Need help setting up Eqtn of motion.

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the equation of motion for the charged square plate in an electric field is established. The torque acting on the plate is influenced by both the force, which varies with the angle of rotation, and the distance from the center, which also depends on the angle. The force is derived from the electric field strength and the charge on the plate, while the torque is expressed as QEr cos²(θ). The moment of inertia for the plate is calculated as 1/2 mr², leading to the angular acceleration equation α = (2QEr cos²(θ)) / (mr²). This framework allows for the analysis of the plate's rotational dynamics in the electric field.
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Torque in Electric Field...need help with eqtns of motion...

Ok - I have a charged square plate Q with a weightless rod attached through the centre of the plane so that the plate can rotate like a propeller.

Half of the plate sits in an E field and so feels a torque.
The E field drops off as \frac{1}{r^2}

I need to set up the equation of motion.

Now, I know that:

\Gamma = Fd

My problem is that F=F(\theta) \:and\: d=d(\theta)

i.e as the plate rotates less of it will feel the electric field - it will be completely half immersed in the E field at an angle of 0 deg (perp to field)and will feel the max force, and be at a min when the plate is parallel to the field and feel zero force.

Also as the plate rotates some if it will be closer to the E field and some of it will be further away so there is also the theta dependant distance.

Can anyone help me set up the eqtns of motion?
 
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The equation of motion can be written as follows:\frac{d^2 \theta}{dt^2} = \frac{Q}{m}\left(\frac{E}{d^2}\right)\sin \theta Where m is the mass of the plate, E is the electric field and d is the distance between the center of the plate and the point where the electric field is applied.
 


Sure, I can help you with setting up the equations of motion for this problem. First, let's define some variables:

- Q: charge of the square plate
- m: mass of the square plate
- E: electric field strength
- r: distance from the center of the plate to the edge
- \theta: angle of rotation of the plate
- \Gamma: torque acting on the plate
- F: force on the plate due to the electric field
- d: distance from the center of the plate to the point where the force is applied

Now, let's break down the problem into two parts: the torque and the force.

1. Torque:

The torque acting on the plate is given by:
\Gamma = Fd

We know that the force, F, is dependent on the angle of rotation, \theta, and the distance, d, is also dependent on \theta. So, we can rewrite the equation as:
\Gamma = F(\theta)d(\theta)

2. Force:

The force on the plate due to the electric field is given by:
F = QE

Since the electric field drops off as \frac{1}{r^2}, we can rewrite this as:
F = Q\frac{E}{r^2}

Now, we need to find the distance, d, from the center of the plate to the point where the force is applied. We can use trigonometry to find this distance:
d = r\cos\theta

Substituting this into our equation for torque, we get:
\Gamma = Q\frac{E}{r^2}\cos\theta \times r\cos\theta

Simplifying, we get:
\Gamma = QEr\cos^2\theta

Finally, we can use the equation of motion for rotational motion:
\Gamma = I\alpha

Where I is the moment of inertia and \alpha is the angular acceleration. Since we are dealing with a plate that can rotate like a propeller, the moment of inertia is given by:
I = \frac{1}{2}mr^2

Substituting this into our equation, we get:
QEr\cos^2\theta = \frac{1}{2}mr^2\alpha

Solving for \alpha, we get:
\alpha = \frac{2QEr\cos^2\theta}{mr^2}

And
 
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