November 6, 2022

Reasoning for distinct acceleration due to gravity on Polygons


REASONING FOR DISTINCT ACCLERATION DUE TO GRAVITY VALUES ON POLYGONS


INTRODUCTION

The gravitational field of Polygons viz. Pentagon, Hexagon, Heptagon and Octagon were determined in previous articles. One of the profound observations was, the magnitude of gravitational field at corner and mid-point were mathematically same for all the above mentioned four polygons. Although the equations for gravitational field at corner and mid-point were mathematically same, it is worthy to note that they do not yield same results for every polygon. The two predominant metrics defining the gravitational field of polygon are the side length of the polygon ‘a’ and its height ‘h’. This article aims at analyzing the equations to prove that the magnitude of gravitational field for all polygons will be distinct.

ASSUMPTIONS

1. All polygons considered are regular.
2. The thickness of the polygon is negligible compared to its length and width.
3. The polygon is not under the influence of an external gravitational field.
4. The polygon is homogeneous in nature.
5. All the mass of the polygon is assumed to be concentrated at the center.

CALCULATION

Consider a Polygonal plate of side length ‘a’ [m] and mass M [Kg]. The types of polygons considered are Pentagon, Hexagon, Heptagon and Octagon respectively. From the calculations of center of gravity of polygons, it is evident that every polygon can be divided equally into isosceles triangles with the exception of Hexagon which can be divided equally into equilateral triangles.
Figure .1

Consider one such isosceles triangle of side length ‘a’, height ‘h’ and slant length ‘b’ as depicted in figure .1. Assume all polygons considered have same side length ‘a’.

In ABC by simple trigonometry,
θ – Angle between side ‘b’ and side ‘a’

Angle ‘θ’ is also half of the interior angle of the polygon. Hence θ = ϕ/2 where ‘ϕ’ is the interior angle of the polygon. The interior angle of the polygon increases with the increase in the number of sides of the polygon. Hence a pentagon has smaller interior angle compared to an Octagon. From equation (2) height ‘h’ is directly proportional to side ‘a’ and tan (θ). As angle ‘θ’ increases, tan (θ) will also increase. This implies that height ‘h’ would change for every polygon despite the same side ‘a’ since each polygon has different interior angle. 

The magnitude of gravitational field at corner (Point A) and mid-point (Point B) are as follows:
The gravitational field magnitude only depends on side length ‘a’ and height ‘h’. Since it is proved that height ‘h’ cannot be the same for every polygon, it is clear that gravitational field magnitude for every polygon at both corner and mid-point will not be the same despite the same equation.

INSIGHTS

The two most important observations regarding the dependency of height ‘h’ on the gravitational field magnitude are as follows:
  •     For a given polygon of side length ‘a’, the height ‘h’ will always be different for every type of polygon.
  •     The height ‘h’ is proportional to tangent of the angle of the triangle. Hence ‘h’ will increase as the angle increases or in other words ‘h’ will be greater for multi sided polygons assuming constant length ‘a’ for every polygon.


September 24, 2022

Gravitational field lines of Hyperbola


GRAVITATIONAL FIELD LINES OF A HYPERBOLA


INTRODUCTION

The force of gravity as described by Sir Isaac Newton is a force of attraction. The gravitational force acting on a body of mass ‘m’ is equal to the product of its mass ‘m’ and the acceleration due to gravity acting on that body. Now Force is a vector quantity since it is a product of mass [scalar] and acceleration [vector]. By definition a scalar quantity can be represented by magnitude alone whereas a vector quantity must be represented by magnitude and direction. Thus while solving a vector quantity, it is important to obtain both magnitude and direction to obtain complete information of the vector. Acceleration due to gravity being a vector quantity has both magnitude and direction. The direction of gravitational force is termed as gravitational field lines or orthogonal trajectories which are always orthogonal [perpendicular] to the surface as explained in detail in the calculation section. This article intends to determine the gravitational field lines of a hyperbolic arc or a hyperbolic plate.

ASSUMPTIONS

1. The plate has negligible thickness hence is assumed to be two dimensional
2. The plate is homogeneous in nature meaning composed of only one material
3. The plate is not under the influence of an external gravitational field
4. The whole mass of the plate is assumed to be concentrated in the center

CALCULATION

Consider a hyperbola of major axis ‘a’ [m], minor axis ‘b’ [m] and mass ‘m’ [Kg].
Fig .1 A hyperbola
There is a 3 step procedure to determine the field lines

Step1 Determine differential equation of Hyperbola and its slope

The equation of a regular Hyperbola with major and minor axes ‘a’ and ‘b’ is,

Rearranging the above equation,


Differentiating equation (2) with respect to x, 

Equation (3) represents the slope of equation (1) [Hyperbola]. Thus an orthogonal trajectory to the Hyperbola must have a slope that is negative inverse of the slope in equation (3).

Step2 Determine the slope of the orthogonal trajectory

Thus the new slope or the slope of the orthogonal trajectory which is a negative inverse of equation (3) is

Step3 Determine equation of the orthogonal trajectory by integration

To obtain the equation of the orthogonal trajectory, integrate equation (4) by separating the variables. Rearranging equation (4)

{‘k’ is a constant of integration}

Equation (5) represents the family of orthogonal trajectories of a Hyperbola. The orthogonal trajectories which represent hyperbolas are pictorially represented in figure 2. It is interesting to note that both ellipse and hyperbola have the same orthogonal trajectory which is the hyperbola.

REPRESENTATION

The graph of a Hyperbola and its orthogonal trajectories are represented in Figure 2. The hyperbolas itself which are orthogonal trajectories to the hyperbola appear emanating outward and perpendicular to the parent hyperbola. Thus a hyperbola or a hyperbolic plate will have its gravitational field directed as hyperbolas.
Fig .2 Gravitational field lines of Hyperbola

EXPLANATION

Since Hyperbola is only symmetric about one axis x or y but not both, the gravitational field lines are not equidistant from the center and hence the magnitude of gravitational field is not the same at all points on the perimeter of Hyperbola. From figure 2, it is evident that the field lines are non-uniform since they are not parallel to each other. The non-uniformity stems from the curvature of the curve [Hyperbola]. The field lines in general represent the direction of the field.

CONCLUSION

The final equation (5) implies that the orthogonal trajectory of Hyperbola is family of hyperbolas. It is important to note that the constant ‘2k’ can have infinite values hence there are infinite orthogonal trajectories for a given shape in this case the Hyperbola.


April 15, 2022

Gravitational field lines of Parabola


GRAVITATIONAL FIELD LINES OF A PARABOLA


INTRODUCTION

The force of gravity as described by Sir Isaac Newton is a force of attraction. The gravitational force acting on a body of mass ‘m’ is equal to the product of its mass ‘m’ and the acceleration due to gravity acting on that body. Now Force is a vector quantity since it is a product of mass [scalar] and acceleration [vector]. By definition a scalar quantity can be represented by magnitude alone whereas a vector quantity must be represented by magnitude and direction. Thus while solving a vector quantity, it is important to obtain both magnitude and direction to obtain complete information of the vector. Acceleration due to gravity being a vector quantity has both magnitude and direction. The direction of gravitational force is termed as gravitational field lines or orthogonal trajectories which are always orthogonal [perpendicular] to the surface as explained in detail in the calculation section. This article intends to determine the gravitational field lines of a two dimensional parabolic plate.

ASSUMPTIONS

1. The plate has negligible thickness hence is assumed to be two dimensional
2. The plate is homogeneous in nature meaning composed of only one material
3. The plate is not under the influence of an external gravitational field
4. The whole mass of the plate is assumed to be concentrated in the center

CALCULATION

Consider a two dimensional parabolic plate of focal length ‘a’ [m] and mass ‘m’ [Kg].

Fig .1 A parabola

There is a 3 step procedure to determine the field lines

Step1 Determine differential equation of Parabola and its slope

The equation of a regular Parabola with focal length ‘a’ is,

Rearranging the above equation,


Differentiating equation (2) with respect to x, 

Equation (3) represents the slope of equation (1) [Parabola]. Thus an orthogonal trajectory to the Parabola must have a slope that is negative inverse of the slope in equation (3).

Step2 Determine the slope of the orthogonal trajectory

Thus the new slope or the slope of the orthogonal trajectory which is a negative inverse of equation (3) is


Step3 Determine equation of the orthogonal trajectory by integration

To obtain the equation of the orthogonal trajectory, integrate equation (4) by separating the variables. Rearranging equation (4)

{‘k’ is a constant of integration}


Equation (5) represents the family of orthogonal trajectories of a Parabola. The orthogonal trajectories which represent family of ellipses are pictorially represented in figure 2.

REPRESENTATION

The graph of a Parabola and its orthogonal trajectories are represented in Figure 2. The ellipses which are orthogonal trajectories to the Parabola appear emanating outward and complete the trajectory. Thus a parabolic plate will have its gravitational field directed as ellipses.

Fig .2 Gravitational field lines of Parabola

EXPLANATION

Since Parabola is only symmetric about one axis x or y but not both, the gravitational field lines are not equidistant from the center and hence the magnitude of gravitational field is not the same at all points on the perimeter of Parabola. From figure 2, it is evident that the field lines are non-uniform since they are not parallel to each other. The non-uniformity stems from the curvature of the curve [Parabola]. The field lines in general represent the direction of the field.

CONCLUSION

The final equation (5) implies that the orthogonal trajectory of a Parabola is family of ellipses. It is important to note that the constant ‘m’ can have infinite values hence there are infinite orthogonal trajectories for a given shape in this case the Parabola.


January 29, 2022

X and O Privacy Policy

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  4. Privacy Policy Changes
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  4. Privacy Policy Changes
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  4. Privacy Policy Changes
  5. Contact Information

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4. Privacy Policy Changes

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Effective Date: 03-12-2023

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Contents

  1. Collection of your information
  2. Storage of your information
  3. Disclosure of your information
  4. Privacy Policy Changes
  5. Contact Information

1. Collection of your information

The app does NOT collect any information from your device. The app does not require any permission to be granted in order to function.

2. Storage of your information

The app does NOT store any information on your device or on any remote server.

3. Disclosure of your information

The app does NOT disclose any information from your device to third parties.

4. Privacy Policy Changes

We may change this Privacy Policy from time to time in our sole discretion. We encourage visitors to frequently check this page for any changes to this Privacy Policy. Your continued use of the app after any change in this Privacy Policy will constitute your acceptance of such change.

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