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The resistances of the primary and secondary coils of a transformer are 56 and \(14 \Omega\), respectively. Both coils are made from lengths of the same copper wire. The circular turns of each coil have the same diameter. Find the turns ratio \(N_{\mathrm{s}} / N_{\mathrm{p}}\).

Short Answer

Expert verified
The turns ratio \( \frac{N_{\mathrm{s}}}{N_{\mathrm{p}}} \) is \( \frac{1}{4} \).

Step by step solution

01

Understand the Problem

The problem asks us to find the turns ratio \( N_{\mathrm{s}} / N_{\mathrm{p}} \) of a transformer, given the resistances of its primary and secondary coils. This ratio describes the relationship between the number of wire loops in each coil.
02

Identify the Given Information

We are given that the resistance of the primary coil \( R_{\mathrm{p}} = 56 \Omega \) and the resistance of the secondary coil \( R_{\mathrm{s}} = 14 \Omega \). Both coils use the same type of wire and have circular turns of the same diameter.
03

Recall Relational Formula

The resistance \( R \) of a wire is given by the formula \( R = \rho \frac{L}{A} \), where \( \rho \) is the resistivity, \( L \) is the length, and \( A \) is the cross-sectional area. With identical wire properties, relate resistance to length of wire for both coils.
04

Relate Resistance to Turns

Since the cross-sectional area \( A \) and resistivity \( \rho \) are the same for both coils, the ratio of their resistances will be the same as the ratio of their lengths: \[ \frac{R_{\mathrm{p}}}{R_{\mathrm{s}}} = \frac{L_{\mathrm{p}}}{L_{\mathrm{s}}} \] where \( L_{\mathrm{p}} \) and \( L_{\mathrm{s}} \) are the lengths of the wire in the primary and secondary coils, respectively.
05

Connect Length to Turns Ratio

Since each turn is of the same diameter, the length of the wire is directly proportional to the number of turns. So, \[ \frac{L_{\mathrm{p}}}{L_{\mathrm{s}}} = \frac{N_{\mathrm{p}}}{N_{\mathrm{s}}} \] which means \[ \frac{R_{\mathrm{p}}}{R_{\mathrm{s}}} = \frac{N_{\mathrm{p}}}{N_{\mathrm{s}}} \]
06

Calculate the Turns Ratio

With \( \frac{R_{\mathrm{p}}}{R_{\mathrm{s}}} = \frac{56}{14} = 4 \), we find that \( \frac{N_{\mathrm{p}}}{N_{\mathrm{s}}} = 4 \). Therefore, the turns ratio \( \frac{N_{\mathrm{s}}}{N_{\mathrm{p}}} = \frac{1}{4} \).

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Key Concepts

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

Coil Resistance
Understanding coil resistance is crucial when dealing with transformers. Resistance in a wire is determined by how difficult it is for electricity to flow through it. This depends on several factors including the material's resistivity, the length of the wire, and its cross-sectional area.
In the case of transformers, each coil or winding has its own resistance. Primary and secondary coils often have different resistances because they have different numbers of turns. Resistance can be calculated using the formula \( R = \rho \frac{L}{A} \), where \( \rho \) is the resistivity of the material (copper in this case), \( L \) is the length of the wire, and \( A \) is the cross-sectional area.
For identical wires with the same diameter used in both coils, resistance is directly proportional to the length of the wire. Therefore, if one coil has a higher resistance, it generally has more turns (assuming each turn is the same length). As provided, the primary coil has a resistance of 56 Ω and the secondary 14 Ω, indicating the primary coil has more turns compared to the secondary.
Turns Ratio Calculation
The turns ratio of a transformer helps in determining how the voltage changes from primary to secondary coil. This ratio is the comparison of the number of turns in the primary coil to the number of turns in the secondary coil.
Given that both the primary and secondary coils use the same copper wire, their resistances can provide insight into their respective lengths, and thus, their turns. With \( R = \rho \frac{L}{A} \) and identical materials and design properties, the ratio of the resistances \( \frac{R_{\mathrm{p}}}{R_{\mathrm{s}}} \) is equal to the ratio of their turns \( \frac{N_{\mathrm{p}}}{N_{\mathrm{s}}} \).
For our problem, \( \frac{56}{14} = 4 \). This indicates that the number of turns in the primary coil is four times that in the secondary coil. Hence, the turns ratio \( \frac{N_{\mathrm{s}}}{N_{\mathrm{p}}} \) becomes \( \frac{1}{4} \), meaning the primary has 4 times more loops compared to the secondary.
Copper Wire Properties
Copper is widely used in electrical wiring due to its excellent conductivity and favorable physical properties. Key properties of copper that make it ideal for transformer coils include:
  • High Conductivity: Copper's high ability to conduct electricity reduces energy loss due to resistance, making it efficient for transferring electricity in coils.
  • Low Resistivity: The low resistivity of copper means it can carry more current across longer distances without heating up excessively, which is crucial in maintaining transformer efficiency.
  • Ductility: Copper can be easily drawn into thin wires, necessary for winding the numerous turns in transformer coils.
  • Thermal Conductivity: Effective thermal conductivity helps in dissipating heat generated by electrical resistance within the coils, thus preventing overheating.

These properties ensure that transformers can efficiently step up or step down voltage levels with minimal energy loss. In the problem, even though the resistance differed between coils, both coils benefited from using copper, ensuring reliable electrical performance.

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Most popular questions from this chapter

A circular coil \((950\) turns, radius \(=0.060 \mathrm{~m})\) is rotating in a uniform magnetic field. At \(t=0 \mathrm{~s}\), the normal to the coil is per pendicular to the magnetic field. At \(t=0.010 \mathrm{~s}\) the normal makes an angle of \(\phi=45^{\circ}\) with the field because the coil has made oneeighth of a revolution. An average emf of magnitude \(0.065 \mathrm{~V}\) is induced in the coil. Find the magnitude of the magnetic field at the location of the coil.

In 1996 , NASA performed an experiment called the Tethered Satellite experiment. In this experiment a \(2.0 \times 10^{4}-\mathrm{m}\) length of wire was let out by the space shuttle Atlantis to generate a motional emf. The shuttle had an orbital speed of \(7.6 \times 10^{3} \mathrm{~m} / \mathrm{s},\) and the magnitude of the earth's magnetic field at the location of the wire was \(5.1 \times 10^{-5} \mathrm{~T}\). If the wire had moved perpendicular to the earth's magnetic field, what would have been the motional emf generated between the ends of the wire?

Interactive LearningWare 22.2 at reviews the fundamental approach in problems such as this. A constant magnetic field passes through a single rectangular loop whose dimensions are \(0.35 \mathrm{~m} \times 0.55 \mathrm{~m}\). The magnetic field has a magnitude of \(2.1 \mathrm{~T}\) and is inclined at an angle of \(65^{\circ}\) with respect to the normal to the plane of the loop. (a) If the magnetic field decreases to zero in a time of \(0.45 \mathrm{~s}\), what is the magnitude of the average emf induced in the loop? (b) If the magnetic field remains constant at its initial value of \(2.1 \mathrm{~T},\) what is the magnitude of the rate \(\Delta \mathrm{A} / \Delta t\) at which the area should change so that the average emf has the same magnitude as in part (a)?

A standard door into a house rotates about a vertical axis through one side, as defined by the door's hinges. A uniform magnetic field is parallel to the ground and perpendicular to this axis. Through what angle must the door rotate so that the magnetic flux that passes through it decreases from its maximum value to one-third of its maximum value?

A vacuum cleaner is plugged into a \(120.0\) -V socket and uses \(3.0\) A of current in normal operation when the back emf generated by the electric motor is \(72.0 \mathrm{~V}\). Find the coil resistance of the motor.

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