【答案】(1)1m;(2)0;(3)12J
【解析】
【详解】(1)对物块A,根据运动学公式可得
$$
x = h - \frac {1}{2} g t ^ {2} = 1. 2 \mathrm{m} - \frac {1}{2} \times 1 0 \times 0. 2 ^ {2} \mathrm{m} = 1 \mathrm{m}
$$
> ②设B物体从地面竖直上抛的初速度为 $\nu _ { \mathrm { B 0 } }$ ,根据运动学公式可知
$$
x = v _ {\mathrm{B0}} t - \frac {1}{2} g t ^ {2}
$$
即
$$
1 = v _ {\mathrm{B0}} \times 0. 2 - \frac {1}{2} \times 1 0 \times 0. 2 ^ {2}
$$
解得
$$
v _ {\mathrm{B0}} = 6 \mathrm{m/s}
$$
可得碰撞前A 物块的速度
$$
v _ {\mathrm{A}} = g t = 2 \mathrm{m/s}
$$
方向竖直向下;
碰撞前B物块的速度
$$
v _ {\mathrm{B}} = v _ {\mathrm{B0}} - g t = 4 \mathrm{m/s}
$$
方向竖直向上;
选向下为正方向,由动量守恒可得
$$
m _ {\mathrm{A}} v _ {\mathrm{A}} - m _ {\mathrm{B}} v _ {\mathrm{B}} = (m _ {\mathrm{A}} + m _ {\mathrm{B}}) v
$$
$$
\nu = 0
$$
(3)根据能量守恒可知碰撞损失的机械能
$$
\Delta E = \frac {1}{2} m _ {\mathrm{A}} v _ {\mathrm{A}} ^ {2} + \frac {1}{2} m _ {\mathrm{B}} v _ {\mathrm{B}} ^ {2} - \frac {1}{2} (m _ {\mathrm{A}} + m _ {\mathrm{B}}) v ^ {2} = 1 2 \mathrm{J}
$$