Resistance Variable Cross Section

In summary, the question asks for the resistance R of a disk with radius r and width w, whose cross sectional area is variable. The equation for the circle of radius r gives y = \sqrt{r^2-x^2} which needs to be multiplied by 2 and w to get the cross sectional area. The disk is connected to the circuit on the cylindrical sides, and the metalization is deposited along the length of the two thin stripes running the length of the cylinder.
  • #1
millifarads
5
0

Homework Statement



The question asks for resistance R of a disk with radius r and fixed width w, whose cross sectional area is variable. Unlike in the picture below, the resistor is not connected to the circuit on the flat ends, but on the cylindrical sides.


Homework Equations



2_3_4_1_eng.png


The Attempt at a Solution



With [tex]R = \rho \frac{L}{A}[/tex]L = 2r, ρ is given, but I'm having trouble setting up an expression for the cross sectional area. Normally, for cross sectional area of this type of problem it's just the area of a circle, and some integration will be required with the bounds being the radius at each end.

But here my initial thought is to set up an expression for a one dimensional line along the top of the disk, then multiple that by the width of the disk, w. The area will change with the radius though, so I'm not sure if integration is required.

From the equation for the circle of radius r, I get

[tex]y = \sqrt{r^2-x^2}[/tex]

which then needs to be multiplied by 2, and then by w to get a sort of cross sectional area:

[tex]R = \rho \frac{2r}{2w*\sqrt{r^2-x^2}}[/tex]

Am I on the right track?
 
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  • #2
How are the connections made to the resistor? Is the curved area divided into two with conductor deposited along the entire curved surface except for two thin cracks, or ? A picture would be a good thing to have here.
 
  • #3
Attached is a picture. The disk has radius 2r, I'm assuming the wires connect somewhere on the cylindrical sides.
 

Attachments

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    disk.png
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  • #4
The picture still does not show exactly how the metalization is deposited. For example, were the flat ends connected instead, the metalization would be across the entire flat surfaces.

So let's assume two diametrically opposed and arbitrarily thin stripes running the length of the cylinder. Then you can integrate dR from o to r and multiply by two. You definitely need to integrate.
 
  • #5




Yes, you are on the right track. Since the cross sectional area is variable, we need to take into account the changing radius as we move along the disk. Your approach of setting up an expression for a one dimensional line along the top of the disk and then multiplying by the width is a good start. However, you will need to integrate this expression over the entire cross sectional area to get the correct value for R.

To set up the integration, you can use the formula for the area of a circle, A = πr^2, and substitute in your expression for the radius. This will give you an expression for the cross sectional area in terms of x, the distance along the top of the disk. Then, you can integrate this expression from 0 to r (the radius of the disk) to get the total cross sectional area.

Once you have the cross sectional area, you can plug it into your original equation, R = ρL/A, to get the resistance in terms of the variable cross sectional area. Remember to use the correct value for L, which in this case would be the circumference of the disk, 2πr.

I hope this helps guide you towards a solution. Good luck!
 

1. What is resistance variable cross section?

Resistance variable cross section is a type of material or component that has an uneven or varying thickness, leading to changes in its electrical resistance along its length or width. This can be achieved through various methods, such as varying the material composition, changing the shape, or using conductive coatings.

2. How does resistance variable cross section work?

The varying thickness of the material in resistance variable cross section causes changes in its electrical resistance, as the electrons have to travel through different distances and encounter different obstacles. This can be used in various applications, such as sensors, switches, and circuit components.

3. What are the advantages of using resistance variable cross section?

Resistance variable cross section offers several advantages, such as the ability to finely control the resistance of a material, leading to more precise and sensitive sensors. It also allows for more compact and efficient circuit designs, as well as the potential for self-regulation and self-repair in certain applications.

4. What are some real-world applications of resistance variable cross section?

Resistance variable cross section has a wide range of applications in various industries, including automotive, aerospace, medical, and consumer electronics. It can be used in sensors for measuring pressure, temperature, and humidity, as well as in switches, circuit components, and smart materials.

5. Are there any limitations or challenges in using resistance variable cross section?

While resistance variable cross section has many benefits, there are also some limitations and challenges. These include the need for precise manufacturing processes to ensure consistent resistance values, as well as potential reliability issues in harsh environments due to the varying thickness of the material. Additionally, the cost of these materials can be higher compared to traditional materials.

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