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If a number of particles are projected from the same point in the same plane so as to describe enual parabolas, then the vertices of their paths lie on a : (a) parabola (b) circle (c) square (d) rectangle

Short Answer

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(b) circle

Step by step solution

01

Problem Understanding

We have multiple particles projected from the same point in the same plane, each following a parabolic path. We need to determine the geometric shape on which the vertices of these parabolas lie.
02

Identify the Shape for Vertex Collection

Realize that each particle follows a parabolic trajectory. The vertex of each projectile's parabola represents its maximum height. The loci of these vertices for a range of angles will form a particular shape.
03

Visualize the Parabolic Motion

Recall that the vertex of a parabola in projectile motion occurs when the object reaches its maximum height. Also, all these parabolas share the same focus (the point of projection) and have equal parabolas along different angles.
04

Conclusion About the Shape

The vertices of these parabolas create a circular shape, known as the "directrix circle" of the parabolic paths. This is due to the symmetry and equality in the maximum height achieved by each projectile at various angles, considering they have equal initial speed.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Parabolic Trajectory
When we talk about projectile motion, a key concept is the parabolic trajectory. This trajectory is the path that an object follows when it is launched into the air, subject to gravitational forces. For instance, when you throw a ball, it doesn't travel in a straight line. Instead, it follows a curved path which resembles a parabola.

This is mainly because the force of gravity acts downwards, causing the object to rise, slow down, and then fall back down, creating a symmetric arc. This trajectory is crucial in numerous fields, from sports to engineering, as it determines how an object will move through space after being launched.
  • The parabolic shape of the trajectory is fixed by the motion's initial velocity and angle of projection.
  • Gravity is the constant force acting downward throughout the motion, giving the trajectory its downward curve.
Understanding the basics of how objects move in a parabolic trajectory can help us predict and analyze their paths and determine their maximum reach (height and distance).
Vertex of Parabola
In any parabolic motion, the vertex of the parabola is of particular importance. This point signifies the maximum height achieved by the object during its flight path. In terms of projectile motion, the vertex is where the projectile reaches its peak before descending.

Determining the vertex helps in analyzing how high the projectile will travel and at what point along the horizontal axis it will achieve this height. Mathematically, for a parabola given by the equation \(y = ax^2 + bx + c\), the vertex can be found using the formula \(h = -\frac{b}{2a}\).
  • The vertex represents the balance point of the parabola where the upward and downward forces are equal.
  • For any projectile launched at a certain angle with a specific speed, the vertex is crucial for determining its maximum height.
This concept allows us to calculate precisely when and where the maximum height will occur for objects in motion.
Geometric Loci
The concept of geometric loci is pivotal in solving problems involving paths of projectiles or particles. A locus is essentially the set of points that satisfy a particular condition or conditions. In this problem, the geometric loci refers to the collection of points that the vertices of the parabolas create when particles are projected at different angles.

In our exercise, multiple particles are thrown from the same origin and travel along equal parabolas, but at different angles. The vertices of these parabolas collectively form a circle. This circle is referred to as the geometrical locus of those vertices.
  • The circle is not arbitrary; it's a mathematical consequence of the symmetry and constant speed of the particles.
  • This locus forms due to the identical maximum heights achieved by each projectile, caused by the constant initial speed.
Understanding geometric loci is important as it helps in visualizing the collective movement of individual paths and their intersections in space.

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Most popular questions from this chapter

A particle starts from rest with acceleration \(2 \mathrm{~m} / \mathrm{s}^{2}\). The acceleration of the particle decreases down to zero uniformly during time-interval of 4 second. The velocity of particle after 2 second is : (a) \(3 \mathrm{~m} / \mathrm{s}\) (b) \(4 \mathrm{~m} / \mathrm{s}\) (c) zero (d) \(8 \mathrm{~m} / \mathrm{s}\)

A heavy stone is thrown from a cliff of height \(h\) in a given direction. The speed with which it hits the ground (air resistance may be neglected): (a) must depend on the speed of projection (b) must be larger than the speed of projection (c) must be independent of the speed of projection (d) (a) and (b) both are correct

A ball is projected vertically upwards. If resistance due to air is ignored, then which of the following graphs represents the velocity-time graph of the ball during its flight?

Which of the following statements is correct? (a) When air resistance is negligible, the time of ascent is less than the time of descent (b) When air resistance is not negligible, time of ascent is less than the time of descent (c) When air resistance is not negligible, the time ascent is greater than the time of descent (d) When air resistance is not negligible, the time of ascent is lesser than the time of descent

Three particles of equal masses are located at the vertices of an equilateral triangle whose side equals \(a\). They all strart moving simultaneously with constant speed \(v\) with the first point heading continuously for second, the second for third and third for first. Then: (a) the distance travelled by each particle is \(2 a / 3\) (b) at every instant before collision the momentum of the system is zero (c) the force on each particle is perpendicular to velocity of the particle at any instant before collision (d) all the above

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