I like @thegreatmu's answer, but I think we can get closer to the original
problem.
During the day, the concentration decays according to
$$
\frac{\partial C}{\partial t} = - \frac{\log(2)}{t_{1/2}} C
$$
pretty much like @thegreatmu's equation, but without the term $D$, because
during the day, no medicine is added.
At a fixed point during every day, say at breakfast, the medicine is ingested,
and the concentration instantly increases by the dose $D$. At such moments,
whe have both the low concentration $C_-$ and the high concentration $C_+ = C_- + D$.
Let us measure time in days (the half-time is 1.25 days), and let us take breakfast-time to be the moments $t=0$, $t=1$, $t=2$, etcetera.
The concentration at any time $n-1\leq t < n$ in the $n$-th day is given by
$$
C(t) = \exp\left(- \frac{\log(2) }{t_{1/2}} (t-n+1)\right) C_+(n),
$$
so just before taking the medicine again, we have the low concentration
$$
C_-(n+1) = \exp\left(- \frac{\log(2) }{t_{1/2}} \right) C_+(n).
$$
and the high concentration is given by
$$
C_+(n+1) = D + \exp\left(- \frac{\log(2) }{t_{1/2}} \right) C_+(n).
$$
From here it is pssible to calculate the high concentration for any day $n$:
\begin{eqnarray}
C_+(0) = D &,&
C_+(1) = D\left(1 + \exp\left(- \frac{\log(2) }{t_{1/2}} \right)\right), \cdots
\nonumber
\end{eqnarray}
leading to
\begin{eqnarray}
C_+(n) &=& D\sum_{j=0}^{n} \exp\left(- \frac{\log(2) }{t_{1/2}} \right)^j
=
D\frac{1-\exp\left(- \frac{\log(2) }{t_{1/2}} \right)^{n+1}}
{1-\exp\left(- \frac{\log(2) }{t_{1/2}} \right)}
\nonumber
\end{eqnarray}
and at $n-1\leq t < n$, any moment in the $n$-th day, the concentration is given by
\begin{eqnarray}
C(t) &=&
D\frac{1-\exp\left(- \frac{\log(2) }{t_{1/2}} \right)^{n}}
{1-\exp\left(- \frac{\log(2) }{t_{1/2}} \right)}
\exp\left(- \frac{\log(2) }{t_{1/2}} (t-n+1)\right)
\nonumber
\end{eqnarray}
we can compare the current concentration $C(t)$ to the concentration
$C(t+m)$, the same time of day, but $m$ days later:
\begin{eqnarray}
C(t) =
\frac{1-\exp\left(- \frac{\log(2) }{t_{1/2}} \right)^{n}}
{1-\exp\left(- \frac{\log(2) }{t_{1/2}} \right)^{n+m}} C(t+m)
=
\left(1-\exp\left(- \frac{\log(2) }{t_{1/2}} \right)^{n}\right)C(t+\infty),
\nonumber
\end{eqnarray}
where $C(t+\infty)$ means 'at this time of day, in steady state'.
Therefore, we can say that the concentration is in steady state when
\begin{eqnarray}
\exp\left(- \frac{\log(2) }{t_{1/2}} \right)^{n} < \epsilon,
\nonumber
\end{eqnarray}
where $\epsilon$ is small, for instance $\epsilon = 0.01$ when
you consider 'in steady state' to mean 'less that one percent away from steady state'. This will be after $n$ days, where $n$ is given by
\begin{eqnarray}
n > {}^2\log(1/\epsilon)~t_{1/2}.
\nonumber
\end{eqnarray}
In the case where the half-time is $1.25$ days, and $\epsilon=0.01$, we get
$n > 8.3$: just over a week. After 7 days, steady stage is approached up to
2%.