Write an expression w1 of the angle shown in the first picture

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Homework Help Overview

The discussion revolves around the relationship between the angular velocity w1 of a bicycle wheel rolling along a circular path and its angle of inclination. The wheel is treated as a homogeneous ring with specific parameters, and participants are exploring the kinematic relationships and forces involved in the system.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the relationship between angular velocities, specifically questioning the correctness of the relation between ω0 and ω1. There are attempts to derive expressions for velocity and torque, and some participants suggest corrections to the original poster's equations.

Discussion Status

There is ongoing exploration of the relationships between the variables involved, with some participants providing guidance on substituting expressions. Multiple interpretations of the equations are being discussed, and while some progress has been made, there is no explicit consensus on the final formulation.

Contextual Notes

Participants note the complexity of the equations and the involvement of matrices, which may affect the clarity of communication. There is also a request for clearer formatting of mathematical expressions to facilitate discussion.

Karl Karlsson
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Homework Statement
A bicycle wheel rolls at a constant speed along a circular path on a horizontal surface. The wheel has a constant angle of inclination to the vertical direction and the distance from its center of mass G to the fixed Z axis is R. Determine the relationship between the angular velocity w1 around the Z axis and the angle of inclination (shown in the picture above). Treat the wheel as a homogeneous ring with mass m and radius r.
Relevant Equations
A bicycle wheel rolls at a constant speed along a circular path on a horizontal surface. The wheel has a constant angle of inclination to the vertical direction and the distance from its center of mass G to the fixed Z axis is R. Determine the relationship between the angular velocity w1 around the Z axis and the angle of inclination (shown in the picture above). Treat the wheel as a homogeneous ring with mass m and radius r.
Skärmavbild 2019-10-10 kl. 00.45.01.png

A bicycle wheel rolls at a constant speed along a circular path on a horizontal surface. The wheel has a constant angle of inclination to the vertical direction and the distance from its center of mass G to the fixed Z axis is R. Determine the relationship between the angular velocity w1 around the Z axis and the angle of inclination (shown in the picture above). Treat the wheel as a homogeneous ring with mass m and radius r.

Lead:
1) Introduce a resale system Gxyz as shown in the figure.
2) Use the kinematics (speed relationship between G and C) and determine the relationship between
wheel spinning speed ω0 around x-axis and ω1. Consider the direction of ω0.
3) Formulate the force equation maG F and determine the frictional force F and the normal force N of
the wheel at the contact point C.
4) Determine the wheel's torque HG = IGω in the resal system. What is ω here?
5) Formulate the torque equation HG  ωS  HG  MG. What is ωS here?
6) Insert the relationship between 0 and 1 in the torque equation and determine 1.

My attempt:
IMG_0419.jpg

IMG_0420.jpg


The correct answer is w1=(2gtan(angle)/(4R+r*sin(angle)))^(1/2)
 
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I think the mistake is with the relation ##\omega_0 = \frac{R}{r} \omega_1##.

I believe the correct relation is ##\omega_0 = \frac{R+r\sin\theta}{r} \omega_1##.

In your derivation where you have an expression for ##\vec V_c##, I think you should have

##\vec V_c =\omega_x \hat e_x \times (-r \hat e_z)+R \omega_1 \hat e_y = (-\omega_0 +\omega_1\sin \theta)\hat e_x \times (-r \hat e_z)+R \omega_1 \hat e_y##.

Here, ##\omega_x## is the x-component of the vector ##\vec \omega## that you used in the matrix calculation of the angular momentum. From ##\vec V_c = 0##, you then get ##\omega_0 = \frac{R+r\sin\theta}{r} \omega_1##.

If you use this expression for ##\omega_0## in the next-to-last line of your first page of notes, then I think things will work out.

If possible, we ask that you please try to type out your work rather than post a picture of your hand written notes. It is difficult to quote a specific part of a picture.
 
Last edited:
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TSny said:
I think the mistake is with the relation ##\omega_0 = \frac{R}{r} \omega_1##.

I believe the correct relation is ##\omega_0 = \frac{R+r\sin\theta}{r} \omega_1##.

In your derivation where you have an expression for ##\vec V_c##, I think you should have

##\vec V_c =\omega_x \hat e_x \times (-r \hat e_z)+R \omega_1 \hat e_y = (-\omega_0 +\omega_1\sin \theta)\hat e_x \times (-r \hat e_z)+R \omega_1 \hat e_y##.

Here, ##\omega_x## is the x-component of the vector ##\vec \omega## that you used in the matric calculation of the angular momentum. From ##\vec V_c = 0##, you then get ##\omega_0 = \frac{R+r\sin\theta}{r} \omega_1##.

If you use this expression for ##\omega_0## in the next-to-last line of your first page of notes, then I think things will work out.

If possible, we ask that you please try to type out your work rather than post a picture of your hand written notes. It is difficult to quote a specific part of a picture.

Thanks! Of course, I must have forgotten about that. But now, for some reason, I still don't manage to get the correct answer:

IMG_0421.JPG


IMG_0422.JPG


There are so many equations and a matrix involved which makes it a lot easier for me to send a picture compared to writing all the equations on the computer
 
This part of your first post looks correct to me
1570817256729.png


You just need to substitute for ##\omega_0## in terms of ##\omega_1##.
 
Last edited:
TSny said:
This part of your first post looks correct to me
View attachment 250981

You just need to substitute for ##\omega_0## in terms of ##\omega_1##.
That's right, it works now. Thanks!
 

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