The solution to problem D1-76 (Figure D1.7 condition 6 S.M. Targ 1989) consists in describing the movement of a load of mass m, which received an initial speed v0 at point A and moves in a curved pipe ABC located in a vertical plane. The pipe sections are either both inclined, or one horizontal and the other inclined (see Figures 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 (the direction is shown in the figures) and a resistance force of the medium R, depending on the speed v of the load (directed against the movement). We neglect the friction of the load on the pipe in section AB. 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 affected 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 is given in table.
To find the law of cargo movement on the aircraft section, i.e. x = f(t), where x = BD, we consider the load to be a material point and know the distance AB = l or the time t1 of movement of the load from point A to point B.
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Our solution contains a detailed description of the movement of a mass m, which received an initial speed v0 at point A and moves in a curved pipe ABC located in a vertical plane. The task is presented in a beautiful html design, preserving the structure of tables and figures.
The solution contains all the necessary calculations and formulas for finding the law of movement of the load on the aircraft section, where, in addition to the force of gravity, it is acted upon by the friction force and the variable force F, the projection of which Fx on the x axis is given in the table.
By purchasing our solution, you get access to a high-quality product that will help you successfully solve problem D1-76 and improve your knowledge in physics.
Solution D1-76 (Figure D1.7 condition 6 S.M. Targ 1989) is a product that is a detailed description of the movement of a load of mass m, which received an initial speed v0 at point A and moves in a curved pipe ABC, located in a vertical plane. The solution is presented in the form of a beautifully designed HTML document, preserving the structure of tables and figures.
The task is to find the law of movement of the load on the section BC of the pipe, where, in addition to the force of gravity, the load is affected by the friction force and the variable force F, the projection of which Fx on the x axis is given in the table. 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 v of the load (directed against the movement). 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 and the variable force F.
The solution contains all the necessary calculations and formulas for finding the law of cargo movement in the section BC, where x = BD, considering the cargo as a material point and knowing the distance AB = l or the time t1 of movement of the cargo from point A to point B.
By purchasing this solution, you get access to a high-quality product that will help you successfully solve problem D1-76 and improve your knowledge in physics.
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Solution D1-76 is a dynamics problem that describes the movement of a load of mass m in a pipe ABC located in a vertical plane. The load receives an initial speed v0 at point A and moves along a curved pipe, overcoming the force of gravity, the constant force Q and the resistance force of the medium R, which depends on the speed of the load. In the section BC, the load is acted upon by a friction force (friction coefficient f = 0.2) and a variable force F, the projection of which Fx on the x axis is given in the table.
To solve the problem, it is necessary to find the law of movement of the load on the aircraft section, i.e. x = f(t), where x = BD. The distance AB = l or the time t1 of movement of the load from point A to point B is known. The solution to the problem involves neglecting the friction of the load on the pipe in section AB.
To solve the problem, you can use the equation of motion of a body, which relates the movement of a body to time and acceleration. You can also use the law of conservation of energy, which allows you to find the speed of a body at any point in its motion.
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