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Two identical light bulbs are connected to a battery. Will the light bulbs be brighter if they are connected in series or in parallel?

Short Answer

Expert verified
Answer: The light bulbs will be brighter when connected in parallel.

Step by step solution

01

Calculate Current and Voltage in Series Connection

When the light bulbs are connected in series, the total resistance (R_total) is the sum of their individual resistances (R), i.e., R_total = 2R. Since the battery provides a constant voltage (V), we can use Ohm's law (V = I * R) to find the total current (I_total) in the circuit. In this case, I_total = V / (2R).
02

Calculate Current and Voltage in Parallel Connection

When the light bulbs are connected in parallel, the total resistance (R_total) in the circuit is given by the formula (1/R_total) = (1/R) + (1/R). Solving for R_total, we find that R_total = R/2. Again, using Ohm's law, we can find the total current (I_total) in the circuit. In this case, I_total = V / (R/2) = 2V / R.
03

Calculate Power (Brightness) in Series Connection

The power (P) of a light bulb is directly related to its brightness and can be calculated using the formula P = I^2 * R. Since the bulbs are identical, they have the same resistance and current through them in series connection. Therefore, the power of each light bulb in series connection is P_series = I_total^2 * R = (V^2 / (4R^2)) * R = V^2 / (4R).
04

Calculate Power (Brightness) in Parallel Connection

For the parallel connection, we'll find the power of each bulb again using P = I^2 * R. However, in a parallel connection, the voltage across each bulb is the same as the battery voltage, and the currents through each bulb are equal (since they have the same resistance) and sum up to the total current (I_total). That means the current through each bulb is I_parallel = I_total / 2 = (2V / R) / 2 = V / R. The power of each light bulb in parallel connection is P_parallel = I_parallel^2 * R = (V^2 / R^2) * R = V^2 / R.
05

Compare Brightness in Series and Parallel Connection

Now, let's compare the brightness (power) of the bulbs in series and parallel connection. We have P_series = V^2 / (4R) and P_parallel = V^2 / R. Since P_parallel > P_series, the light bulbs will be brighter when connected in parallel compared to when they are connected in series.

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Key Concepts

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

Ohm's Law
Ohm's Law is a fundamental principle in electrical engineering that relates voltage (\( V \)), current (\( I \)), and resistance (\( R \) in a circuit. It's presented as the simple equation \( V = I \times R \). This equation tells us that the current flowing through a conductor between two points is directly proportional to the voltage across the two points, assuming the temperature remains constant. The resistance in the circuit acts as the proportionality constant.

When applying Ohm's Law to solve for the brightness of bulbs in a circuit, as in the textbook exercise, it's crucial to understand how altering the resistance—whether by arranging bulbs in series or parallel—affects the current. In a series connection, resistances add up which increases the total resistance, hence reducing the current. Conversely, in a parallel connection, resistances
Electrical Resistance
Electrical resistance is a measure of the opposition to the flow of electric current. It's what determines how much current will flow through the circuit for a given voltage, following Ohm's Law. Resistance is measured in ohms (\( \(\Omega \) \).

In the context of the textbook exercise, when bulbs are placed in series, the total resistance increases as each bulb adds its own resistance to the circuit. Therefore, \( R_{\text{total}} = R_1 + R_2 + ... + R_n \), where \( R_i \) is the resistance of the \( i^{\text{th}} \) bulb. However, when bulbs are arranged in parallel, the total resistance is less than any individual resistance and can be calculated using the formula \( 1/R_{\text{total}} = 1/R_1 + 1/R_2 + ... + 1/R_n \). This decreased resistance leads to a higher current for a given voltage, based on Ohm's Law.
Circuit Brightness
Circuit brightness is a term often used to describe the luminous efficacy of a circuit component, like a light bulb. It is largely dependent on the electrical power (\( P \) consumed by the bulb, where \( P = I^2 \times R \) or \( P = V \times I \), depending on which values are known. Brightness, in this sense, is a practical way of visualizing power. The greater the power dissipated by a bulb, the brighter it will shine.

From the step-by-step solution provided, we understand that the bulbs in a parallel circuit are brighter than those in a series circuit. This conclusion aligns with the calculation of power in each configuration: in a series circuit, the power is divided among the components, while in a parallel circuit, each bulb can draw power equivalent to being directly connected to the voltage source. Therefore, due to the higher power drawn in parallel, each light bulb exhibits greater brightness.
Power Calculation in Circuits
Power calculation in circuits is crucial for understanding the workload, or electrical energy consumption, of circuit components per unit time. Measured in watts (\( W \), power in an electrical circuit is given by \( P = V \times I \), where \( V \) is voltage and \( I \) is current. Another useful form, especially for resistive loads like incandescent light bulbs, derives from Ohm's Law: \( P = I^2 \times R \) or \( P = V^2 / R \.

Applying these formulas to our exercise, for bulbs connected in series, power is dissipated over a greater resistance, which results in less power per bulb and correspondingly, less brightness. For bulbs in parallel, each has the full circuit voltage across it and operates at a power level as if alone in the circuit. Consequently, light bulbs in parallel shine brighter, which is evident when comparing \( P_{\text{parallel}} \) to \( P_{\text{series}} \). This is an important consideration for real-world applications where the distribution of power affects the performance and functionality of electrical devices.

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Most popular questions from this chapter

A material is said to be ohmic if an electric field, \(\vec{E}\), in the material gives rise to current density \(\vec{J}=\sigma \vec{E},\) where the conductivity, \(\sigma\) is a constant independent of \(\vec{E}\) or \(\bar{J}\). (This is the precise form of Ohm's Law, ) Suppose in some material an electric field, \(\vec{E}\), produces current density, \(\bar{J},\) not necessarily related by Ohm's Law; that is, the material may or may not be ohmic. a) Calculate the rate of energy dissipation (sometimes called ohmic heating or joule heating) per unit volume in this material, in terms of \(\vec{E}\) and \(\vec{J}\). b) Express the result of part (a) in terms of \(\vec{E}\) alone and \(\vec{J}\) alone, for \(\overrightarrow{\boldsymbol{E}}\) and \(\vec{J}\) related via Ohm's Law, that is, in an ohmic material with conductivity \(\sigma\) or resistivity \(\rho\).

When a battery is connected to a \(100 .-\Omega\) resistor, the current is 4.00 A. When the same battery is connected to a \(400 .-\Omega\) resistor, the current is \(1.01 \mathrm{~A}\). Find the emf supplied by the battery and the internal resistance of the battery.

What would happen to the drift velocity of electrons in a wire if the resistance due to collisions between the electrons and the atoms in the crystal lattice of the metal disappeared?

What is the current density in an aluminum wire having a radius of \(1.00 \mathrm{~mm}\) and carrying a current of \(1.00 \mathrm{~mA}\) ? What is the drift speed of the electrons carrying this current? The density of aluminum is \(2.70 \cdot 10^{3} \mathrm{~kg} / \mathrm{m}^{3}\), and 1 mole of aluminum has a mass of 26.98 g. There is one conduction electron per atom in aluminum.

The most common material used for sandpaper, silicon carbide, is also widely used in electrical applications, One common device is a tubular resistor made of a special grade of silicon carbide called carborundum. A particular carborundum resistor (see the figure) consists of a thick-walled cylindrical shell (a pipe) of inner radius \(a=1.50 \mathrm{~cm},\) outer radius \(b=2.50 \mathrm{~cm},\) and length \(L=60.0 \mathrm{~cm}\). The resistance of this carborundum resistor at \(20.0^{\circ} \mathrm{C}\) is \(1.00 \mathrm{f}\). a) Calculate the resistivity of carborundum at room temperature, Compare this to the resistivities of the most commonly used conductors (copper, aluminum, and silver). b) Carborundum has a high temperature coefficient of resistivity: \(\alpha=2.14 \cdot 10^{-3} \mathrm{~K}^{-1}\). If, in a particular application, the carborundum resistor heats up to \(300 .{ }^{\circ} \mathrm{C}\), what is the percentage change in its resistance between room temperature \(\left(20.0^{\circ} \mathrm{C}\right)\) and this operating temperature?

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