Updated 2.2.39, 2.3.45-46,2.6.37,2.6.41

astrosander правка от
правка #6384 предыдущая #6321 GitHub 1ee7785 ← раньше позже →
@@ -88,9 +88,10 @@
As $\Delta x$ must be positive, we keep only the plus solution
$$\Delta x = \frac{mg}{k}\left(1+\sqrt{1+\frac{2k\cdot(h-l)}{mg}}\right)$$
Since at the bottom point, there are no forces other than the support reaction force $N$ and spring elasticity force $k\Delta x$, and at the bottom position the acceleration is zero ($a=0$) and the forces are compensated, the condition of equilibrium on the vertical axis has the form
−$$F_y:~N=k\cdot \Delta x$$
+$$F_y=N$$
Whence we obtain the maximum force of pressure on the floor, which is equal to the force with which the support acts on the load, according to Newton's third law
−$$\boxed{F=mg\left(1+\sqrt{1+\frac{2k\cdot(h-l)}{mg}}\right)}$$
+$$F_y=k\cdot \Delta x\Rightarrow \boxed{N=mg\left(1+\sqrt{1+\frac{2k\cdot(h-l)}{mg}}\right)}$$
+Analysing the obtained expression, we obtain that $F\sim \sqrt{k}\to$ Therefore, the greater the spring stiffness $k$, the greater the support reaction force $N$
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<h4>Answer</h4>
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