平抛运动性质¶ 基础¶ Δv=gt\Delta v = gtΔv=gt 水平: {vx=v0x=v0t\left\{ \begin{aligned} v_x &= v_0 \\ x &= v_0 t \end{aligned} \right.{vxx=v0=v0t 竖直: {vy=gty=12gt2\left\{ \begin{aligned} v_y &= gt \\ y &= \frac{1}{2} g t^2 \\ \end{aligned} \right.⎩⎨⎧vyy=gt=21gt2 合成: {v=vx2+vy2x=x2+y2\left\{ \begin{aligned} v &= \sqrt{v_x^2 + v_y^2} \\ x &= \sqrt{x^2 + y^2} \\ \end{aligned} \right.⎩⎨⎧vx=vx2+vy2=x2+y2 推论¶ ∵{tanθ=vyvx=2yAxAtanα=yAxA\because \left\{ \begin{aligned} \tan{\theta} &= \dfrac{v_y}{v_x} = \dfrac{2y_A}{x_A} \\ \tan{\alpha} &= \dfrac{y_A}{x_A} \end{aligned} \right.∵⎩⎨⎧tanθtanα=vxvy=xA2yA=xAyA ∴tanθ=2tanα\therefore \tan{\theta} = 2 \tan{\alpha}∴tanθ=2tanα tanθ=2tanα\tan{\theta} = 2 \tan{\alpha}tanθ=2tanα xb=12xax_b = \frac{1}{2} x_axb=21xa Comments