Excel is an awkward language for this type of thing so we can make easier if we do a little math upfront. Doing complex math in Excel is just about as much fun as slamming your fingers in the car door, so we shall try to avoid it.
We have
$$H(z) = \frac{b_0 + b_1z^{-1}+ b_2z^{-2}}{a_0 + a_1z^{-1}+ a_2z^{-2}}= \frac{B(z)}{A(z)}$$
If we want to evaluate this at normalized frequency $z = e^{j\omega}$ we get
$$B(z) = b_0 + b_1\cos(\omega)+b_2\cos(2\omega)-j\left[b_1\sin(\omega)+b_2\sin(2\omega)\right] = B_r+jB_i$$
with
$$B_r = b_0 + b_1\cos(\omega)+b_2\cos(2\omega) \\
B_i = -b_1\sin(\omega)-b_2\sin(2\omega) $$
So the whole thing becomes
$$H(\omega) = \frac{B_r+jB_i}{A_r+jA_i}$$
With this we can calculate both magnitude and phase
$$|H(\omega)| = \sqrt{\frac{B_r^2+B_i^2}{A_r^2+A_i^2}} $$
$$\angle{H(\omega)} = \tan^{-1}\left(\frac{B_i}{B_r}\right)-\tan^{-1}\left(\frac{A_i}{A_r}\right)$$
We can implement this in excel by first calculating $B_r$, $B_i$, $A_r$, and $A_i$ and then using the last two formulas to calculate magnitude and phase. The phase can be done using the Excel function atan2()
which in typical Excel fashion uses non-standard conventions and reverses the argument order.
You can find an example with a second order Butterworth lowpass at https://docs.google.com/spreadsheets/d/1ye7-WzmwNRpTglJsGk6Dtvb8kge9PICc/edit?usp=sharing&ouid=110367350423053204811&rtpof=true&sd=true
EDIT based on comments
It's been rightfully pointed out that the subtraction of the two phases can run into numerical problems and wrapping problems.
A better way to calculate the phase is the following one
$$H(\omega) = \frac{B_r+jB_i}{A_r+jA_i} = \frac{B_r+jB_i}{A_r+jA_i} \cdot \frac{A_r-jA_i}{A_r-jA_i} = \cdot \frac{B_rA_r+B_iA_i+j(B_iA_r-B_rA_i)}{X}, x \in \mathbb{R}$$
So we can get the phase of a single biquad as
$$\angle{H(\omega)} = \text{atan2}(B_iA_r-B_rA_i, B_rA_r+B_iA_i) $$ where $\text{atan2}()$ is the quadrant correct version of the inverse tangent. The spreadsheet has an added column for the new phase calculation.