Define the jolt/jerk to be
$$J(f)={{d^3 f} \over {dt^3}}$$
Why don't we use the concept of jolt more often considering that the change in acceleration is most definitely an important characteristic in the universe. Is there some mathematical proof that essentially kicks jolt out of the useful units club? However, it seems like initial conditions relying on jerk/jolt should be the norm rather than the exception. I mean, the universe doesn't care about what's easy to measure...
In addition, what about the other neglected members of the rate of change community. Why isn't
$${{d^4 f} \over {dt^4}}$$
or
$${{d^{55} f} \over {dt^{55}}}$$
Used in physics? In fact wouldn't having a function that just gives all order derivatives of a function useful? You could presumably study the rate of change of the spread rates of change!
$$S(f(x),n)={{d^nx} \over {dt^n}}$$
In fact, on a more math intensive note, using fractional calculus, you could treat this Spread function as a real continuous function, since fractional calculus defines fractional order derivatives.
Of course, lets not leave out the integral. Shouldn't an expression that integrates the position with respect to time have physical meaning?
$$\int x \ dt$$
what about $$\iint x \ dt$$ or even $$\iiint x \ dt$$
In fact, it seems you could derive a function very similar to the one mentioned above.
Questions: So why don't we use these other forms of rate of change? In addition, isn't the integral of position important. I mean, it has units of $L \cdot M$ which seems to me at least to be very important. In addition, what about this Spread function, what physical significance does it have. In addition aren't initial conditions subject to the effects of jerk/jolt etc...!!