The numerator is typically easy to compute. I.e. $p(x | \theta, \phi)$ is just a likelihood function multiplied by a prior.
The problem here is integration. For a lot of functions, integration is straightforward. For example, $\int_0^1 x^2 \mathrm{d}x = \frac{1}{3}$. However, in general, it's not easy to compute an integral in an analytic form (i.e. I can't "write down" the answer).
I think the issue here is that we can compute $p(x|\theta, \phi)$ for lots of values of $\theta, \phi$ but a computer is probably going to do this for us. Although it feels like computers are arbitrarily precise, they do only work to finite precision. Therefore, this integration is going to be a numerical integration and thus approximate. As the number of parameters gets large, the quality of this approximation can deteriorate a lot.
When we are working with density function we expect $$\int_{\Phi} \int_{\Theta} \frac{p(x | \theta, \phi)}{\int_{\Phi} \int_{\Theta} p(x | u, v) \mathrm{d}u\, \mathrm{d}v} \mathrm{d}\theta\, \mathrm{d}\phi = 1$$
If we numerically approximate the denominator $\hat{I} = \frac{1}{N}\sum_{i = 1}^N p(x | \theta_i, \phi_i) $ then the approximate posterior $$\hat{\pi}(\theta, \phi |x) = \frac{p(x|\theta, \phi)}{\hat{I}}$$ will not be a valid density function therefore not a valid posterior.
And as I said, if we have more than two parameters, $\hat{I}$ could be a very poor approximation, so the approximate posterior (which isn't even a valid posterior!) could an awful estimate. Therefore, any conclusions you make from your posterior will be meaningless.