Homework H3.E – Sp 26

Problem statement
Solution video

DISCUSSION THREAD


Any questions??


Discussion and hints:

The disk shown above has TWO components of rotation (note that ω0 = 0):

  • a rotation rate of θ_dot about a fixed axis (the “+” K-axis), and,
  • a rotation rate of ωdisk about a moving axis (the “-” x-axis)

(Be sure to make a clear distinction between the lower case and upper case symbols.)

Therefore, the angular velocity of the disk is given by:

ω =θ_dot* K – ωdisk i

The angular acceleration vector α is simply the time derivative of the angular velocity vector ω : α = dω/dt. In taking this time derivative,

  • Recall that the K-axis is fixed. Since K is fixed, then dK/dt = 0.
  • Recall that the i-axis is NOT fixed. Knowing that, how do you find di/dt?

 

33 thoughts on “Homework H3.E – Sp 26”

  1. Does theta-dot not also contribute to the angular velocity of the disk? I noticed it was not included in the formula posted in the discussion/hints and I am unsure as to why.

    1. It appears that the hints provided were based on a different set of parameters. That set of parameters had omega_0 ≠ 0 and theta_dot = 0. The version of the problem here is for omega_0 = 0 and theta_dot ≠ 0.

      I will modify the hints to align them for the later version described above.

    1. Please note that omega_0 = 0 according to the problem statement.

      There was a typo in the discussion points above in that the component of rotational velocity about the K-axis is theta_dot, not omega_0. That has now been fixed.

    1. That would not be a good assumption to make.

      In this problem, as well as all problems in this section, you need to first write down the angular velocity (omega) of the rigid body that is being asked. This omega vector will likely have components about more than one axis: some axes will be fixed; some axes will be rotating. You need to take this into account as you take the derivative of omega to find the angular acceleration of the body.

      As stated in the Discussion above, this disk has two components of rotation: theta_dot about K_hat and omega_disk about negative i_hat . K_hat is fixed, and i_hat is moving.

      1. Can we assume alpha disk is in the same direction as omega disk? I understand that total angular acceleration is given by the derivative of the summation of angular velocities, however, alpha disk specifically I thought referred to the angular acceleration of the disk itself about its axis at C. Therefore, I assumed the angular acceleration of the disk was specifically increasing the magnitude of angular velocity of the disk about point C.

        1. No. The angular velocity of the disk has two components: theta_dot about K_hat and omega_disk about -i_hat.The angular acceleration has a component in the direction of omega x i_hat.

    1. You should start out each problem by defining to which rigid body your moving xyz-axes are attached. In this case, you would choose the disk. Then, for example, d(i_hat)/dt = omega x i_hat, where omega is the angular velocity of your xyz-axes.

  2. For W_disk isn’t it rotating in the + x direction based on the arrow, in the hints it mentions the -x direction. also would it be on the X axis instead of the lowercase x axis since theta = 0?

    1. For the first question, it is rotating in the negative x-axis: curl the fingers of your right hand in the direction shown in the figure. Your thumb will point in the negative x-direction.

      For the second question, yes, at this instant i_hat = I_hat. However, when you take the time derivative of omega to find alpha, you need an expression for omega that is valid for ALL time. The direction of the omega_disk tracks the x-axis, NOT the fixed X-axis. Therefore, prior to taking the derivative we need to distinguish between the moving i_hat axis and the fixed I_hat axis.

      Let me know if this is not clear. Good question, though.

  3. I’m confused why there are two omega disks? Like they give angular velocity of disk = 2 rad/s, but then part a asks you to determine the angular velocity of the disk? I understand there’s a difference between omega total and omega disk, but why do we call them the same thing?

    1. As the problem description states, omega_disk is the name given to the angular speed of the disk relative to arm OC. That is only one component of the angular velocity of the disk. The angular velocity of the disk is the vector sum of the angular velocity of arm OC with the angular velocity of the disk relative to the arm.

      If the name omega_disk is confusing, feel free to give it a different name.

    1. When finding the time derivative of a unit vector, you take the cross product of the angular velocity vector omega with the unit vector. Since the cross product involves two vectors, then omega must be a vector, not a magnitude.

  4. The omega in the theta direction would have a fixed z direction. For differentiation, the theta double dot term would go to zero, leaving an answer in the x and y directions only.

  5. The capital Y and Z terms will be equivalent to the y and z terms as they are in line with the instant. The w0 and w distk dot term in the acceleration would go to zero as they are constant.

  6. It’s clear that the coordinate systems are aligned correct? Will it be given to us that the coordinate systems are aligned or will we just have to think about it intuitively?

  7. I’m a little confused about the signs on w_disk and w’_disk. The problem gives them as 2 and 5. Based off of the diagram, w_d is in the negative x-axis. However, we don’t know if w’_d is in the same clockwise direction or if it’s actually positive. When plugging in, should I use -w_d in the i direction and +w’_d in the i direction?

    1. As you state here, the disk is rotating about OC in the negative x direction with an angular speed of omega_disk, making a contribution of -2*i_hat to the omega vector. That number omega_disk is INCREASING at a rate of 5 rad/s^2. This would correspond to a contribution of -5*i_hat to the alpha vector.

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