Lets begin with the assumption that R=kv. What are the units
of the coefficient k in...
dv 6. The equation of motion now becomes mº mg - Kv. dt This equation is also separable because all the terms involving v can be brought to the left side of the dv equation: 1 = 1. dig-(K/m) As before, we integrate both sides of the equation with respect to t and use a change of variables. The resulting equation is s [dt . g-(K/m)v dy K dt, where a mg a-v2 к Evaluate the integrals on both sides of this equation and use the initial condition (O) = 0 to determine the arbitrary constant. Show that the velocity function is given in either of the two forms dy It's easiest to write the equation as I am not jdt, mg K mg (1-e K 1+