/*! 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 15 The current in a single-loop cir... [FREE SOLUTION] | 91Ó°ÊÓ

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The current in a single-loop circuit with one resistance \(R\) is \(5.0 \mathrm{~A}\). When an additional resistance of \(2.0 \Omega\) is inserted in series with \(R\), the current drops to \(4.0 \mathrm{~A}\). What is \(R ?\)

Short Answer

Expert verified
The resistance \( R \) is \( 8.0 \Omega \).

Step by step solution

01

Understand Ohm's Law

Ohm's Law tells us that the voltage across an entire circuit is equal to the current flowing through the circuit times the resistance of the circuit. This can be represented mathematically as \( V = I \times R \). In this step, we prepare to use this formula to represent the circuits described in the problem.
02

Apply Ohm's Law to the Initial Circuit

For the initial circuit, we know that the current \( I \) is \( 5.0 \text{ A} \). The equation can be written as \( V = 5.0 \times R \), where \( V \) is the voltage and \( R \) is the resistance we are trying to find.
03

Apply Ohm's Law to the Modified Circuit

When an additional resistance of \( 2.0 \Omega \) is added in series, the current drops to \( 4.0 \text{ A} \). The new equation for the circuit becomes \( V = 4.0 \times (R + 2.0) \). This accounts for the total resistance of the circuit now being \( R + 2.0 \Omega \).
04

Equate the Two Expressions for Voltage

Since the voltage \( V \) in both scenarios is the same, we can equate the expressions from steps 2 and 3: \( 5.0R = 4.0(R + 2.0) \). This new equation helps us to solve for \( R \) by setting the two expressions for voltage equal to each other.
05

Simplify and Solve for R

Start by expanding the equation: \( 5.0R = 4.0R + 8.0 \). To solve for \( R \), subtract \( 4.0R \) from both sides to get \( 1.0R = 8.0 \). Thus, \( R = 8.0 \Omega \).

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Key Concepts

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

Single-loop circuit
In a single-loop circuit, the components are connected end-to-end in a single path. This means the current has only one path to travel through all components in the circuit. For instance, imagine a simple circuit with a battery and just one resistor connected in a loop. The current flows from the positive side of the battery, through the resistor, and back to the negative side of the battery.

A unique aspect of a single-loop circuit is that the current remains the same at all points within the loop because there are no junctions or multiple paths for the current to split. In the context of the given problem, understanding that the circuit is a single loop helps simplify calculations and assure that the same current moves through all resistors. Keep in mind:
  • Current is a consistent value around the loop.
  • The total voltage supplied by the battery is used across the total resistance in the loop.
Series Resistance
Resistors in a circuit can be arranged in series or parallel configurations.When resistors are arranged in series, they are connected end-to-end, just like beads on a string.In this problem, an additional resistor is added in series with an existing one, meaning:

  • The total resistance is simply the sum of the individual resistances.
  • The same current flows through each resistor in the series.
For example, if you start with one resistor with a resistance of \(R\) and add another resistor of \(2.0 \Omega\), the total resistance becomes \(R + 2.0 \Omega\).

The concept of series resistance is crucial when assessing how the total resistance affects the current in the circuit.The increase in total resistance is directly linked to the current drop, which is highlighted in the given problem when comparing the initial and modified circuits.
Current Drop
The current drop is a key factor in a circuit when you add more resistance.It refers to the decrease in current flow through the circuit as resistance increases.Ohm's Law tells us that \( V = I \times R \).Keeping the voltage constant, if the total resistance increases, the current must decrease.

In this problem, initially, with just one resistor \(R\), the current is \(5.0 \text{ A}\).When another \(2.0 \Omega\) resistor is added in series, the current drops to \(4.0 \text{ A}\).This drop in current signifies the increase in resistance after adding the additional resistor.Remember:
  • More resistance leads to less current if the voltage stays the same.
  • The current drop helps in calculating the original resistance \(R\) using Ohm's Law equations.
Voltage Equality
Voltage equality refers to the fact that in a closed circuit, the total voltage supplied must equal the sum of the voltage drops across all components.When analyzing circuits like the one in this exercise, understanding this principle is key to ensuring the correct application of Ohm's Law in both scenarios described.

For both the initial and modified circuits, the supply voltage remains constant. By equating the expressions that represent the voltage in both situations, we can effectively solve for the unknown resistance \(R\). Following the steps outlined in the problem:
  • For the initial circuit: \( V = 5.0 \times R \)
  • For the modified circuit: \( V = 4.0 \times (R + 2.0) \)
By setting these equal to each other (because voltage is consistent in a single-source circuit), we can solve for \(R\) and uncover the resistor's value.

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Most popular questions from this chapter

Suppose that, while you are sitting in a chair, charge separation between your clothing and the chair puts you at a potential of \(200 \mathrm{~V}\), with the capacitance between you and the chair at \(150 \mathrm{pF}\). When you stand up, the increased separation between your body and the chair decreases the capacitance to \(10 \mathrm{pF}\). (a) What then is the potential of your body? That potential is reduced over time, as the charge on you drains through your body and shoes (you are a capacitor discharging through a resistance). Assume that the resistance along that route is \(300 \mathrm{G} \Omega\). If you touch an electrical component while your potential is greater than \(100 \mathrm{~V}\), you could ruin the component. (b) How long must you wait until your potential reaches the safe level of \(100 \mathrm{~V}\) ? If you wear a conducting wrist strap that is connected to ground, your potential does not increase as much when you stand up; you also discharge more rapidly because the resistance through the grounding connection is much less than through your body and shoes. (c) Suppose that when you stand up, your potential is \(1400 \mathrm{~V}\) and the chair-to-you capacitance is \(10 \mathrm{pF}\). What resistance in that wrist-strap grounding connection will allow you to discharge to \(100 \mathrm{~V}\) in \(0.30 \mathrm{~s}\), which is less time than vou would need to reach for, say, your computer?

A group of \(N\) identical batteries of \(\operatorname{emf} \mathscr{E}\) and internal resistance \(r\) may be connected all in series (Fig. \(27-80 a\) ) or all in parallel (Fig. \(27-80 b\) ) and then across a resistor \(R\). Show that both arrangements give the same current in \(R\) if \(R=r\).

A 10 -km-long underground cable extends east to west and consists of two parallel wires, each of which has resistance 13 \(\Omega / \mathrm{km} .\) An electrical short develops at distance \(x\) from the west end when a conducting path of resistance \(R\) connects the wires (Fig. 27 31). The resistance of the wires and the short is then \(100 \Omega\) when measured from the east end and \(200 \Omega\) when measured from the west end. What are (a) \(x\) and (b) \(R\) ?

Two resistors \(R_{1}\) and \(R_{2}\) may be connected either in series or in parallel across an ideal battery with emf \(\mathscr{E}\). We desire the rate of energy dissipation of the parallel combination to be five times that of the series combination. If \(R_{1}=100 \Omega\), what are the (a) smaller and (b) larger of the two values of \(R_{2}\) that result in that dissipation rate?

Two identical batteries of emf \(\mathscr{E}=12.0\) \(V\) and internal resistance \(r=0.200 \Omega\) are to be connected to an external resistance \(R\), either in parallel (Fig. \(27-50\) ) or in series (Fig. 27-51). If \(R=2.00 r\), what is the current \(i\) in the external resistance in the (a) parallel and (b) series arrangements? (c) For which arrangement is \(i\) greater? If \(R=r / 2.00\), what is \(i\) in the external resistance in the (d) parallel and (e) series arrangements? (f) For which arrangement is \(i\) greater now?

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