How fast does the observable Universe grow?
The observable Universe is $r = 46.3\,\mathrm{Glyr}$ (billion light-years) in radius, so by Hubble's law, galaxies at that distance recede from us at a speed
$$
v_\mathrm{rec} = H_0\,r = 9.6\times10^5\,\mathrm{km}\,\mathrm{s}^{-1},
$$
or $3.2$ times the speed of light, $c$.
At the same time, light from ever-increasing distances will have had the time to reach us. Since light travels at the speed of light, this adds another factor to the edge of the observable Universe. That is, its distance recedes at $v_\mathrm{rec}+c = 4.2c$.
Hence, today the radius of the observable Universe is
$$
\begin{array}{rcl}
dr & = & (v_\mathrm{rec} + c)\,dt\\
& \simeq & 4.2\,\mathrm{light\text{-}days}\\
& \simeq & 10^{11}\,\mathrm{km}\\
& \simeq & 730\,\mathrm{AU}
\end{array}
$$
bigger than it was yesterday ($dt=1\,\mathrm{day}$).
But remember that most of this growth does not mean that our observable Universe encompasses more galaxies; only that they're farther apart.
How far apart were two photons emitted, if they arrive one day apart?
In reality, we don't see photons from the Big Bang. The oldest photons we can detect are from the cosmic microwave background, but humans don't see those. But for the sake of the argument, consider two photons, both emitted right after cosmic inflation, but at slightly different distances from the place you will once stand.
Taking inflation to end when the Universe was $t\sim10^{-32}\,\mathrm{s}$ old, and the Universe has expanded by a factor of $a^{-1} \simeq 2.3\times10^{26}$ since then. Hence, what we today call the observable Universe was, at the end of inflation, only
$$
r_\mathrm{then} = ar\simeq10\,\mathrm{m}.
$$
That is, the photon you saw yesterday, was emitted 13.8 Gyr ago, only 10 meters from you.
To find the distance at which the photon you see today was emitted, we can calculate the fractional distance between the two regions emitting the photons — but now we shouldn't use physical coordinates, but instead comoving coordinates, because the part of the extra distance that is due to expansion shouldn't be taken into account. In comoving coordinates, the observable Universe increases a distance of $r_\mathrm{com} =$ one light-day per day, or a fraction
$dr_\mathrm{com}/r_\mathrm{com} = dr_\mathrm{com} / r = 6\times10^{-14}$.
In other words, the region emitting photon #2 is, and always has been, a fraction $6\times10^{-14}$ farther away than the region emitting photon #1.
If region 1 was 10 meters away, then region 2 was
$$
\begin{array}{rcl}
\frac{dr_\mathrm{com}}{r_\mathrm{com}}\times 10\,\mathrm{m} & \simeq & 6\times10^{-11}\,\mathrm{cm}\\
& \simeq & 0.6\,\mathrm{picometers}.
\end{array}
$$
(I originally forgot to calculate in coming coordinates, resulting in a slightly too large value.)
A note on the calculations
In the above calculations, I've used cosmological parameter data from Planck Collaboration et al. (2016), because those are implemented in Python's astropy module. The newer data from Planck Collaboration et al. (2018) would change the result only a little bit. If instead of $10^{-32}\,\mathrm{s}$ you assume $10^{-33}\,\mathrm{s}$ for the end of inflation, as some models predict, you'd get slightly smaller Universe at the end of inflation (a factor $\sqrt{10^{-32}/10^{-33}}\simeq3$).
