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(a) When a \(9.00-\mathrm{V}\) battery is connected to the plates of a capacitor, it stores a charge of \(27.0 \mu \mathrm{C}\). What is the value of the capacitance? (b) If the same capacitor is connected to a \(12.0-\mathrm{V}\) battery, what charge is stored?

Short Answer

Expert verified
The capacitance of the capacitor is \(3.00 \times 10^{-6} F\) and the charge stored when a 12.0V battery is connected is \(36.0 \mu C\).

Step by step solution

01

Calculate the Capacitance

The formula to calculate the capacitance \(C\) of a capacitor is \(C = \frac{Q}{V}\), where \(Q\) is the charge stored on the capacitor and \(V\) is the voltage across it. Substituting the given values (Q=27.0 μC and V=9.0 V) into the formula gives \(C = \frac{27.0 \times 10^{-6} C}{9.0V} = 3.00 \times 10^{-6}F\).
02

Calculate the stored charge

Now we'll calculate the charge stored when the same capacitor is connected to a 12.0V battery. We'll use the formula \(Q = CV\) and substitute the values (C=3.00 × 10^-6 F and V=12.0V) into the formula to calculate the new charge which gives \(Q = 3.00 × 10^{-6} F × 12.0V = 36.0 \mu C\).

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Key Concepts

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

Capacitor Charge Relationship
The relationship between the charge stored in a capacitor and the voltage across it is foundational to understanding how capacitors work. To put it simply, capacitance is the property that defines a capacitor's ability to store charge. This relationship is described by the equation \( C = \frac{Q}{V} \), where \( C \) represents the capacitance, \( Q \) the charge, and \( V \) the voltage.

Imagine you have a tiny bucket (the capacitor) that can hold a certain amount of water (the charge). The size of the bucket represents its capacitance—the larger the bucket, the more water it can hold. However, the amount of water (charge) that actually goes into the bucket depends on the water pressure (voltage) you use to fill it. More pressure means more water gets in, up to the bucket's capacity. Therefore, with higher voltage, a capacitor can store more charge, provided it has the capacity (capacitance) to do so.

Looking at the given exercise, a battery voltage of \(9.00-\text{V}\) enables the capacitor to store \(27.0 \text{ }\text{μC}\) of charge. If the voltage were different, so too would be the charge stored, as long as the capacitance remains unchanged. This is crucial when designing circuits because it informs what voltage source is needed for a desired charge storage.
Voltage and Capacitance
Voltage and capacitance are like two sides of a coin in the realm of electronics; they are interdependent. Capacitance, measured in Farads (F), is an intrinsic property of a capacitor and does not change when the voltage changes, as long as the physical structure of the capacitor remains intact.

The voltage, on the other hand, is an external factor applied to the capacitor. It's the electrical potential difference between the two plates of the capacitor and is what 'pushes' the charge into the capacitor. The higher the voltage applied to the capacitor, the greater the charge it will hold, until the maximum capacity determined by its capacitance is reached.

To deepen our understanding, let's revisit the exercise. Initially, with a \(9.00-\text{V}\) battery, the calculated capacitance was \(3.00 \times 10^{-6}\text{F}\) (or 3.00 μF). This capacitance remains constant. When we later connect it to a \(12.0-\text{V}\) battery, the capacitor can store more charge due to the increased voltage, but the ratio of charge to voltage (the capacitance) stays the same. This is an essential concept for students working on their homework, ensuring they understand that capacitance is a measure of potential charge storage capacity at a particular voltage and does not vary with the voltage itself.
Stored Charge in Capacitors
The amount of charge a capacitor can store is not just a theoretical concept; it has real-world implications in electronic devices. Think of charge as the 'energy currency' that a capacitor can provide to a circuit. It varies depending on both the capacitance and the voltage applied to the capacitor. This storage is possible due to the electric field created between the two plates of the capacitor when a voltage is applied.

In the exercise provided, we begin with a known voltage and charge to find the capacitance. Then, using this constant capacitance, we can determine the new amount of stored charge for a different voltage. The ability to calculate this is incredibly useful for designing circuits with specific power needs or for troubleshooting when things don't work as expected.

For instance, if we have a flashlight powered by capacitors, knowing the stored charge helps us to estimate how long the flashlight might work before needing a recharge. In summary, the understanding of how much charge can be stored in capacitors, under varying voltages, allows students to grasp the potential and limitations of capacitors in various applications. Enhancing problem-solving exercises with these practical examples can significantly improve the comprehension of such abstract concepts.

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Most popular questions from this chapter

Two capacitors give an equivalent capacitance of \(9.00 \mathrm{pF}\) when connected in parallel and an equivalent capacitance of \(2.00 \mathrm{pF}\) when connected in series. What is the capacitance of each capacitor?

A \(25.0-\mu \mathrm{F}\) capacitor and a \(40.0-\mu \mathrm{F}\) capacitor are charged by being connected across separate \(50.0-\mathrm{V}\) batteries. (a) Determine the resulting charge on each capacitor. (b) The capacitors are then disconnected from their batteries and connected to each other, with each negative plate connected to the other positive plate. What is the final charge of each capacitor, and what is the final potential difference across the \(40.0-\mu \mathrm{F}\) capacitor?

Three parallel-plate capacitors are constructed, each having the same plate area \(A\) and with \(C_{1}\) having plate spacing \(d_{1}, C_{2}\) having plate spacing \(d_{2}\), and \(C_{g}\) having plate spacing \(d_{3}\). Show that the total capacitance \(C\) of the three capacitors connected in series is the same as a capacitor of plate area \(A\) and with plate spacing \(d=d_{1}+d_{2}+d_{3}\).

A proton is located at the origin, and a second proton is located on the \(x\) -axis at \(x=6.00 \mathrm{fm}\left(1 \mathrm{fm}=10^{-15} \mathrm{~m}\right)\). (a) Calculate the electric potential energy associated with this configuration. (b) An alpha particle (charge \(=2 e\), mass \(=6.64 \times 10^{-27} \mathrm{~kg}\) ) is now placed at \((x, y)=(3.00\) 3.00) fm. Calculate the electric potential energy associated with this configuration. (c) Starting with the three particle system, find the change in electric potential energy if the alpha particle is allowed to escape to infinity while the two protons remain fixed in place. (Throughout, neglect any radiation effects.) (d) Use conservation of energy to calculate the speed of the alpha particle at infinity. (e) If the two protons are released from rest and the alpha particle remains fixed, calculate the speed of the protons at infinity,

A certain storm cloud has a potential difference of \(1.00 \times 10^{8}\) V relative to a tree. If, during a lightning storm, \(50.0\) C of charge is transferred through this potential difference and \(1.00 \%\) of the energy is absorbed by the tree, how much water (sap in the tree) initially at \(30.0^{\circ} \mathrm{C}\) can be boiled away? Water has a specific heat of \(4186 \mathrm{~J} / \mathrm{kg}^{\circ} \mathrm{C}\), a boiling point of \(100^{\circ} \mathrm{C}\), and a heat of vaporization of \(2.26 \times 10^{6} \mathrm{~J} / \mathrm{kg}\)

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