/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 34 Find the equivalent capacitance ... [FREE SOLUTION] | 91Ó°ÊÓ

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Find the equivalent capacitance of a \(4.20-\mu \mathrm{F}\) capacitor and an \(8.50-\mu \mathrm{F}\) capacitor when they are connected (a) in series and (b) in parallel.

Short Answer

Expert verified
The equivalent capacitance of the capacitors when connected in series is calculated using the reciprocal formula and when connected in parallel is equal to the sum of the individual capacitances.

Step by step solution

01

Understand the concept

When capacitors are connected in series or parallel, their total or equivalent capacitance changes. The total capacitance (\(C_{t}\)) of capacitors in series is given by the formula \(\frac{1}{C_{t}} = \frac{1}{C_{1}} + \frac{1}{C_{2}} + ... + \frac{1}{C_{n}}\). When capacitors are connected in parallel, the total capacitance is the sum of the individual capacitances: \(C_{t} = C_{1} + C_{2} + ... + C_{n}\).
02

Calculate the equivalent capacitance in series

Using the formula for capacitors in series, the equivalent capacitance for the \(4.20-\mu \mathrm{F}\) capacitor and \(8.50-\mu \mathrm{F}\) capacitor can be calculated as: \(\frac{1}{C_{t}} = \frac{1}{4.20} + \frac{1}{8.50}\) Solving this will give the value of \(C_{t}\) for the capacitors in series.
03

Calculate the equivalent capacitance in parallel

Now using the formula for capacitors in parallel, the equivalent capacitance for the \(4.20-\mu \mathrm{F}\) capacitor and \(8.50-\mu \mathrm{F}\) capacitor can be calculated as: \(C_{t} = 4.20 + 8.50\) which will give the value of \(C_{t}\) for the capacitors in parallel.
04

Conclusion

The solution to the problem is the equivalent capacitance in microfarads when the capacitors are connected in series and in parallel

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Key Concepts

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

Capacitors in Series
When trying to understand the behavior of capacitors in series, envision a row of water bottles connected by thin tubes at their bases. The electrical charge is akin to water, and the thin tubes represent the limited flow between each bottle (capacitor). Here's the key: the total capacity for charge storage is restricted by the smallest tube (capacitor).

In formulas, we express the total capacitance (\(C_{t}\)) of a series connection using the reciprocal sum: \[ \frac{1}{C_{t}} = \frac{1}{C_{1}} + \frac{1}{C_{2}} + ... + \frac{1}{C_{n}} \. \]This can be challenging if you're new to it, but once you understand that the overall ability to store charge is lessened by the 'constriction' of having to pass through each capacitor, it becomes more intuitive. Even if one capacitor is gigantic (high capacitance), a small one in series sets the limit for the entire chain.
Capacitors in Parallel
On the flip side, capacitors in parallel work more like a series of water containers with wide openings—each connected to a common big basin. The overall water storage capacity? Just add up the volume of all the containers.

For capacitors, this means the total capacitance (\(C_{t}\)) is simply the sum of all individual capacitances: \[ C_{t} = C_{1} + C_{2} + ... + C_{n} \. \] Honestly, it's much like joining forces; every capacitor contributes its full storage ability to the system. No blockages here—instead, they team up to create a bigger storage 'reservoir' for electrical charge.
Capacitance Calculation
So, how do we actually calculate these values? Let's dig into the exercise. Assume we are working with an elementary circuit of two capacitors, one rated at \(4.20-\mu \mathrm{F}\) and the other at \(8.50-\mu \mathrm{F}\).

For series setup, the calculation is a tad more intricate because we can't just add the capacitances. Remember those formulas mentioned before? They’re your best friends here. Plugging in our specific values, the series capacitance calculation looks like this: \[ \frac{1}{C_{t}} = \frac{1}{4.20} + \frac{1}{8.50} \. \]In contrast, when these buddies are in parallel, it's a straight addition \[ C_{t} = 4.20 + 8.50 \. \] Simplification and standard algebra apply from this point to obtain the final values. But don't forget units—maintaining the microfarads throughout is crucial.
Electrical Circuits
But where do capacitors fit into electrical circuits? Think of an electrical circuit as a city road map where the roads are wires and the traffic is the current. Various components like capacitors are akin to buildings and landmarks—each plays a unique role in the flow and control of traffic.

Capacitors, specifically, can store and release electrical energy, behaving somewhat like rubber speed bumps that can release the stored energy when needed. This capability is vital in smoothing out energy supply, filtering out noise, or in timing applications within electronic devices. They’re essential in everything from the flash of your camera to smoothing out the power supply in your computer’s complex circuitry.

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Most popular questions from this chapter

Capacitors \(C_{1}=6.0 \mu \mathrm{F}\) and \(C_{2}=2.0 \mu \mathrm{F}\) are charged as a parallel combination across a \(250-V\) battery. The capacitors are disconnected from the battery and from each other. They are then connected positive plate to negative plate and negative plate to positive plate. Calculate the resulting charge on each capacitor.

On planet Tehar, the free-fall acceleration is the same as that on the Earth, but there is also a strong downward electric field that is uniform close to the planet's surface. A \(2.00-\mathrm{kg}\) ball having a charge of \(5.00 \mu \mathrm{C}\) is thrown upward at a speed of \(20.1 \mathrm{~m} / \mathrm{s}\). It hits the ground after an interval of \(4.10 \mathrm{~s}\). What is the potential difference between the starting point and the top point of the trajectory?

Two capacitors, \(C_{1}=18.0 \mu \mathrm{F}\) and \(C_{2}=36.0 \mu \mathrm{F}\), are connected in series, and a \(12.0-\mathrm{V}\) battery is connected across them. (a) Find the equivalent capacitance, and the energy contained in this equivalent capacitor. (b) Find the energy stored in each individual capacitor. Show that the sum of these two energies is the same as the energy found in part (a). Will this equality always be true, or does it depend on the number of capacitors and their capacitances? (c) If the same capacitors were connected in parallel, what potential difference would be required across them so that the combination stores the same energy as in part (a)? Which capacitor stores more energy in this situation, \(C_{1}\) or \(C_{2} ?\)

Four point charges each having charge Qare located at the corners of a square having sides of length \(a\). Find symbolic expressions for (a) the total electric potential at the center of the square due to the four charges and (b) the work required to bring a fifth charge \(q\) from infinity to the center of the square.

Metal sphere A of radius \(12.0 \mathrm{~cm}\) carries \(6.00 \mu \mathrm{C}\) of charge, and metal sphere \(\mathrm{B}\) of radius \(18.0 \mathrm{~cm}\) carries \(-4.00 \mu \mathrm{C}\) of charge. If the two spheres are attached by a very long conducting thread, what is the final distribution of charge on the two spheres?

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