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Two inductors are connected in parallel across the terminals of a generator. One has an inductance of \(L_{1}=0.030 \mathrm{H},\) and the other has an inductance of \(L_{2}=0.060 \mathrm{H.}\) A single inductor, with an inductance \(L,\) is connected across the terminals of a second generator that has the same frequency and voltage as the first one. The current delivered by the second generator is equal to the total current delivered by the first generator. Find \(L\)

Short Answer

Expert verified
The equivalent inductance is approximately 0.020 H.

Step by step solution

01

Understanding the Problem

We have two inductors connected in parallel, and we need to find the equivalent inductance such that a single inductor with this equivalent inductance draws the same current as the combination of the two parallel inductors.
02

Formula for Parallel Inductors

For inductors in parallel, the total inductance \(L_t\) can be calculated using the formula: \[ \frac{1}{L_t} = \frac{1}{L_1} + \frac{1}{L_2} \] where \(L_1 = 0.030 \, H\) and \(L_2 = 0.060 \, H\).
03

Substitute Values

Substitute the given inductance values into the formula: \[ \frac{1}{L_t} = \frac{1}{0.030} + \frac{1}{0.060} \] Calculate each term on the right side of the equation.
04

Calculate Individual Terms

Calculate the values: \[ \frac{1}{0.030} = 33.33 \quad \text{and} \quad \frac{1}{0.060} = 16.67 \]
05

Calculate Total Inductance

Add the two calculated values: \[ \frac{1}{L_t} = 33.33 + 16.67 = 50.00 \] Therefore, \[ L_t = \frac{1}{50.00} \approx 0.020 \, H \]
06

Solution

The equivalent inductance \(L\) across the second generator terminals is equal to \(L_t\), which is approximately \(0.020 \, H\).

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Key Concepts

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

Equivalent Inductance
When dealing with electrical circuits, understanding equivalence is crucial. The equivalent inductance of a system simplifies complex networks of inductors into a single inductor that has the same magnetic and electrical properties as the system it represents. In a parallel configuration, the total magnetic effect is distributed across several inductors.To find the equivalent inductance for inductors in parallel, like in the given problem, we use a formula similar to calculating resistors in parallel, just reversed. For two inductors with inductances \(L_1\) and \(L_2\), their total or equivalent inductance \(L_t\) is found using:\[ \frac{1}{L_t} = \frac{1}{L_1} + \frac{1}{L_2} \]This formula allows for the calculation of a single inductance value that represents the combined effect of the two parallel inductors. This calculation is essential in designing circuits and ensuring energy efficiency. Once we understand how to calculate the equivalent inductance, we can simplify complex circuit analyses.
Inductance Calculation
Calculating inductance, especially for parallel inductors, is crucial in electrical engineering and physics. In this scenario, we substitute known values of \(L_1 = 0.030 \mathrm{H}\) and \(L_2 = 0.060 \mathrm{H}\) into the formula for parallel inductance:\[ \frac{1}{L_t} = \frac{1}{0.030} + \frac{1}{0.060} \]Breaking it down:- Convert each inductance value into its reciprocal: - \( \frac{1}{0.030} = 33.33 \) - \( \frac{1}{0.060} = 16.67 \)- Add these reciprocals to find the total: \[ 33.33 + 16.67 = 50.00 \] Finally, find the reciprocal of the sum to determine the equivalent inductance:\[ L_t = \frac{1}{50.00} \approx 0.020 \mathrm{H} \]This process highlights the core principles of solving parallel inductor problems, where effectively handling the reciprocals is key.
Step-by-Step Physics Problem
Approaching a physics problem step-by-step ensures clarity and accuracy. The approach taken in the solution simplifies a potentially complex topic into manageable steps.
  • Step 1 involved understanding what the problem is asking, which is crucial for finding the right path forward.
  • Step 2 introduced the necessary formula, which serves as the mathematical foundation for solving the problem.
  • Step 3 to Step 5 encompassed the substitution of known values and calculation of results, which translates theory into practical application.
  • Finally, Step 6 concluded by delivering the final answer, tying the solution back to the physical scenario.
Such a structured method not only resolves this particular problem but builds a useful analytical procedure for approaching various physics exercises. These steps embody a logical pathway that helps ensure that nothing is missed and each part of the problem is addressed systematically. This methodical breakdown into easily digestible parts encourages a deeper understanding and solid foundation for solving more advanced physics problems.

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Most popular questions from this chapter

Part \(a\) of the figure shows a heterodyne metal detector being used. As part \(b\) of the figure illustrates, this device utilizes two capacitor/ inductor oscillator circuits, A and B. Each produces its own resonant frequency, \(f_{0 A}=1 /\left[2 \pi\left(L_{A} C\right)^{1 / 2}\right]\) and \(f_{0 B}=1 /\left[2 \pi\left(L_{B} C\right)^{1 / 2}\right] .\) Any difference between these frequencies is detected through earphones as a beat frequency \(\left|f_{0 B}-f_{0 A}\right| \cdot\) In the absence of any nearby metal object, the inductances \(L_{\mathrm{A}}\) and \(L_{\mathrm{B}}\) are identical. When inductor \(\mathrm{B}\) (the search coil) comes near a piece of metal, the inductance \(L_{\mathrm{B}}\) increases, the corresponding oscillator frequency \(f_{0 \mathrm{B}}\) decreases, and a beat frequency is heard. Suppose that initially each inductor is adjusted so that \(L_{\mathrm{B}}=L_{\mathrm{A}},\) and each oscillator has a resonant frequency of \(855.5 \mathrm{kHz}\). Assuming that the inductance of search coil \(\mathrm{B}\) increases by \(1.000 \%\) due to a nearby piece of metal, determine the beat frequency heard through the earphones.

The reactance of a capacitor is \(68 \Omega\) when the ac frequency is 460 Hz. What is the reactance when the frequency is \(870 \mathrm{Hz} ?\)

In the absence of a nearby metal object, the two inductances \(\left(L_{\mathrm{A}}\right.\) and \(\left.L_{\mathrm{B}}\right)\) in a heterodyne metal detector are the same, and the resonant frequencies of the two oscillator circuits have the same value of \(630.0 \mathrm{kHz} .\) When the search coil (inductor \(\mathrm{B}\) ) is brought near a buried metal object, a beat frequency of \(7.30 \mathrm{kHz}\) is heard. By what percentage does the buried object increase the inductance of the search coil?

An ac series circuit has an impedance of \(192 \Omega\), and the phase angle between the current and the voltage of the generator is \(\phi=-75^{\circ} .\) The circuit contains a resistor and either a capacitor or an inductor. Find the resistance \(R\) and the capacitive reactance \(X_{\mathrm{C}}\) or the inductive reactance \(X_{\mathrm{L}},\) whichever is appropriate.

Two parallel plate capacitors are filled with the same dielectric material and have the same plate area. However, the plate separation of capacitor 1 is twice that of capacitor 2 . When capacitor 1 is connected across the terminals of an ac generator, the generator delivers an rms current of 0.60 A. Concepts: (i) Which of the two capacitors has the greater capacitance? (ii) Is the equivalent capacitance of the parallel combination \(\left(C_{\mathrm{P}}\right)\) greater or smaller than the capacitance of capacitor \(1 ?\) (iii) Is the capacitive reactance of \(C_{\mathrm{P}}\) greater or smaller than for \(C_{1} ?\) (iv) When both capacitors are connected in parallel across the terminals of the generator, is the current from the generator greater or smaller than when capacitor 1 is connected alone? Calculations: What is the current delivered by the generator when both capacitors are connected in parallel across the terminals?

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