Analyzing the Setup
We are given three fixed points on the Cartesian plane: P(1,0), Q(−1,0), and R(2,0). These points are collinear, lying entirely on the x-axis.
Let the moving point
S be represented by the coordinates
(x,y). The motion of
S is governed by the geometric constraint:
SQ2+SR2=2SP2
The Algebraic Translation
To translate this geometric condition into an algebraic equation, we utilize the distance formula. The squared distance between two points (x1,y1) and (x2,y2) is given by (x2−x1)2+(y2−y1)2.
Applying this to our specific points, we define the squared distances as follows:
1. SQ2=(x+1)2+y2
2. SR2=(x−2)2+y2
3. SP2=(x−1)2+y2
Substituting these expressions into our governing equation, we obtain:
(x+1)2+y2+(x−2)2+y2=2[(x−1)2+y2]
The Great Cancellation
Next, we expand both sides of the equation to simplify the expression.
Expanding the Left-Hand Side (LHS):
(x2+2x+1)+y2+(x2−4x+4)+y2=2x2−2x+5+2y2
Expanding the Right-Hand Side (RHS):
2[(x2−2x+1)+y2]=2x2−4x+2+2y2
Equating the two sides, we have:
2x2−2x+5+2y2=2x2−4x+2+2y2
Notice that the terms 2x2 and 2y2 appear on both sides of the equation. By subtracting 2x2+2y2 from both sides, the quadratic components vanish entirely.
Final Calculation
We are left with a simple linear equation:
−2x+5=−4x+2
Rearranging the terms to solve for
x:
4x−2x=2−5
2x=−3
x=−23
The locus of the point S is the vertical straight line defined by the equation x=−1.5. This line is parallel to the y-axis and represents all possible positions the dancer can occupy while satisfying the given condition.