Projectile motion of tennis ball with air resistance

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Homework Help Overview

The discussion revolves around modeling the projectile motion of a tennis ball when served, specifically incorporating air resistance into the equations of motion. The original poster has developed differential equations for acceleration in two dimensions and seeks to determine the angle required for the ball to travel a specified distance.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster presents two differential equations related to the motion of the tennis ball and expresses uncertainty about the next steps in their analysis. They mention using trigonometric ratios to find initial velocities but are unclear on how to proceed with the equations.
  • Some participants discuss the correctness of the equations, particularly the sign of the drag term in the vertical motion equation, and suggest that drag should oppose the direction of movement.
  • There are inquiries about integrating the equations and how to implement the calculations in Excel, indicating a desire to understand the relationship between acceleration and position.
  • One participant notes the absence of a closed form solution for the equations presented.

Discussion Status

The discussion is ongoing, with participants providing guidance on the formulation of equations and potential methods for solving the problem. There is a recognition of the complexity involved, particularly regarding the integration of the equations and the effects of drag. Multiple interpretations of the equations and their implications are being explored.

Contextual Notes

Participants are working under the assumption that drag is proportional to the square of the speed, and there is some debate about the correct sign for the drag term in the equations. The original poster has defined variables such as mass and gravity, but there may be constraints related to the specific setup of the problem that are not fully articulated.

Shruf
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Hi, so I am trying to model the path of a tennis ball when serving. I already have the model without air resistance, but now I'm getting into differential equations with the air resistance. I obtained two differential equations for acceleration that i think are correct, but I'm not sure where to go from here exactly. It is in two dimensions. What I want to find is what angle the ball must be hit at to travel a set distance.


So far these are what i have:
equation 1: m\stackrel{d^{2}x}{dt^{2}} = -k \stackrel{dx}{dt} \sqrt{\stackrel{dx}{dt}^{2}+\stackrel{dy}{dt}^{2}}

equation 2: m\stackrel{d^{2}y}{dt^{2}} = k \stackrel{dy}{dt} \sqrt{\stackrel{dx}{dt}^{2}+\stackrel{dy}{dt}^{2}} - g

K is drag co-efficient, m is mass, g is gravity acceleration, all of which are defined.I have the initial velocity, and I know that I can use trig ratios to get the initial x and y velocities, but I have not idea what to do with them. BTW all the above below things are meant to be fractions, but i am not sure how to make them fractions, sorry.
 
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Shruf said:
Hi, so I am trying to model the path of a tennis ball when serving. I already have the model without air resistance, but now I'm getting into differential equations with the air resistance. I obtained two differential equations for acceleration that i think are correct, but I'm not sure where to go from here exactly. It is in two dimensions. What I want to find is what angle the ball must be hit at to travel a set distance.


So far these are what i have:
equation 1: m\stackrel{d^{2}x}{dt^{2}} = -k \stackrel{dx}{dt} \sqrt{\stackrel{dx}{dt}^{2}+\stackrel{dy}{dt}^{2}}

equation 2: m\stackrel{d^{2}y}{dt^{2}} = k \stackrel{dy}{dt} \sqrt{\stackrel{dx}{dt}^{2}+\stackrel{dy}{dt}^{2}} - g

K is drag co-efficient, m is mass, g is gravity acceleration, all of which are defined.I have the initial velocity, and I know that I can use trig ratios to get the initial x and y velocities, but I have not idea what to do with them. BTW all the above below things are meant to be fractions, but i am not sure how to make them fractions, sorry.

Assuming drag is proportional to the square of the speed (which is a fair approximation at high speeds) then your equations are basically right. You do have the sign wrong on the drag term in the y-equation. Drag will always oppose the direction of movement.
For the LaTex, put the m inside the LaTex, use \frac, not \stackrel, and wrap the dx/dt terms in braces so that the squaring applies to the whole term, not just the x or y:
m\frac{d^{2}x}{dt^{2}} = -k \frac{dx}{dt} \sqrt{{\frac{dx}{dt}}^{2}+{\frac{dy}{dt}}^{2}}
As to solutions, I believe there is no closed form solution.
 
haruspex said:
As to solutions, I believe there is no closed form solution.

Thank; I do know that there is no closed solution but I am wondering how to do the mass calculations on something like excel? I am not sure how to incorporate these two equations for acceleration in my position equation, or in my calculations for range. Also, I think my sign is correct since the ball is being hit downwards, which I've made negative. I think i have to integrate the equations, but I'm not sure in what way I need to use them yet.
 
Last edited:
Shruf said:
I think my sign is correct since the ball is being hit downwards, which I've made negative.
The contribution of drag to the acceleration must be a negative multiple of the speed.
 

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