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+ <meta name="description" content="The moment of inertia of a solid body of mass m relative to the O-axis is equal to J. The center of mass of the body is located at a distance R from this axis. Find the force acting on the axis when a force F is briefly applied to a solid body perpendicular to the segment of length x that connects the point of application of the force and the axis. At which x is the smallest force acting on the axis?">
+ <meta name="author" content="Aliaksandr Melnichenka">
+ <meta name="date" content="2023-10" scheme="YYYY-MM">
+ <meta property="og:title" content="The moment of inertia of a solid body of mass m relative to the O-axis is equal to J. The center of mass of the body is located at a distance R from this axis. Find the force acting on the axis when a force F is briefly applied to a solid body perpendicular to the segment of length x that connects the point of application of the force and the axis. At which x is the smallest force acting on the axis?">
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+ <h3 id="back-link"><a href="../../#2.7">$\leftarrow$Back</a></h3>
+
+ <h3> Statement </h3>
+ <p>
+ $2.7.44.$ The moment of inertia of a solid body of mass $m$ relative to the $O$-axis is equal to $J$. The center of mass of the body is located at a distance $R$ from this axis. Find the force acting on the axis when a force $F$ is briefly applied to a solid body perpendicular to the segment of length $x$ that connects the point of application of the force and the axis. At which $x$ is the smallest force acting on the axis?
+</p>
+<center>
+ <figure>
+ <img src="2.7.44.png"
+ loading="lazy" width="130" />
+ <figcaption>
+ For problem $2.7.44$
+ </figcaption>
+ </figure>
+</center>
+<p>
+ </p>
+
+ <h3>Solution</h3>
+ <p>
+
+</p>
+<center>
+ <figure>
+ <img src="2.7.44_1.png"
+ loading="lazy" width="130" />
+ <figcaption>
+ Force $\vec{F}_0$ that will produce the rotational torque
+ </figcaption>
+ </figure>
+</center>
+<p>
+Force $\vec{F}$ creates an angular momentum $\vec{F}\cdot x$ (with $x$ perpendicular to $\vec{F}$):
+$$\tau_0=F\cdot x$$
+$$\tau_f=J\cdot\varepsilon$$
+In steady-state mode, the angular moments will be equal
+$$\tau_0=\tau_f=Fx=J\varepsilon$$
+From where
+$$\varepsilon = \frac{Fx}{J}$$
+Newton's second law for the rotational motion
+$$F+F_0=m\varepsilon R$$
+$$F_0=mR\cdot \frac{Fx}{J}-F\Leftrightarrow \boxed{F_0=F\left(\frac{mRx}{J}-1\right)}$$
+From here, the minimum values of $F_0 = 0$, described by the expression
+$$F_0=0\Leftrightarrow \frac{mRx}{J}-1=0$$
+which will be observed at length that connects the point of application of the force and the axis
+$$\boxed{x=\frac{J}{mR}}$$
+ </p>
+
+ <h4>Answer</h4>
+ <p>
+ $F'=F(mRx/J-1)$. With $x=J/(mR),~F'=0$
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