I'm trying to use the mechanical impedance analogy to describe a spring mass damper system as an electrical circuit.
Mechanical Impedances for linear motion are
$$ Z_{lin}(s) = \frac{F(s)}{\dot X(s)} = Ms + B + \frac{K}{s} $$
where M has units of kg, B has units of N-s/m and K has units N/m. The units of mechanical impedance then are N-s/m.
When I translate this to the rotational domain, I start having problems.
Rotational impedance will again be the ratio of an effort (torque) to a flow (rotational velocity).
Similarly, we have
$$ Z_{rot}(s) = \frac{\tau(s)}{\omega(s)} = Js + B_{rot} + \frac{K_{rot}}{s} $$
Based on dividing torque by angular velocity, the units of rotational impedance are [N-m-s/rad], or $\frac{ML^2}{T}$. When I try to verify that the units of rotational impedance are consistent, I get
$$J\cdot s = \frac{kg\cdot m^2\cdot rad}{s} = N\cdot m\cdot s \cdot rad = \frac{ML^2}{T}$$
$$B = N\cdot m\cdot\frac{s}{rad} =\frac{ML^2}{T} $$ and $$\frac{K}{s} = \frac{N\cdot m\cdot s}{rad^2}=\frac{ML^2}{T}$$
I can't sleep with all those radians being all over the place! It seems awfully inconsistent to have them in different place and I haven't been able to find any sources on the web or in my textbooks that adequately deal with this since mechanical impedance is such a niche topic. In doing this, I've assumed that the $s$ has units of [rad/s], which some people dislike and just use $s= \frac{1}{T}$ Is there a way for me to make this a little more consistent, possibly by using radians in the units for rotational inertia and the spring constant?
I've also looked at the discussions here: