Jeff K. answered 06/17/20
Together, we build an iron base of understanding
Given: a = k – bv
=> dv/dt = k - bv since a = dv/dt by definition of acceleration1
1/(k - bv) dv = dt
∫1/(k - bv) dv = ∫ dt integrating both sides
(-1/b) ln (k - bv) = t + C for some constant, C . . . . . . . . . . . . . . eqn (1)
(-1/b) ln k = 0 + C plugging in the initial condition v0 = 0
C = (-1/b) ln k
(-1/b) ln (k - bv) = t - (1/b) ln k plugging C back into eqn (1)
ln (k - bv) = -b ( t - (1/b) ln k)
ln (k - bv) = -bt + ln k
k - bv = e-bt + ln k by the laws of logs
k - bv = e-bt . eln k
k - bv = ke-bt
bv = k - ke-bt
v = (k/b) (1 - e-bt)
This is the required v-t equation.
I leave you to draw the graph.