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\({ }^{}\) SSM A \(2.0 \mu \mathrm{F}\) capacitor and a \(4.0 \mu \mathrm{F}\) capacitor are connected in parallel across a \(300 \mathrm{~V}\) potential difference. Calculate the total energy stored in the capacitors.

Short Answer

Expert verified
The total energy stored in the capacitors is 0.27 J.

Step by step solution

01

Understand the Problem

We have two capacitors connected in parallel, meaning the potential difference across each capacitor is the same. We need to calculate the total energy stored in both capacitors when they are charged to a 300 V potential difference.
02

Identify the Formula for Energy Stored in a Capacitor

The energy stored in a single capacitor can be calculated using the formula \( E = \frac{1}{2} C V^2 \), where \( E \) is the energy, \( C \) is the capacitance, and \( V \) is the voltage across the capacitor.
03

Calculate the Energy for Each Capacitor

For the \(2.0 \, \mu F\) capacitor, the energy stored is: \[E_1 = \frac{1}{2} \times 2.0 \times 10^{-6} \, F \times (300 \, V)^2 = 0.09 \, J\] For the \(4.0 \, \mu F\) capacitor, the energy stored is: \[E_2 = \frac{1}{2} \times 4.0 \times 10^{-6} \, F \times (300 \, V)^2 = 0.18 \, J\]
04

Calculate the Total Energy Stored in Both Capacitors

Since the capacitors are in parallel, the total energy stored is the sum of the energies stored in each capacitor:\[E_{total} = E_1 + E_2 = 0.09 \, J + 0.18 \, J = 0.27 \, J\]
05

Conclusion

The total energy stored in the capacitors is 0.27 joules.

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Key Concepts

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

Understanding Capacitance
Capacitance is a measure of a capacitor's ability to store charge per unit voltage. To put it simply, it's how well the capacitor can store electrical energy. The unit of capacitance is the farad (F), named after the English scientist Michael Faraday. However, typical capacitors in electronic circuits are often measured in microfarads (\(\mu F\)), which are a millionth of a farad.
Capacitors come in various sizes and values. They are used in many applications ranging from smoothing out power fluctuations in power supplies to tuning circuits in radios. Understanding how a capacitor operates helps in configuring them appropriately in circuits.
For instance, in our exercise, a 2.0 \(\mu F\) and a 4.0 \(\mu F\) capacitor are used. When connected, they perform their role in storing energy, measured in joules, which is crucial for functioning of electronic devices.
Connecting Capacitors in Parallel Circuits
In parallel circuits, multiple components are connected across the same voltage source. This means that every component, such as capacitors in this context, experiences the same voltage.
When capacitors are connected in parallel, their total capacitance is simply the sum of their individual capacitances. This increases the ability of the circuit to store more charge.
For example, in our problem, a 2.0 \(\mu F\) capacitor and a 4.0 \(\mu F\) capacitor are arranged in parallel. Their effective capacitance is calculated by adding the two values:
  • Total capacitance = \(2.0 \mu F + 4.0 \mu F = 6.0 \mu F\)
This setup allows us to use the same formula for energy stored across capacitors with a consistent voltage applied across each one.
Voltage in Electrical Circuits
Voltage, or electric potential difference, is the force that pushes electric charges through a conductor. It's a fundamental concept in electricity, indicating how much energy is available to push each unit of charge through the circuit.
  • The unit of voltage is the volt (V).
  • Voltage in many circuits acts like a "pressure" that drives the flow of electrons.
In parallel circuits, each component is exposed to the full voltage of the source.
Using our example, the capacitors are connected to a 300 V source, meaning both experience the same 300 V potential difference. This uniformity simplifies calculations, allowing us to evaluate each capacitor under the same voltage condition, assisting in finding the energy stored as shown in the original problem.
Electric Potential Energy in Capacitors
Electric potential energy is the energy stored in charged particles because of their positions. In the case of capacitors, this energy is stored in the electric field created between their plates when they hold a charge.
The energy stored in a capacitor can be calculated using the formula:
  • \(E = \frac{1}{2} C V^2\)
  • \(E\) is the energy (in joules)
  • \(C\) is the capacitance (in farads)
  • \(V\) is the voltage (in volts)
Each capacitor can independently store energy. For example, in our exercise, the 2.0 \(\mu F\) capacitor stores 0.09 joules and the 4.0 \(\mu F\) stores 0.18 joules when subjected to a 300 V potential difference.
By calculating both separately and summing them, the total energy stored across these parallel-connected capacitors can be established, as shown in the worked solution.

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Most popular questions from this chapter

A \(10 \mathrm{~V}\) battery is connected to a series of \(n\) capacitors, each of capacitance \(2.0 \mu \mathrm{F}\). If the total stored energy is \(25 \mu \mathrm{J}\), what is \(n\) ?

What capacitance is required to store an energy of \(10 \mathrm{~kW} \cdot \mathrm{h}\) at a potential difference of \(1000 \mathrm{~V} ?\)

A potential difference of \(300 \mathrm{~V}\) is applied to a series connection of two capacitors of capacitances \(C_{1}=2.00 \mu \mathrm{F}\) and \(C_{2}=8.00 \mu \mathrm{F}\). What are (a) charge \(q_{1}\) and (b) potential difference \(V_{1}\) on capacitor 1 and (c) \(q_{2}\) and (d) \(V_{2}\) on capacitor 2? The charged capacitors are then disconnected from each other and from the battery. Then the capacitors are reconnected with plates of the same signs wired together (the battery is not used). What now are (e) \(q_{1},(\mathrm{f}) V_{1},(\mathrm{~g}) q_{2}\), and \((\mathrm{h}) V_{2} ?\) Suppose, instead, the capacitors charged in part (a) are reconnected with plates of opposite signs wired together. What now are (i) \(q_{1},(\mathrm{j}) V_{1},(\mathrm{k}) q_{2}\), and \((\mathrm{l}) V_{2} ?\)

A parallel-plate air-filled capacitor having area \(40 \mathrm{~cm}^{2}\) and plate spacing \(1.0 \mathrm{~mm}\) is charged to a potential difference of \(600 \mathrm{~V}\). Find (a) the capacitance, (b) the magnitude of the charge on each plate, (c) the stored energy, (d) the electric field between the plates, and (e) the energy density between the plates.

A parallel-plate capacitor has plates of area \(0.12 \mathrm{~m}^{2}\) and a separation of \(1.2 \mathrm{~cm}\). A battery charges the plates to a potential difference of \(120 \mathrm{~V}\) and is then disconnected. A dielectric slab of thickness \(4.0 \mathrm{~mm}\) and dielectric constant \(4.8\) is then placed symmetrically between the plates. (a) What is the capacitance before the slab is inserted? (b) What is the capacitance with the slab in place? What is the free charge \(q(\mathrm{c})\) before and \((\mathrm{d})\) after the slab is inserted? What is the magnitude of the electric field (e) in the space between the plates and dielectric and (f) in the dielectric itself? (g) With the slab in place, what is the potential difference across the plates? (h) How much external work is involved in inserting the slab?

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