Imagine you are observing a high-energy physics experiment. We have two distinct ions, both possessing the exact same mass, but they differ in their electrical charges and the speeds at which they are traveling. They are both shot perpendicularly into a region containing a uniform magnetic field.
Our goal is to determine the ratio of the radii of the circular paths they will trace out. The problem provides us with three crucial pieces of information: their masses are equal (m1=m2=m), the ratio of their charges is q2q1=21, and the ratio of their speeds is v2v1=32.
The Master Equation
When a charged particle enters a magnetic field perpendicularly, the magnetic force acts as a centripetal force, causing the particle to move in a perfect circle. The radius r of this circular path is governed by a fundamental equation in electromagnetism:
r=qBmv
Here, m is the mass, v is the velocity, q is the charge, and B is the magnetic field strength. This equation tells us that the radius is directly proportional to the particle's momentum (mv) and inversely proportional to its charge and the magnetic field strength.
Setting up the Ratio
Since we need to find the ratio of the radii for the two ions, we can set up an equation by dividing the radius of the first ion by the radius of the second ion:
r2r1=q2Bm2v2q1Bm1v1
Because both ions are moving through the exact same uniform magnetic field, the value of B is identical for both. This allows us to elegantly cancel out B from our equation, simplifying it to:
r2r1=(m2m1)×(v2v1)×(q1q2)
Final Calculation
Now, we simply substitute the given ratios into our simplified equation. We know the masses are equal, so m2m1=1. The ratio of their speeds is given as v2v1=32.
Watch out for the trap here! The formula requires the ratio q1q2, but the problem gives us q2q1=21. Therefore, we must invert it: q1q2=12.
Substituting these values yields:
r2r1=(1)×(32)×(12)
Multiplying these fractions together, we get:
r2r1=34
Thus, the ratio of the radii of their circular trajectories is 4:3.