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| <h3 id="back-link"><a href="../../#2.1">$\leftarrow$Back</a></h3> | | <h3 id="back-link"><a href="../../#2.1">$\leftarrow$Back</a></h3> |
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| <h3> Statement </h3> | | <h3> Statement </h3> |
| <p> | | <p> |
| $2.1.47^*.$ Two bodies of the same mass connected by a thread slide along an inclined plane. Thread tension force $T$. There is no friction between one body and the board. Determine the friction force between the board and another body. | | $2.1.47^*.$ Two bodies of the same mass connected by a thread slide along an inclined plane. Thread tension force $T$. There is no friction between one body and the board. Determine the friction force between the board and another body. |
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| <figcaption> | | <figcaption> |
| For problem $2.1.47^*$ | | For problem $2.1.47^*$ |
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| <p> | | <p> |
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| <h3>Solution</h3> | | <h3>Solution</h3> |
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| <figcaption> | | <figcaption> |
| System of connected bodies | | System of connected bodies |
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| <p> | | <p> |
| Body of mass $m_3$ moves with acceleration of the center of mass of the system | | Body of mass $m_3$ moves with acceleration of the center of mass of the system |
| </p> | | </p> |
| <p> | | <p> |
| Considering the system as a whole (not taking into account internal forces) | | Considering the system as a whole (not taking into account internal forces) |
| $$ \boxed{a_3 = \frac{F}{M+2m}} $$ | | $$ \boxed{a_3 = \frac{F}{M+2m}} $$ |
| In this case, a force equivalent to double the tension force of the thread $2T$ acts on the body $m_3$. | | In this case, a force equivalent to double the tension force of the thread $2T$ acts on the body $m_3$. |
| $$ 2T = M a_3 $$ | | $$ 2T = M a_3 $$ |
| | | |
| $$ T = F\frac{M}{2(M+2m)} $$ | | $$ T = F\frac{M}{2(M+2m)} $$ |
| The body $m_1$ is acted upon by two forces $\vec{T}$ and $\vec{F}$ | | The body $m_1$ is acted upon by two forces $\vec{T}$ and $\vec{F}$ |
| </p> | | </p> |
| <p> | | <p> |
| We write Newton's second law for the first body as | | We write Newton's second law for the first body as |
| $$ F-T = ma_1 $$ | | $$ F-T = ma_1 $$ |
| | | |
| $$ \boxed{a_1=\frac{F(M+4m)}{2m(M+2m)}} $$ | | $$ \boxed{a_1=\frac{F(M+4m)}{2m(M+2m)}} $$ |
| Similarly, the second body $m_2$ is acted upon only by $\vec{T}$ | | Similarly, the second body $m_2$ is acted upon only by $\vec{T}$ |
| $$ m_2 = T $$ | | $$ m_2 = T $$ |
| | | |
| $$ \boxed{a_2=\frac{FM}{2m(M+2m)}} $$ | | $$ \boxed{a_2=\frac{FM}{2m(M+2m)}} $$ |
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| | | |
| <h4>Answer</h4> | | <h4>Answer</h4> |
| <p> | | <p> |
| Acceleration of cargoes 1–3: | | Acceleration of cargoes 1–3: |
| $$ a_1=\frac{F(M+4m)}{2m(M+2m)} $$ | | $$ a_1=\frac{F(M+4m)}{2m(M+2m)} $$ |
| | | |
| $$ a_2=\frac{FM}{2m(M+2m)} $$ | | $$ a_2=\frac{FM}{2m(M+2m)} $$ |
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| $$ a_3=\frac{F}{M+2m} $$ | | $$ a_3=\frac{F}{M+2m} $$ |
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