Without loss of generality, and simplicity of calculations, assume $E[X]=\mu=0$. Subtracting a constant from a random variable does not change its variance. Define Y to be the truncated random variable:
$$f_y(y)= b f_x(y)$$ for $y<a$ and zero otherwise, where $b^{-1}=\int_{-\infty}^a f_x(x)dx\le1$. Then,
$$E[Y^2] = \int_{-\infty}^a y^2 b f_x(y)\, dy = b\left(E[X^2]-\int_a^{\infty} y^2 f_x(y)\, dy\right)$$
$$E[Y] = \int_{-\infty}^a y b f_x(y)\, dy = b\left(E[X]-\int_a^{\infty} y f_x(y)\, dy\right)= -b\int_a^{\infty} y f_x(y)\, dy$$
so,
$$V[Y]=E[Y^2]-E[Y]^2=bV[X] - b\int_a^{\infty} y^2 f_x(y)\, dy -b^2\left(\int_a^{\infty} y f_x(y)\, dy\right)^2$$
Define Z to be the random variable:
$$f_z(z)= c f_x(z)$$ for $z>a$ and zero otherwise, where $c^{-1}=\int_a^{\infty} f_x(x)dx = 1-b^{-1}$.
$$V[Y]=bV[X] - {b\over c}E[Z^2] -\left({b\over c}E[Z]\right)^2=bV[X] - (b-1)E[Z^2] -\left((b-1)E[Z]\right)^2$$
$$V[Y]=bV[X] - (b-1)V[Z] -b(b-1)E[Z]^2$$
$$\Delta=V[Y]-V[X]=(b-1)\left(V[X]-V[Z]-bE[Z]^2\right)$$
If $b=1$, then $V[Y]=V[X]$, otherwise $b>1$ in which case, $V[Y] \le V[X]$ iff:
$$V[Z]+bE[Z]^2 \ge V[X]$$
where $Z$ is the random variable with a distribution corresponding to the removed part of $X$ for the case $\mu=0$. For the general case, the condition is:
$$V[Z]+bE[Z-\mu]^2 \ge V[X]$$