Solution D1-51 (Figure D1.5 condition 1 S.M. Targ 1989)

Solution to problem D1-51 (Figure D1.5, condition 1, S.M. Targ, 1989)

In this problem, a load of mass m, having received an initial speed v0 at point A, moves along a curved pipe ABC, which is located in a vertical plane. Pipe sections can be inclined or horizontal (Fig. D1.0 - D1.9, Table D1). In section AB, in addition to the force of gravity, the load is acted upon by a constant force Q (its direction is shown in the figures) and a resistance force of the medium R, which depends on the speed v of the load and is directed against the movement. The friction of the load on the pipe in section AB is not taken into account.

At point B, the load, without changing its speed, moves to the section BC of the pipe, where, in addition to the force of gravity, it is acted upon by the friction force (friction coefficient of the load on the pipe f = 0.2) and the variable force F, the projection of which Fx on the x axis given in the table.

If we consider the load to be a material point and the distance AB = l or the time t1 of movement of the load from point A to point B is known, then we can find the law of movement of the load on the section BC, that is, x = f(t), where x = BD.

It is necessary to solve the problem and find the law of cargo movement on the aircraft section.

This solution is a digital product available for purchase in a digital goods store. Solution D1-51 is a solution to the problem of moving a load of mass m along a curved pipe ABC located in a vertical plane. Figure D1.5 and condition 1 are given according to the book by S.M. Targa 1989.

This digital product is designed in a beautiful html format, which makes it easy to read and study the solution to the problem. The description contains all the necessary details and conditions that will allow you to fully understand the solution to the problem and apply it in practice.

By purchasing Solution D1-51 (Figure D1.5 condition 1 S.M. Targ 1989), you receive a useful digital product that will help you deepen your knowledge in the field of physics and mathematics, as well as solve similar problems in practice.

Solution D1-51 (Figure D1.5 condition 1 S.M. Targ 1989) is a digital product that represents a solution to the problem of moving a load of mass m along a curved pipe ABC located in a vertical plane. The solution includes all the necessary details and conditions for solving the problem, including Figure D1.5 and condition 1 from the book by S.M. Targa 1989.

A load D of mass m moves along a curved pipe ABC, where sections of the pipe can be inclined or horizontal. In section AB, in addition to the force of gravity, the load is acted upon by a constant force Q and a resistance force of the medium R, which depends on the speed of the load and is directed against the movement. The friction of the load on the pipe in section AB is not taken into account. At point B, the load moves to section BC of the pipe, where it is acted upon by a friction force (coefficient of friction of the load on the pipe f = 0.2) and a variable force F, the projection of which Fx on the x axis is given in the table.

To find the law of movement of cargo on the section BC, it is necessary to know the distance AB = l or the time t1 of movement of the cargo from point A to point B. Considering the cargo as a material point, you can find x = f(t), where x = BD.

The D1-51 solution is available in a beautiful html format, which makes it easy to read and study the solution to the problem. This digital product will help you deepen your knowledge in the field of physics and mathematics, as well as solve similar problems in practice.


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Solution D1-51 is a problem about the movement of a load of mass m along a curved pipe ABC located in a vertical plane. The load receives an initial speed v0 at point A and moves along the section AB, on which, in addition to the force of gravity, a constant force Q and a resistance force of the medium R, depending on the speed of the load, act. At point B, the load moves to section BC of the pipe, where it is acted upon by friction and variable force F.

To solve the problem, it is necessary to find the law of cargo movement on the aircraft section, that is, the function x = f(t), where x is the distance between points B and D, and t is the time of cargo movement on the aircraft section. The coefficient of friction between the load and the pipe in the aircraft section is f = 0.2.

To solve the problem, it is necessary to know the distance AB = l or the time t1 of movement of the load from point A to point B.


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