Question
Question: Two particles \(1\) and \(2\) move with constant velocities \({v_1}\) and \({v_2}\) . At the initial...
Two particles 1 and 2 move with constant velocities v1 and v2 . At the initial moment their radius vectors are equal to r1 and r2 . The relation between four vectors for the particles to collide is ∣r1−r2∣(r1−r2)=x∣v1−v2∣(v1−v2). Find x.
Solution
In order to solve this question we need to understand the rule of vector addition. First defining vectors, so vectors are scalar having a particular direction. So in order to add two vectors with direction we use a method known as triangle rule of vector addition and later to add more vectors we use polygonal law of vector addition. Triangle law of vector addition states that if we add two vectors such that they form two sides of a triangle then the third side represents a vector which is the sum of two vectors.
Complete step by step answer:
Let the first particle be at point A and second particle be at point B
Let the position vector of first particle be OA and it is equal to r1
And second position vector of second particle be OB and it is equal to r2
Let the first particle start moving towards second with speed v1 and second particle starts moving towards first with v2 .Let these particles collide with each other at C. Also let time “t” be taken to move each particle from their respective positions to C.Then from triangle law of vector addition in triangle ΔOAC we have OC=OA+AC.
That is OC=r1+v1t. Similarly in the triangle ΔOBC we have OC=OB+BC. That is OC=r2+v2t.
Equating both OC we get r1+v1t=r2+v2t.
(r1−r2)=t(v1−v2)
Since time is scalar so
t=∣v1−v2∣∣r1−r2∣
So putting value of t we get
∣r1−r2∣(r1−r2)=∣v1−v2∣(v1−v2)
Comparing with problem given we get x=1
Hence the correct answer is x=1.
Note: It should be remembered that here we do not concern with direction of final vector also here collision type not considered whether elastic or in-elastic collision. In elastic collision both momentum and energy is conserved but in in-elastic collision only momentum is conserved because energy is lost by mechanical force in performing work either for or against the motion.