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A metal wire of resistance \(R\) is cut into three equal pieces that are then connected side by side to form a new wire the length of which is equal to one- third the original length. What is the resistance of this new wire?

Short Answer

Expert verified
The resistance of the new wire is \(R/9\), where \(R\) is the original resistance of the wire.

Step by step solution

01

Identify the relevant principles

The concept crucial to solving the problem is Ohm's law, which describes the relationship between resistance (\(R\)), resistivity (\(蟻\)), length (\(L\)) and cross-sectional area (\(A\)). It's expressed as \(R = 蟻 * (L/A)\).
02

Break down the changes to the wire

When the wire is cut into three equal pieces and reconnected side by side, two properties of the wire change. The length of each piece becomes \(L/3\) and since they are connected side by side, the total cross sectional area is three times the original, i.e., \(3A\).
03

Calculate the new resistance

Substitute the new values into Ohm's Law. The new resistance \(R'\) is equal to \( 蟻 * ((L/3) / 3A)\). Since \(蟻\) and \(L\) are constants, this simplifies to \(R' = (蟻 * L / 9A) = R/9\), where \(R\) is the original resistance of the wire.

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Key Concepts

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

Electrical Resistance
Resistance is a fundamental concept in the field of electronics and electrical engineering. It indicates how much a material opposes the flow of electric current. Think of it like a constriction in a water hose that makes it harder for water to pass through. In electrical terms, this constriction is the resistance, and the water would be the electric current.

It's measured in Ohms (), and the higher the resistance, the more difficult it is for the current to flow, much like a narrower hose would restrict water flow more than a wider one. This is crucial because it helps to understand why different materials conduct electricity better than others and how this changes power consumption in electrical circuits.

The metal wire exercise demonstrates how resistance changes when the configuration of the wire changes. By cutting and rearranging the wire, we've altered the 'hose' 鈥 our wire 鈥 and by understanding resistance, we can predict how these changes affect current flow. It's essential to grasp that resistance is not just an inherent property of the material, but also depends on the shape and size of the conductor.
Resistivity
Resistivity is often compared to resistance but these concepts, while related, are not the same. Resistivity, designated by the symbol ), is a material-specific property that quantifies how strongly a material opposes the flow of electric current. In essence, resistivity is the 'DNA' of the material, determining its ability to conduct electricity regardless of size and shape of the material.

Ohm's law, which involves both resistance and resistivity, gives us a clearer picture. The formula ) incorporates both these elements and highlights that while resistance depends on the size and shape of the material (length ) and cross-sectional area )), resistivity is a constant for a specific material under certain temperature conditions. It鈥檚 crucial to note that temperature can affect resistivity, typically increasing it in metals as the temperature rises.

In the context of the exercise, resistivity stays constant when the metal wire is cut and reconfigured, but the resistance changes due to the new shape and size. Understanding resistivity is vital because it is a primary factor that dictates the resistance of a conductor in a particular environment.
Series and Parallel Circuits
When discussing electrical circuits, two basic ways to connect components are in series and in parallel. A series circuit is like a single-track path where every part of the path must be followed in sequence, with the same current flowing through all components. On the other hand, a parallel circuit is like having multiple pathways for the current to travel through.

Components in series share the same current but the total resistance is the sum of individual resistances, as the paths are consecutive. However, for parallel circuits, while the voltage across each component is the same, the total resistance is not simply the sum because the current can divide and take multiple paths. The total resistance of parallel components is always less than the smallest individual resistance, a concept evident in our exercise with the metal wire.

By cutting and reconfiguring the wire into three side-by-side pieces, we've created an example of a parallel circuit. Each segment has one-third the original length and when placed in parallel, the combined resistance of the wire decreases to one-ninth of the original. This highlights the dramatic effect of circuit configuration on resistance and is crucial for designing circuits with the desired electrical properties.

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Most popular questions from this chapter

Suppose that the current through a conductor decreases exponentially with time according to the equation \(I(t)=I_{0} e^{-t / \tau}\) where \(I_{0}\) is the initial current (at \(t=0),\) and \(\tau\) is a constant having dimensions of time. Consider a fixed observation point within the conductor. (a) How much charge passes this point between \(t=0\) and \(i=\pi^{2}\) (b) How much charge passes this point between \(t=0\) and \(t=10 \tau ?\) (c) What If? How much charge passes this point between \(t=0\) and \(t=\infty ?\)

A close analogy exists between the flow of energy by heat because of a temperature difference (see Section 20.7 ) and the flow of electric charge because of a potential difference. The energy \(d Q\) and the electric charge \(d q\) can both be transported by free electrons in the conducting material. Consequently, a good electrical conductor is usually a good thermal conductor as well. Consider a thin conducting slab of thickness \(d x,\) area \(A,\) and electrical conductivity \(\sigma,\) with a potential difference \(d V\) between opposite faces. Show that the current \(I=d q / d t\) is given by the equation on the left below: Charge Conduction\(\frac{d q}{d t}=\sigma A\left|\frac{d V}{d x}\right|\) Thermal Conduction \((E q, 20.14)$$\frac{d Q}{d t}=k A\left|\frac{d T}{d x}\right|\) In the analogous thermal conduction equation on the right, the rate of energy flow dQ/de (in SI units of joules per second) is due to a temperature gradient \(d T / d x,\) in a material of thermal conductivity \(k .\) State analogous rules relating the direction of the electric current to the change in potential, and relating the direction of energy flow to the change in temperature.

A straight cylindrical wire lying along the \(x\) axis has a length \(L\) and a diameter \(d\). It is made of a material that obeys Ohm's law with a resistivity \(\rho .\) Assume that potential \(V\) is maintained at \(x=0,\) and that the potential is zero at \(x=L .\) In terms of \(L, d, V, \rho,\) and physical constants, derive expressions for (a) the electric field in the wire, (b) the resistance of the wire, (c) the electric current in the wire, and (d) the current density in the wire. Express vectors in vector notation. (e) Prove that \(\mathbf{E}=\rho \mathbf{J}\).

A conductor of uniform radius \(1.20 \mathrm{cm}\) carries a current of 3.00 A produced by an electric field of \(120 \mathrm{V} / \mathrm{m} .\) What is the resistivity of the material?

A small sphere that carrics a charge \(q\) is whirled in a circle at the end of an insulating string. The angular frequency of rotation is \(\omega .\) What average current does this rotating charge represent?

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