Deriving Position & Motion Functions of Moving Particles

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Textbook authors derive position functions for moving particles from Newton's laws of motion, which are based on differential equations. The general equation for linear position incorporates initial displacement, velocity, and acceleration, with higher-order terms like "jerk" accounting for changes in acceleration. Variations in position functions arise from different initial conditions or scenarios, leading to different forms of equations. Some functions may appear arbitrary or simplified for educational purposes, not always reflecting real-world physics. Understanding these derivations helps clarify the relationship between calculus and motion in physics.
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Where do textbook authors get the formula for the position function or the function of a moving particle that are used as examples in solving derivatives? Here are examples:

s=t^3-6t^2-9t

f(t)=t^2-10t+12


I am interested on how to derive these kind of functions. How?
 
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What exactly are you asking? If you're talking about Newtonian physics, all the relations which describe the position of a particle are derived from Newton's law of motion, which is a differential equation.
 
I am interested to know how are those equations or functions were derived. Yes, these are equations in physics.

I wonder if they were made up by calculus textbook authors and were not based on Newtonian physics because sometimes the functions are not the same. For example:

Sometimes the position function is like this

s = 16t^2 - t

then in the next example it would look like this

s = 16t^3-t^2-t-12
 
I have never used LaTex before, so excuse me if this looks funny:

It depends on the situation. The general one dimensional equation for linear position is
x(t) = x0 + v0t + (1/2)a0t2 + (1/3)jt3

where x0 is the initial displacement, v0 is the initial velocity, and a0 is the initial acceleration. The cubed term represents the change in acceleration with respect to time and is called "jerk." For the reason why some terms are missing in your examples consider:
a particle that is initially at rest would have v0=0, a particle that starts at the origin would have x0=0 and so on.
 
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