Analyzing the Geometry of the Staircase
Imagine you are standing at the origin of a coordinate plane, watching a tiny α-particle begin an extraordinary journey. It starts at the point (1,0), resting on the innermost circle C1.
This is a rhythmic, expanding dance. The particle travels along the circumference of C1, then jumps radially outward to C2, travels along C2, and jumps again to C3. It is a staircase of circles spiraling outward.
The Constant Rhythm
In circular motion, the relationship between arc length s, radius r, and the angle θ (in radians) is governed by the identity:
On the first circle C1, the radius is r=1 cm, and the particle travels an arc length of s=1 cm. Thus, the angle covered is θ1=11=1 radian.
Now, consider the k-th circle Ck. The radius is r=k cm, and the particle travels an arc length of s=k cm. The angle covered is:
This is the key insight: regardless of how large the circle becomes, the particle always sweeps out exactly 1 radian of angle before jumping to the next circle. The rhythm is constant and steady.
The Cumulative Journey
If the particle covers 1 radian on every circle, then after completing its motion on n−1 circles, the total angle Θ it has accumulated is the sum of these individual steps:
We are looking for the moment the particle crosses the positive x-axis for the first time. Since it starts at an angle of 0, it will cross the positive x-axis whenever its total angular displacement Θ reaches or exceeds 2π radians.
Given that 2π≈6.283 radians, we seek the smallest integer n such that the particle crosses the threshold during its traversal of circle Cn.
The Final Leap
As the particle enters circle Cn, its starting angle is (n−1) radians. By the time it finishes its motion on Cn, it will have reached an angle of n radians.
Therefore, the crossing occurs on circle Cn if the value 2π lies within the interval [n−1,n].
Let us test our integers:
For n=6, the interval is [5,6]. Since 6<6.283, the particle has not yet reached the positive x-axis.
For n=7, the interval is [6,7]. Because 6<6.283<7, the value 2π is trapped inside this interval.
This means that while the particle is traversing the 7th circle, it crosses the 2π threshold. It has completed its first full revolution and is crossing the positive x-axis for the first time.
The beauty of this problem lies in how a complex-sounding motion simplifies into a basic inequality. By focusing on the angular displacement, we find that the particle is simply a clock, ticking one radian at a time.
The final answer is n=7.