Difference between revisions of "1962 IMO Problems/Problem 3"
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− | + | First we prove a small lemma: If the particles <math>X</math> and <math>Y</math> move along straight lines at constant velocities, then the locus of the midpoint of <math>XY</math> is also a line. This is rather trivial, since all lines in 3D space may take the parametric form <math>(at+n, bt+m, ct+p)</math>, with <math>t</math> being time, and the average of two such lines must also have a linear parametric form. | |
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+ | The locus clearly starts at the midpoint of <math>AB'</math>, or the center of face <math>ABB'A'</math>. As <math>X</math> moves from <math>A</math> to <math>B</math>, and <math>Y</math> moves from <math>C'</math> to <math>C</math>, both <math>X</math> and <math>Y</math> move along straight lines, so the midpoint of <math>XY</math> traces out a line segment, starting at the midpoint of <math>AB'</math> and ending at the midpoint of <math>BC'</math>, or the center of face <math>BCC'B'</math>. This concludes the first phase of motion. A quick check reveals that the locus goes nowhere during the second and fourth phases of motion, and only moves backward on the third. Thus the locus is just the segment connecting the centers of sides <math>ABB'A'</math> and <math>BCC'B'</math>. | ||
==See Also== | ==See Also== |
Revision as of 23:29, 17 January 2018
Problem
Consider the cube ( and are the upper and lower bases, respectively, and edges , , , are parallel). The point moves at constant speed along the perimeter of the square in the direction , and the point moves at the same rate along the perimeter of the square in the direction . Points and begin their motion at the same instant from the starting positions and , respectively. Determine and draw the locus of the midpoints of the segments .
Solution
First we prove a small lemma: If the particles and move along straight lines at constant velocities, then the locus of the midpoint of is also a line. This is rather trivial, since all lines in 3D space may take the parametric form , with being time, and the average of two such lines must also have a linear parametric form.
The locus clearly starts at the midpoint of , or the center of face . As moves from to , and moves from to , both and move along straight lines, so the midpoint of traces out a line segment, starting at the midpoint of and ending at the midpoint of , or the center of face . This concludes the first phase of motion. A quick check reveals that the locus goes nowhere during the second and fourth phases of motion, and only moves backward on the third. Thus the locus is just the segment connecting the centers of sides and .
See Also
1962 IMO (Problems) • Resources | ||
Preceded by Problem 2 |
1 • 2 • 3 • 4 • 5 • 6 | Followed by Problem 4 |
All IMO Problems and Solutions |