Правка раздела «Solution»

astrosander правка от
правка #12605 предыдущая #12563 ← раньше
@@ -47,7 +47,7 @@Solution
Considering $\sin\varphi\approx\tan\varphi$ and $h\gg l$, we obtain
$$
−\sqrt{l^2+h^2}\approx h\Rightarrow \boxed{l=h-\Delta x}\tag{2}
+\sqrt{l^2+h^2}\approx h\Rightarrow \boxed{l=h-\Delta x}\tag{3}
$$
$L_1,~L_2$ — Length of threads at the initial moment
@@ -73,7 +73,7 @@Solution
$$
$$
−v_1^2+v_2^2=2g\left(h-\Delta x\right)\tag{3}
+v_1^2+v_2^2=2g\left(h-\Delta x\right)\tag{4}
$$
By the Newton's second law for the $m$ weight
@@ -98,13 +98,13 @@Solution
\left|a\right|=\left|a^*\right|\Rightarrow v=v^*
$$
−Given that the system is being run from a stationary state $(v_0=v_0^*=0)$, let's substitute into $(3)$
+Given that the system is being run from a stationary state $(v_0=v_0^*=0)$, let's substitute into $(4)$
$$
2v^2=2g\left(h-\Delta x\right)
$$
−Taking into consideration $(2)$
+Taking into consideration $(3)$
$$
v^2=gl\Rightarrow \boxed{v=\sqrt{gl}}
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