Acceleration due to gravity and One Dimensional Motion Equations

Acceleration due to gravity

The Earth is a huge massive body. According to Newton law of gravitation, the force of attraction between the two bodies is directly proportional to the product of the masses and inversely proportional to the square of the distance of separation. Here the two masses involved are the mass of the body and the mass of the Earth. The distance between the bodies is generally radius of the Earth, as the body is on the surface of the earth or near to the surface of the earth. As the mass of the earth is comparatively very high when compared with the body, the gravitational force of attraction will be always towards the Centre of the Earth. This gravitational force provides acceleration to all the bodies on the Earth and the corresponding acceleration is called acceleration due to gravity. The numerical value of acceleration due to gravity on the Earth is 9.8 m/s Squire. It may vary slightly from place to place but in general it can be taken as a constant.

This acceleration on the surface of the earth is uniform and constant. Hence when the body is coming towards the Earth, because of acceleration due to gravity its velocity will be keep on increasing until it strikes the ground. If you throw the body against the acceleration due to gravity, into the sky, it’s velocity will be keep on decreasing and finally it stops at a certain height called maximum height. Time taken to reach that maximum height is called time of ascent and time taken to reach the ground from a certain height is called time of descent.

We have four different equations of the motion to express the translatory motion of a body. In all that equations where ever acceleration is there, we can substitute acceleration due to gravity and we can rewrite the corresponding equations of motion due to gravity. Here there are practically two possibilities. The body may be coming towards the Earth or the body may be going away from the Earth. The acceleration due to gravity on the bodies that are coming towards the earth is generally treated as positive and vice versa.

We can write the equations of motion and the corresponding values as shown below.


Using this equations we can find the time taken by the body to reach a particular height against the gravity and it is called time of ascent. If the body is falling from the same height to reach the ground to take the same time and that is called time of dissent. The sum of the time of ascent and time of dissent is called time of flight.

A body is said to be a freely falling body if it is falling from a certain height with zero initial velocity. In that case, using the equations of motion we can calculate the final velocity of the body after covering a certain height h.

It can be also proved that if your body is thrown up with the velocity from the ground, after reaching the maximum height it will come back to the ground with the same velocity but in the reverse direction.


In general we have ignored the impact of the air resistance while measuring the time of ascent and time of descent. If we consider the air resistance, then the time of ascent is going to be little bit different from time of dissent. The direction of the force due to the air resistance is always in opposition to the relative motion.

So the effective acceleration in this case is going to be more than acceleration due to  gravity and hence the time of ascent is less than that of the case when the air resistance is ignored. When we are ignoring air resistance we are imagining that the environment is vacuum for the calculation purpose. Though it is not practically vacuum the given equations will be approximately valid in almost all the real-time situations.

By taking their resistance into consideration if we try to calculate the time of dissent, being their resistances against the relative motion, it is in the upward direction but the gravity is in the downward direction. And hence the effective acceleration will be less and hence time of dissent will be more and more than the case of vacuum.

It can be also be noticed that time of decent is more than the time of recent when their resistances taken into consideration.


Problem and solution

Two balls are dropped from different heights. One ball is drop two seconds after the other but both the strikes the ground at the same time which is five seconds after the first ball. Find the heights from where these two balls dropped?

As the first stone is taking five seconds to reach the ground and the second stone is two seconds late, it shall be only taking three seconds to reach the ground. The corresponding equations for the heights of the bodies can be written basing on the equation of motion as shown below. Simply the difference between the heights of the two equations we can calculate it as shown below.


Problem and solution

A body balls freely from a height of 125 m. After two seconds gravity ceases to act. Find the time taken by it to reach the ground if acceleration due to gravity is considered as 10 metre per second Squire.

The body is a freely falling body means its initial velocity equal to 0. For the first two seconds acceleration due to gravity is acting and hence it falls due to the gravity and it covers a distance of 20 m. During this process the body will acquire some velocity and it can be calibrated using the equations of motion as shown below. It is found that its value equal to 20 meter per second. Being it is drop from 125 m and 20 m is covered in the first two seconds, it has to further cover a distance of 105 m per reach the ground.

As acceleration due to gravity is no more acting the velocity of the body will remain constant. Does the body will continue to move with the same velocity of 20 m/s for the remaining time. We can calculate the time taken to cover the 105  m is in the formula that the displacement equal to velocity multiplied by time. By adding this time of the two seconds with can get the total time of the journey.



Problem and solution

A parachutist drops freely from an aeroplane for 10 seconds before the parachute opens out. He’s velocity when he reach the ground is 8 m/s. Once if the parachute is open he has a standard retardation of two meter per second Squire. Find the height at which he gets out of the aeroplane.

Before the parachute opens he falls down due to the gravitational effect and he’s not having a initial velocity in the vertically downward direction. Hence we can find that is going to cover a distance of 490 m in the first 10 seconds. In this 10 seconds will also acquire some velocity due to acceleration due to gravity and it can be found that the velocity is 98 m/s.

He covers the further distance with the standard retardation of two meter per second Squire and we can calculate the distance that he covers with a initial velocity of 98 m/s and a final velocity of 8 m/s and with an acceleration of two meter per second Squire using the equation of motion. By substituting the value is we can get the total height as 2875 m.




Related Posts

Problems on Motion of a Body Along a Straight Line

A body moving along only one direction during its motion is said to be in one-dimensional motion. It is also the motion along a straight line when the air friction is neglected. To apply the laws of motion, we can consider a particle concept. Particle is a body of negligible dimensions. It is of point size and having negligible mass. In mechanics we generally derive all the laws and formulas for this particle. As the body is the combination of identical particles, the concepts that are generated for the particle can be applied to the body also at the broader level.

To study the motion of the body along one-dimension, we have four equations of motion. If the body is moving along the horizontal direction, it may have acceleration which is nothing but rate of change of velocity. If the body is moving along the vertical direction, it is moving against or in favor of the gravity. In that case acceleration of the body is called acceleration due to gravity and it is a constant value which is equal to 9.8 m/s Squire.

The relation among initial velocity, final velocity, acceleration, time of travel and the distance is discussed in the previous post and we are going to use the same relations to solve these problems.

Problem 

A bus accelerates from rest at constant a rate for some time, after which it starts de accelerates at another constant rate to come to the state of rest. If the total time allotted for the journey is given, calculate the maximum speed and the total distance traveled by the bus?

Solution:

Let us divide the total time of the travel into two parts and when we add these two parts where going to get the total time. To solve this problem we can draw a graph taking the time on x-axis and the velocity on y-axis. The graph starts from the origin and is a straight line until it reaches its maximum velocity during the positive acceleration period. After reaching the peak, as per the problem the particle starts negative acceleration and hence the graph also starts decreasing in the reverse way and finally reaches the x-axis as shown.

We know that the slope of the velocity and the time graph gives the acceleration. The first part of the slope is going to be a positive slope because it is an increasing slope and the second part of the graph is a negative slope because it is decreasing. Anyway we can consider the magnitude of the slope to solve the problem.

By identifying the slope and further by identifying the time taken for the journey, we can calculate the total time as shown below.

We also know that the area of velocity and time graph gives the displacement. By identifying the area of the diagram, we can also calculate the total displacement as shown in the attached diagram.



Alternate solution

We can solve the same problem without using the graphical concept. Here also let us assume that a body is accelerated for a specific time, reaches its maximum velocity, and then starts de accelerating and finally comes the state of rest after a specified time. The sum of these two specified times gives the total time of the journey and it is given in the problem.

By using the first equations of motion we can calculate the time of travel and by adding that two equations, we can get the total time as shown below. From the velocity maximum equation, we can calculate the acceleration as the effective value of both acceleration and de acceleration and by substituting the value in the second equation of motion, we can also get the total displacement as shown below.



Problem 

A body starts from rest and travel is a distance with a uniform acceleration. Then it moves further some distance with a uniform velocity and after covering the specified distance, starts de accelerating and comes to the state of rest after covering some different distance. We need to find out the ratio of average velocity to the maximum velocity?

Solution

We can again draw a graph taking the time and x-axis and the velocity on y-axis. Initially the graph starts from the origin and it is a straight line and reaches a point where the body acquires a maximum velocity. As this velocity is going to remain constant for the second part of the displacement, the graph is going to be a straight line parallel to the x-axis. 

After covering that specified second part of the distance, the body starts de accelerating, the graph also starts reversing itself to the x- axis as shown. Every time taking the concept that the area of velocity and the time graph is equal to displacement, we can get the equations for individual times of the three different parts of the problem.

We know that the average velocity is defined as the ratio of total displacement to the total time and by substituting the respective values we can calculate the ratio of average velocity to the maximum velocity as shown below.



Problem 

In the arrangement shown in the diagram, the ends of in extensible string moves in the downward direction with the uniform speed. The pullies in the given situation are fixed. Find the speed with which the mass moves in the upward direction?

Solution

By looking at the diagram, it can be understood that the length is a constant value and its differentiation with respect to time is going to give zero. This is the basic rule of the differentiation that differentiation of any constant is equal to 0. We can assume that the body is moving up with a certain displacement and correspondingly with a certain velocity. By identifying the relation between positions and by differentiating the positions equation once with respect to time we can get the velocities as shown below.



Problem 

The diagram shows a Rod of a specified length resting on a wall in the floor. Its lower end is pulled two words the left direction with a constant velocity. Find the velocity of the other end of rod moving in the downward direction, where the rod is making a specific and a known angle with the horizontal?

Solution 

The situation the problem is as shown in the diagram. We can again read the relation between lengths of the Rod, the distance of one end of the rod from the origin along the x-axis and the distance of the second end of the Rod from the origin along the y-axis.

As we are in need of velocity, differentiating the displacement equation is with respect to time, we can get them as shown below.