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A fuel gauge uses a capacitor to determine the height of the fuel in a tank. The effective dielectric con- stant \(K_{\text {eff }}\) changes from a value of 1 when the tank is empty to a value of \(K\), the dielectric constant of the fuel, when the tank is full. The appropriate electronic circuitry can determine the effective dielectric constant of the combined air and fuel between the capacitor plates. Each of the two rectangular plates has a width \(w\) and a length \(L\) (Fig. \(\mathbf{P 2 4 . 6 6}\) ). The height of the fuel between the plates is \(h\). You can ignore any fringing effects. (a) Derive an expression for \(K_{\text {eff }}\) as a function of \(h\). (b) What is the effective dielectric constant for a tank \(\frac{1}{4}\) full, \(\frac{1}{2}\) full, and \(\frac{3}{4}\) full if the fuel is gasoline \((K=1.95) ?\) (c) Repeat part (b) for methanol \((K=33.0)\). (d) For which fuel is this fuel gauge more practical?

Short Answer

Expert verified
The short answer will depend on the calculations made in Steps 2 and 3, and the comparison made in Step 4.

Step by step solution

01

Derive expression for \(K_{\text {eff }}\)

Let the distance between the plates be \(d\). The effective dielectric constant \(K_{\text {eff }}\) can be derived by considering the capacitor as two capacitors in series, one filled with air and the other with fuel. The dielectric constant of air is 1, and the height of the air part is \(d-h\). The dielectric constant of fuel is \(K\) and the height is \(h\). The total capacitance of the capacitor would be \(C_{total}=(\varepsilon_{0}wL/(d-h\))\(C_{2}=\varepsilon_{0}KwL/h\), where \(C_{1}\) and \(C_{2}\) are the capacitances of the air and fuel parts respectively. The total capacitance when two capacitors are in series is given by \(1/C_{total}=1/C_{1}+1/C_{2}\). Solve this equation for \(K_{\text {eff }}=\varepsilon_{0}K_{eff}wL/d\), where \(K_{eff}\) is the effective dielectric constant.
02

Calculate \(K_{\text {eff }}\) for different fuel heights

To find \(K_{\text {eff }}\) for a tank \(\frac{1}{4}\) full, \(\frac{1}{2}\) full, and \(\frac{3}{4}\) full for gasoline, substitute the corresponding \(h\) values and \(K = 1.95\) into the expression derived in Step 1 and calculate \(K_{\text {eff }}\) respectively.
03

Repeat calculations for methanol

Repeat the calculations in Step 2, but this time using \(K = 33.0\), the dielectric constant for methanol.
04

Determine the more practical fuel

The fuel gauge will be more practical for the type of fuel that leads to larger changes in the effective dielectric constant for changes in fuel height. Compare the results from Steps 2 and 3 to make this determination.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Dielectric Constant
The dielectric constant is a measure of a material's ability to store charge and affects how capacitors behave when different substances are between the plates. In this problem, the dielectric constant varies based on the fuel level in a tank, impacting the capacitance measurement used by a fuel gauge.
When a tank is empty, the dielectric constant of air, which is 1, dominates. As fuel fills the tank, the dielectric constant increases to the value characteristic of the fuel used. For gasoline, the constant is 1.95 and for methanol, it's 33.0. The effective dielectric constant, denoted as \(K_{\text{eff}}\), changes between these values as the fuel level changes.
  • If the tank is full, \(K_{\text{eff}}\) equals the dielectric constant of the fuel.
  • When the tank is empty, \(K_{\text{eff}}\) is 1, as only air is between the capacitor plates.
  • For intermediate levels, \(K_{\text{eff}}\) can be calculated by considering the tank as comprising two series capacitors—one with air and the other with fuel.
Understanding how \(K_{\text{eff}}\) changes helps engineers design more accurate fuel gauges.
Fuel Gauge Mechanics
Fuel gauges often utilize capacitors, which change capacitance based on the material between their plates. This feature is employed in determining the fuel level in a tank. Here's how it works:
First, the capacitor plates are installed in the fuel tank. As the fuel level changes, the material between the plates changes from air to fuel, significantly affecting capacitance.
It's important to accurately establish the effective dielectric constant at different fuel levels. This helps electronic circuits measure fuel height based on the changing capacitance. By detecting changes in \(K_{\text{eff}}\), the fuel gauge can effectively calculate the fuel level, whether the tank is 1/4, 1/2, or 3/4 full.
  • For instance, when the fuel is gasoline, the gauge must measure changes from 1 to 1.95.
  • For methanol, this range is more substantial, from 1 to 33.0.
This technique allows for precise fuel level readings by considering the different dielectric constant values between air and fuel.
Capacitor Design
Capacitor design is critical in developing a reliable fuel gauge that can measure fuel levels accurately. The design considers multiple factors to optimize the capacitor's performance in a fuel gauge.
The main challenge is to handle capacitors" changes in capacitance as they operate with a combination of air and fuel. The approach involves treating the setup as two separate capacitors in series. Here's a simplified process:
  • Design plates considering the tank's dimensions, such as width \(w\) and length \(L\).
  • Calculate \(K_{\text{eff}}\) using the derivation of effective capacitance when combining air-filled and fuel-filled capacitors.
  • Ensure the design allows accurate measurements regardless of fuel level.
The goal is to create a system sensitive enough to distinguish small changes in \(K_{\text{eff}}\). Thus, a tank that is partially filled tweaks the capacitor composition, adjusting the fuel gauge's reading. Understanding the design principles allows for choosing the correct plate size and spacing, improving accuracy, and providing a reliable fuel measurement system.

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Most popular questions from this chapter

BIO Cell Membranes. Cell membranes (the walled enclosure around a cell) are typically about \(7.5 \mathrm{nm}\) thick. They are partially permeable to allow charged material to pass in and out, as needed. Equal but opposite charge densities build up on the inside and outside faces of such a membrane, and these charges prevent additional charges from passing through the cell wall. We can model a cell membrane as a parallel-plate capacitor, with the membrane itself containing proteins embedded in an organic material to give the membrane a dielectric constant of about \(10 .\) (See Fig. \(\mathbf{P 2 4 . 4 8}\).) (a) What is the capacitance per square centimeter of such a cell wall? (b) In its normal resting state, a cell has a potential difference of \(85 \mathrm{mV}\) across its membrane. What is the electric field inside this membrane?

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