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The single-loop circuit shown in the figure has \(V_{e m f, 1}=16.37 \mathrm{~V}\) \(V_{\text {emf } 2}=10.81 \mathrm{~V},\) and \(R_{1}=24.65 \Omega\). The current flowing in the circuit is 0.1600 A. What is the resistance \(R_{2} ?\)

Short Answer

Expert verified
Answer: The resistance R_2 in the given circuit is 10.1 Ω.

Step by step solution

01

Write down Kirchhoff's loop rule formula

Kirchhoff's loop rule states that the sum of the voltage changes around a closed loop must be equal to zero. Therefore, we can write the equation: \(V_{emf_1} - I\cdot R_1 - V_{emf_2} - I\cdot R_2 = 0\) where \(I\) is the current flowing in the circuit.
02

Plug in the known values

We are given the following values: \(V_{emf_1} = 16.37 V\), \(V_{emf_2} = 10.81 V\), \(R_1 = 24.65 \Omega\), and \(I = 0.1600 A\). Plug these values into the equation from Step 1: \(16.37 - 0.1600 \cdot 24.65 - 10.81 - 0.1600 \cdot R_2 = 0\)
03

Solve the equation for \(R_2\)

Simplify and rearrange the equation from Step 2 to solve for \(R_2\): \(16.37 - 3.944 - 10.81 - 0.1600 \cdot R_2 = 0\) \(1.616 = 0.1600 \cdot R_2\) Now, we can divide both sides of the equation by 0.1600 to get the value of \(R_2\): \(R_2 = \frac{1.616}{0.1600}\) \(R_2 = 10.1 \Omega\) So, the resistance \(R_2\) is equal to 10.1 \(\Omega\).

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Key Concepts

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

Electrical Circuits
At the heart of our modern life lies the essential concept of electrical circuits, which can be visualized as the bloodstream of any electrical device. An electrical circuit is essentially a closed loop through which electric charges can flow. The significance of such circuits cannot be overstated, as they underpin every electronic device we use, from the simplest children's toy to the most complex supercomputer.

To comprehend the behavior and function of an electrical circuit, several elements must be considered. These include the power source (like batteries or generators), which creates a potential difference to push electrons through the circuit. Then, we have conducting wires that act as pathways, and components like resistors, capacitors, and transistors, which control the flow and manage the energy in the circuit. The versatility of circuits is immense, allowing them to manage energy in a multitude of ways, performing tasks such as amplifying signals, computing data, or simply lighting a bulb.

When encountering circuits in theory or practice, we also approach various terminologies and laws, such as Kirchhoff's Rules, which empower students and professionals to predict and calculate the behavior of these circuits with astonishing accuracy.
Voltage and Current
The movement of electric charges in a circuit is described by two fundamental concepts: voltage and current. To paint an analogy, imagine water flowing through pipes; voltage is akin to the water pressure that propels the water through the pipes, while current would be the flow rate of that water.

Specifically, voltage (\( V \)), also known as electric potential difference, is the force that pushes electric charges along a conductor. The higher the voltage, the greater the

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Most popular questions from this chapter

Kirchhoff's Junction Rule states that a) the algebraic sum of the currents at any junction in a circuit must be zero. b) the algebraic sum of the potential changes around any closed loop in a circuit must be zero. c) the current in a circuit with a resistor and a capacitor varies exponentially with time. d) the current at a junction is given by the product of the resistance and the capacitance. e) the time for the current development at a junction is given by the product of the resistance and the capacitance.

A \(15.19-\mathrm{mF}\) capacitor is fully charged using a battery that supplies \(V_{\text {emf }}=131.1 \mathrm{~V}\). The battery is disconnected, and a \(616.5-\Omega\) resistor is connected across the capacitor. What current will be flowing through the resistor after 3.871 s?

A \(19.79-\mathrm{mF}\) capacitor is fully charged using a battery. The battery is disconnected, and a \(693.5-\Omega\) resistor is connected across the capacitor. The current flowing through the resistor after \(6.615 \mathrm{~s}\) is \(0.1203 \mathrm{~A} .\) What is the emf supplied by the battery?

In the movie Back to the Future, time travel is made possible by a flux capacitor, which generates 1.21 GW of power. Assuming that a 1.00 - \(F\) capacitor is charged to its maximum capacity with a \(12.0-\mathrm{V}\) car battery and is discharged through a resistor, what resistance is necessary to produce a peak power output of \(1.21 \mathrm{GW}\) in the resistor? How long would it take for a \(12.0-\mathrm{V}\) car battery to charge the capacitor to \(90.0 \%\) of its maximum capacity through this resistor?

How long will it take, as a multiple of the time constant, \(\tau,\) for the capacitor in an RC circuit to be \(98 \%\) charged? a) \(9 \tau\) c) \(90 \tau\) e) \(0.98 \tau\) b) \(0.9 \tau\) d) \(4 \tau\)

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