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In general, in order to truncate the Taylor series at any given order, we must establish that all higher order terms are negligible.
Similarly, Δv is the area under the a(t) curve between two times, and
Δx is the area under the v(t) curve between two times.
Hence Δx/Δt is the average velocity, and
Δv/Δt is the average acceleration, between two times.
For constant acceleration, the average velocity is equal to the instantaneous velocity at the mid-point of the time interval over which the average is
taken.
Also, note that total distance travelled is not necessarily the same as total displacement! A graph of v vs. t should clarify the matter.
Given any four, we can always find the other two; the method of solution is determined by which four variables are given.
Since there are 15 ways to choose 4 things from a group of 6 (6! / (4! 2!)), there are 15 possible one-dimensional kinematic problems.
Kinematics
displacement is specified by differences of coordinates;
distance is specified by the Pythagorean Theorem (and is therefore always positive).
acceleration is the rate of change of velocity (measured in m/s2).
df/dt (the derivative of f with respect to t) is the infinitesimal change in f at the instant of time t.
f(x) = Σk=0∞ f (k) (x0) * (x - x0)k / k!,
where f (k) denotes the kth derivative of f. So
x(t) = x(0) + dx/dt (0) * t + d2x/d2t (0) * t2 / 2 +
d3x/d3t (0) * t3 / 6 + ...
If d2x/d2t does not depend on t (so dk > 2x/dkt = 0), we write
x(t) = x(0) + v(0) * t + a * t2 / 2,
which is the equation for uniformly accelerated motion.
dx(t)/dt = v(t) = v(0) + a * t
and
d2x(t)/dt2 = dv(t)/dt = a.
∫ a dt = a * t + c1
and
= v(t) with c1 = v(0),
∫ v(t) dt = v(0) * t + a * t2 / 2 + c2
= x(t) with c2 = x(0).
Note that for a collision to occur, the solution(s) to this equation must be real.
For two objects, we can usually set one of the initial positions to zero by defining it to be the origin.
There are therefore five equations and 10 unknowns, yielding 252 possible collision problems (10! / (5! 5!)).
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©2010, Kenneth R. Koehler. All Rights Reserved. This document may be freely reproduced provided that this copyright notice is included.
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