Depending on the four given constants we have a set of real roots and complex roots. It is a rotation of two vectors with different speeds with a constant matching y-projection.
However, the derivative can be solved in closed form by letting
$$ \cos T = \dfrac {\alpha_1 \beta_1 }{\sqrt{(\alpha_1 \beta_1)^2 + (\alpha_2 \beta_2)^2} } $$ etc. which can be integrated. (Sorry no, my error !)
EDIT1:
Amplitude and frequency modulation of signals are quite different this way.
Let
$$x(t)= \alpha_1\sin(\beta_1 t)+\alpha_2\sin(\beta_2 t)+1$$
Differentiating
$$x^{'}(t)= \alpha_1 \beta_1\cos(\beta_1 t)+\alpha_2 \beta_2\cos(\beta_2 t) $$
Letting
$$ \cos T = \dfrac {\alpha_1 \beta_1 }{\sqrt{(\alpha_1 \beta_1)^2 + (\alpha_2 \beta_2)^2} },\, \sin T = \dfrac {\alpha_2 \beta_2 }{\sqrt{(\alpha_1 \beta_1)^2 + (\alpha_2 \beta_2)^2} } $$
Then
$$x^{'}(t)= const \cdot [ \cos T \cos(\beta_1 t) + \sin T \cos(\beta_2 t) ] $$
which cannot be simplified due to three frequencies. Read under signal frequency modulation, you may still be lucky.
EDIT2:
Second order differentiation
$$ - x^{''}(t)= \alpha_1 {\beta_1}^2 \sin(\beta_1 t)+\alpha_2 {\beta_2}^2\sin(\beta_2 t) $$
letting each signal expressible in terms of derivatives.