General Scientist said:
I am reading through a textbook on AP Physics, and I came across a few references to non-inertial frames of reference. It doesn't clearly say what a non-inertial frame of reference is. Based on the examples it gives, I assume that it is a frame of reference where the observer is experiencing acceleration.
Am I right?
How about we try to define a reference frame? I will not try to be rigrous here, but merely gather the things I think are necessary for this concept.
Nothwithstanding my previous digression (I agree it was a digression - my bad) to relativity, in Newtonian mechanics we can define a reference frame as an origin ##O## and a set of unit vectors, ##\hat{\vec{a}}, \hat{\vec{b}}, \hat{\vec{c}}##, such that any vector ##\vec{v}## in space can be written as a linear combination of this set ##\vec{v}=v_a\hat{\vec{a}}+v_b\hat{\vec{b}}+v_c\hat{\vec{c}}##.
Next we can define an "observer in the reference frame" as observer who's position is (relative to ##O##): ##\vec{u}=u_a\hat{\vec{a}}+u_b\hat{\vec{b}}+u_c\hat{\vec{c}}##, where ##u_{a,b,c}## are constant in time.
Now the difference between the intertial reference frame and a non-intertial one is simply that the basis vectors depend on time (t): ##\hat{\vec{a}}=\hat{\vec{a}}(t)## and same for others. More precisely, for a non-inertial reference frame the dependence of the basis vectors on time, should be at least quadratic (so that second derivative should not vanish).
We can now easily deduce that the observer in the non-intertial reference will be accelerating.
This all may seem quite trivial, but the TC complained about the lack of definition of the reference frame. I think my little sketch above contains sufficient flexibility to cover all exercises with non-inertial reference frames I have seen thusfar.
PS: Of course on must also allow for unit-vectors to depend on position to have the full generality of treatment.