Lets define the following probability density distributions as: $$ \begin{align} p(θ) &= N(θ; 0,1) \\ q(θ) &= N(θ; μ,σ^2)\\ p(y|θ,x) &= N(y; θx,σ_n^2) \end{align} $$ where $N(x; m,v)$ means $x$ is a univariate Gaussian random variable density distribution with mean $m$ and variance $v$.
Calculate variational free-energy $$ F(q(θ)) = \int dθ\, q(θ) \left[\log q(θ) - \log p(θ) - \log p(y|θ,x)\right] $$
According to Difference between Variance and 2nd moment, I cannot simplify $\int dθ\, q(θ)(θ - μ)^2$ to $σ^2$, because $μ$ is not $0$?
According to https://gregorygundersen.com/blog/2020/09/01/gaussian-entropy/, this is also the assumption when calculating the entropy: $$ H(θ) = - ∫ q(θ) \log q(θ) dθ = 0.5 \log(2πσ^2) + 0.5 $$ meaning I cannot do this either?
If this is the case, how do I calculate the original integral?
Can I simplify $\int dθ\, q(θ)θ^2$?
Edit1
About @Ricky's comment "how can a random variable follow two distributions", I think the intended meaning of the question is being an input of a function. The two random variables may be $P$ and $Q$, $P\sim N(0,1)$ and $Q\sim (μ,σ^2)$
Edit2
About @Joako's comment, I don't think () and $+^2⋅()$ are the same, because:
$$ q(θ) = \frac{1}{\sqrt{2\pi\sigma^2}} e^{\frac{-(\theta-\mu)^2}{2\sigma^2}}\\ $$
$$ p(θ) = \frac{1}{\sqrt{2\pi}} e^{\frac{-\theta^2}{2}}\\ $$
@JimB suggested $∫()^2 d=^2+^2$, why?
If I apply the integration by parts formula: $$ ∫u \cdot dv = uv - ∫v \cdot du\\ u = θ^2\\ dv = q(θ) dθ\\ du = 2θ dθ\\ v = ∫q(θ) dθ = 1 $$
so
$ ∫θ^2q(θ)dθ\\ =θ^2-∫2θ dθ\\ =θ^2-(θ^2+C)\\ =C $
?