
The direction of the magnetic field is determined by the right-hand rule for the Lorentz force. The magnetic force \( \vec{F} \) on a charged particle is defined as: \[ \vec{F} = q \vec{V} \times \vec{B} \] where \( \vec{V} \) is the particle's velocity and \( \vec{B} \) is the magnetic field. This force is consistently perpendicular to both the velocity and the magnetic field.
At point P, the proton moves rightward (towards Q). For the magnetic force to be perpendicular to this velocity, if the deflection is upward, the magnetic field must be directed out of the paper (towards the observer).
At point Q, the proton's trajectory curvature, similar to P, implies the magnetic field is still directed out of the paper.
At point R, the proton moves downward. The resulting force on the proton indicates that the magnetic field is likely also directed out of the paper.
Concerning the magnetic field's magnitude, a more rapid change in the proton's velocity suggests a stronger magnetic field. Consequently, the magnetic field is inferred to be strongest at P, followed by Q, and weakest at R.
In summary, the magnetic field is directed out of the plane of the paper and exhibits its greatest strength at point P, decreasing at Q, and being weakest at R.
Three long straight wires carrying current are arranged mutually parallel as shown in the figure. The force experienced by \(15\) cm length of wire \(Q\) is ________. (\( \mu_0 = 4\pi \times 10^{-7}\,\text{T m A}^{-1} \)) 