Detailed modeling of a Pulley System, HELP

In summary, the conversation discusses the detailed modeling of a pulley system, with a focus on the considerations and equations needed for accurate representation. These include modeling the sheaves, calculating tension due to friction, determining moments on the sheaves, and considering forces on the weight. There is also a question about how to model individual sheaves with different velocities, which can be done by taking into account the linear velocity of the cable and the radius of the pulley.
  • #1
gtavictor
7
0
Detailed modeling of a Pulley System, HELP!

Hello people,

Currently I have a project of a pulley system, and I have to model it with fair detailed equations. Actually this continues from another thread I started sometime ago, but I made a new thread because now I'm continuing with the project. The next are the considerations I need to be aware of:
  • Wire rope as a stretchable string (I suppose I have to model it as a spring).
  • Damping in the wire can be neglected but consider a very high stifness of the wire so small permanent oscillations occur in the system.
  • Angular position, velocity and acceleration of each sheave.
  • Displacement, velocity and position of the sheaves attached to the weight, in this case is obvious both sheaves and the weight share the same translational movements.
  • Consider [itex]\mu[/itex] as the friction between shaft and bearing of the sheave.
  • Consider the friction between wire rope and sheave high enough so no sliding occurs.

ForumProject1.png
ForumProject2.png
ForumProject3.png


Sheave modeling: For this I'm based on the first and second images. I'm doing the modeling for the velocities, so if I integrate or derivate I get position or acceleration respectively:

Sheave1: in this case [itex] v_{c1}=0 [/itex]
[tex] v_{a1}=v_{c1}-R*\omega_1=-R*\omega_1 [/tex]
[tex] v_{b1}=v_{c1}+R*\omega_1=R*\omega_1 [/tex]
[tex] v_{a1}=-v_{b1} [/tex]

Sheave2:
[tex] v_{a2}=v_{c2}-R*\omega_2 [/tex]
[tex] v_{b2}=v_{c2}+R*\omega_2 [/tex]

Sheave3: in this case [itex] v_{c3}=0 [/itex]
[tex] v_{a3}=v_{c3}-R*\omega_3=-R*\omega_3 [/tex]
[tex] v_{b3}=v_{c3}+R*\omega_3=R*\omega_3 [/tex]

Sheave4: in this case [itex] v_{b4}=0 [/itex]
[tex] v_{a4}=v_{c4}-R*\omega_4 [/tex]
[tex] v_{b4}=v_{c4}+R*\omega_4 [/tex] --> [tex] v_{c4}=-R*\omega_4 [/tex]
also --> [tex] v_{a4}=-2*R*\omega_4 [/tex]

Then I consider the velocities the same where I have one same string connected:
[tex] v_{b1}=v_{a2} [/tex]
[tex] v_{b2}=v_{a3} [/tex]
[tex] v_{a4}=v_{b3} [/tex]

From this sheaves modeling I don't know if these velocities I mentioned before are the same, from the initial considerations I have a stretchable spring but from what I know the velocities in both ends of the wire segment between sheave and sheave should not be the same, if that's the case then, how can I model each sheave individually with different velocities?

Tensions in each wire segment due to friction shaft-bearing: For this I'm based on the first image, starting for the rightest sheave (where less tension should be applied in the wires due to the final fixed point).

r=Radius of shaft
R=Radius of sheave
For sheave 4:
[tex] N=T_2+T_1 [/tex]
[tex] \mu*N*r=(T_2-T_1) [/tex]
[tex] N=\frac{(T_2-T_1)*R}{\mu*r} [/tex]
[tex] \frac{(T_2-T_1)*R}{\mu*r}-T_1-T_2=0 [/tex]
[tex] T_2=\frac{T_1*(R+\mu*r)}{R-\mu*r} [/tex]

then for sheave 3:
[tex] T_4=\frac{T_1*(R+\mu*r)^2}{(R-\mu*r)^2} [/tex]

then for sheave 2:
[tex] T_6=\frac{T_1*(R+\mu*r)^3}{(R-\mu*r)^3} [/tex]

then for sheave 1:
[tex] F_w=\frac{T_1*(R+\mu*r)^4}{(R-\mu*r)^4} [/tex]

For this modeling I just did I see from the equations that I have an increase of tension due to the friction between shaft and bearing of the sheave, but like for the previous modeling I'm not sure if I'm doing good, also, the tension in 1 should be IDEALLY:

[itex] T_1=\frac{W}{MA} [/itex] where MA is the mechanical advantage equal to 4 for this pulley system, but still this is IDEALLY, so I don't know how to model some good equations for this part, at least I have something.

Moments on sheaves: I did some modeling about the moments present on each sheave and for that I come up with a general equation:

[tex] J_o*\ddot{\theta}_n=[(\frac{T_1*(R+\mu*r)^{n-1}}{(R-\mu*r)^{n-1}})-(\frac{T_1*(R+\mu*r)^{n}}{(R-\mu*r)^{n}})]*R-(-1)^{n+1}*\mu*[(\frac{T_1*(R+\mu*r)^{n-1}}{(R-\mu*r)^{n-1}})+(\frac{T_1*(R+\mu*r)^{n}}{(R-\mu*r)^{n}})]*r [/tex]
where n = sheave number from the first image (not the number or quantity of sheaves)

Forces on the Weight: For this modeling I use the third image.

[tex] m*a+K_1*y+K_2*y+K_3*y+K_4*y=0 [/tex]

In this case I might consider the stiffness equal in each wire segment but still when I think about this equation I get problems with the others.

Please I nee good help about the detailed modeling of this system, I guess it's complicated from a first point of view but maybe it's because of my lack of knowledge on this kind of modeling!

Thanks in advance!
 
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  • #2


"how can I model each sheave individually with different velocities?"

Consider the linear velocity of the cable and the radius of the pulley.
 
  • #3


ty2nu said:
"how can I model each sheave individually with different velocities?"

Consider the linear velocity of the cable and the radius of the pulley.

Thanks, I know that but the problem is to model the translational speed of the two sheaves attached to the weight, also, i guess that the sheave on the left of the weight has a higher angular velocity than its partner on the right of the weight!
 

Related to Detailed modeling of a Pulley System, HELP

1. What is a pulley system and how does it work?

A pulley system is a simple machine consisting of a wheel with a groove around its circumference and a rope or cable passing over it. It works by changing the direction of the force applied to the rope, allowing for easier lifting or movement of heavy objects.

2. How do you create a detailed model of a pulley system?

To create a detailed model of a pulley system, you will need to determine the number of pulleys and their arrangement, as well as the type and length of the rope or cable. You will also need to consider the weight of the load and the amount of force needed to lift it. Using these variables, you can create a diagram or use a computer program to simulate the system and calculate the mechanical advantage.

3. What is the mechanical advantage of a pulley system?

The mechanical advantage of a pulley system is the ratio of the output force (the weight being lifted) to the input force (the force applied to the rope or cable). It is determined by the number of pulleys in the system and can be calculated using the formula MA = (2n - 1), where n is the number of movable pulleys in the system.

4. How does friction affect the efficiency of a pulley system?

Friction can affect the efficiency of a pulley system by reducing the output force and increasing the amount of force needed to lift the load. This is because some of the input force is lost due to the friction between the rope and the pulley. To minimize this effect, it is important to use smooth and well-lubricated pulleys and ropes with low friction coefficients.

5. Can a pulley system be used to lift objects of any weight?

Yes, a pulley system can be used to lift objects of any weight as long as the mechanical advantage is high enough. However, the number of pulleys needed and the amount of force required to lift the load will increase as the weight of the load increases. It is important to consider the weight and the capabilities of the pulley system before attempting to lift heavy objects.

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