Animated Solution for Mathematics - Vector Algebra: A1,A2,…,An are the vertices of a regular plane polygon with n sides and O is its centre. Show that ∑i=1n−1(OAi×OAi+1)=(1−n)(OA2×OA1).
Visualized Solution
Visualizing the Regular Polygon
Let us consider a regular polygon with n sides, centered at the origin O.
The vertices are labeled sequentially as A1,A2,…,An in a counter-clockwise direction.
This geometric setup forms the foundation of our vector analysis.
Equal Radial Distances
Since the polygon is regular, all vertices lie on a circumcircle of radius a.
Therefore, the magnitude of each position vector from the center O to any vertex Ai is constant.
We can write: ∣OAi∣=a for all i=1,2,…,n.
Symmetric Angular Spacing
The total angle around the center O is 2π radians.
By symmetry, the angle between any two consecutive radial vectors OAi and OAi+1 is equal.
This angle is given by: θ=n2π.
The Cross Product Definition
Recall the definition of the vector cross product of two vectors A and B:
A×B=∣A∣∣B∣sinθn^
Here, n^ is the unit vector perpendicular to the plane containing A and B.
Consecutive Vector Cross Product
Applying this definition to any consecutive pair of vectors OAi and OAi+1:
OAi×OAi+1=∣OAi∣∣OAi+1∣sinθn^
Substituting the values: OAi×OAi+1=a2sin(n2π)n^
Uniformity of the Terms
Notice that the magnitude a2sin(n2π) is constant for all i.
The direction n^ is also identical for all pairs since they all lie in the same plane.
Thus, every consecutive cross product term in our sum is identical!
Summing the First n−1 Terms
We are asked to find the sum: ∑i=1n−1(OAi×OAi+1)
Since there are exactly n−1 terms in this summation, and each term is identical:
∑i=1n−1(OAi×OAi+1)=(n−1)a2sin(n2π)n^
The Anti-Commutative Property
Recall the anti-commutative property of vector cross products:
A×B=−(B×A)
Applying this to our first two vectors: OA1×OA2=−(OA2×OA1)
Expressing the Base Term
We know that: OA1×OA2=a2sin(n2π)n^
Substituting the anti-commutative relation:
a2sin(n2π)n^=−(OA2×OA1)
Final Substitution & Q.E.D.
Now, substitute this back into our summation result:
Sum=(n−1)[−(OA2×OA1)]
Sum=−(n−1)(OA2×OA1)=(1−n)(OA2×OA1)
Hence Proved.
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The Sigma Insight: Vector (Cross) Product
Solution Diagram
The Symphony of Symmetry
Unlocking the Regular Polygon
Welcome, future engineer. Today, we are not just solving a vector problem; we are peeling back the layers of geometric perfection.
When you look at a regular polygon, do not just see a shape. See a system in perfect equilibrium where every vertex, every angle, and every radial vector is dancing to the same rhythm. This problem is a beautiful exercise in recognizing that rhythm.
Phase 1
The Geometry of the Fan
Imagine you are standing at the center O of a regular n-sided polygon. You look out at the vertices A1,A2,…,An.
Because the polygon is regular, it is inscribed in a circle of radius a. This is our first anchor point, where every radial vector OAi has the exact same magnitude: ∣OAi∣=a.
Now, think about the angular spacing. The total rotation around the center is 2π radians, which is divided perfectly into n equal slices.
Therefore, the angle θ between any two consecutive radial vectors, say OAi and OAi+1, is fixed at:
θ=n2π
This is the 'fan' of the polygon. Every slice of this fan is identical, and this uniformity is the secret weapon that will collapse our complex-looking summation into a simple algebraic expression.
Phase 2
The Cross Product as an Area Vector
Let us recall the definition of the vector cross product. For any two vectors A and B, the cross product is defined as A×B=∣A∣∣B∣sin(θ)n^.
Physically, the magnitude of this cross product represents twice the area of the triangle formed by the two vectors. In our case, for any consecutive pair OAi and OAi+1, the cross product is:
OAi×OAi+1=a2sin(n2π)n^
Here, n^ is the unit normal vector perpendicular to the plane of the polygon. Notice that the magnitude a2sin(n2π) depends only on the radius a and the number of sides n.
Since the entire polygon lies on a flat plane, the direction n^ is identical for every single pair. Every term in our summation is, quite literally, the same vector.
Phase 3
The Power of Uniformity
We are tasked with evaluating the sum ∑i=1n−1(OAi×OAi+1). Because we have established that each term is identical, we simply count the terms.
There are exactly n−1 terms in this sequence. Therefore, the sum becomes:
i=1∑n−1(OAi×OAi+1)=(n−1)a2sin(n2π)n^
This is the moment where many students stop, thinking they are done. However, we must match the target expression: (1−n)(OA2×OA1).
Phase 4
The Final Twist
This is where the anti-commutative property of the cross product saves the day. Remember that A×B=−(B×A).
We know that:
OA1×OA2=a2sin(n2π)n^
By the anti-commutative property, we can write:
a2sin(n2π)n^=−(OA2×OA1)
Now, substitute this back into our summation result. We replace the constant term with −(OA2×OA1):
Sum=(n−1)[−(OA2×OA1)]
Distributing the negative sign, we arrive at the final result:
Sum=−(n−1)(OA2×OA1)=(1−n)(OA2×OA1)
Conclusion
The Elegance of the Result
We started with a geometric shape, applied the symmetry of the polygon, utilized the definition of the cross product, and finished with a simple algebraic manipulation.
The result is not just a proof; it is a testament to the power of looking for patterns. When you face a JEE Advanced problem, do not rush to calculate. Pause, visualize the symmetry, and let the geometry guide your hand.