5)} = \sqrt{F^2} = F \); this exactly reproduces the given condition that the resultant equals either individual force in magnitude.
Only one of the four candidate angles, when substituted into the resultant formula, produces a resultant magnitude exactly equal to the magnitude of either original force.
So the correct answer is \( 120^\circ \).