91影视

• The mass of the block $M=5\mathrm{kg}$.
• The force exerted on the block $F=12\mathrm{N}$.

Newton鈥檚 second law states that the force acting on the body can be calculated with the product of mass and acceleration of the body.

The net force is equal to the vector sum of all the forces acting on the body, which helps us to understand the equilibrium conditions.

Using the Force body diagram and Newton鈥檚 second law, we can find the magnitude of the acceleration of the block and the magnitude of the force and acceleration just before the block is lifted off the floor.

Formulae:

Newton鈥檚 second law is,

$F_{net}=\underset{}{鈭�}Ma$

The forces acting on the block are the weight of the block acting downward, the normal force from the floor on the block, and the force exerted by the cord. The free-body diagram can be used to understand the forces and their directions.

From FBD, we can write that,

$$\begin{gathered} F\cos 胃=Ma \\ a=\frac{\mathrm{贵肠辞蝉胃}}{\mathrm{M}} \\ =\frac{12\cos \left(25掳\right)}{5} \\ =2.18\mathrm{m}/{\mathrm{s}}^2 \end{gathered}$$

From FBD, we can write that,

$$\begin{gathered} F_N=Mg-F\sin 胃 \\ =5\mathrm{kg}\left(9.8\mathrm{m}/{\mathrm{s}}^2\right)-12\mathrm{Nsin}\left({25}^{掳}\right) \\ =43\mathrm{N} \end{gathered}$$

As $F_N$is positive, the bock is on the floor when it moves with acceleration, $2.18\mathrm{m}/{\mathrm{s}}^2$.

If the block is lifted off the floor, the normal force acting on it becomes zero. Therefore, we can write,

$$\begin{gathered} Mg=F\sin 胃 \\ F=\frac{Mg}{\sin 胃} \\ =\frac{5\mathrm{kg}\left(9.8\mathrm{m}/{\mathrm{s}}^2\right)}{\sin \left(25掳\right)} \\ =116\mathrm{N} \end{gathered}$$

Therefore, the force on the box is 116N.

As the box moves in the horizontal direction, the acceleration of the box is,

$$\begin{gathered} \mathrm{a}=\frac{\mathrm{贵肠辞蝉胃}}{\mathrm{M}} \\ =\frac{116\mathrm{N}.\cos \left(25掳\right)}{5\mathrm{kg}} \\ =21\mathrm{m}/{\mathrm{s}}^{} \end{gathered}$$

Therefore, the acceleration of the box is $21\mathrm{m}/{\mathrm{s}}^2$.