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Two resistors with resistances \(R_{1}\) and \(R_{2}\) are connected in parallel. Demonstrate that, no matter what the actual values of \(R_{1}\) and \(R_{2}\) are, the equivalent resistance is always less than the smaller of the two resistances,

Short Answer

Expert verified
Prove your answer. Answer: Yes, the equivalent resistance in a parallel circuit with two resistors is always less than the smaller resistance. This can be proved using the formula for equivalent resistance in a parallel connection, \(R_{eq} = \frac{R_{1}R_{2}}{R_{1}+R_{2}}\). By assuming \(R_1 \leq R_2\) and rearranging the inequality, we get \(0 < R_{1}^2\), which always holds true as the square of a resistance (a positive value) is greater than zero.

Step by step solution

01

Formula for equivalent resistance of parallel resistors

In a parallel circuit, the equivalent resistance \(R_{eq}\) can be calculated using the following formula: \[\frac{1}{R_{eq}} = \frac{1}{R_{1}} + \frac{1}{R_{2}}\]
02

Rewrite the formula and solve for \(R_{eq}\)

We will rewrite the formula to express the equivalent resistance \(R_{eq}\) in terms of the individual resistances \(R_1\) and \(R_2\). To achieve this, let's add the fractions on the right side and solve for \(R_{eq}\): \[\frac{1}{R_{eq}} = \frac{R_{1}+R_{2}}{R_{1}R_{2}}\] Now, to obtain \(R_{eq}\), we will take the reciprocal of both sides of the equation: \[R_{eq} = \frac{R_{1}R_{2}}{R_{1}+R_{2}}\]
03

Prove that \(R_{eq}\) is always less than the smaller resistance

With our present equation, we will show that \(R_{eq}\) is less than the smaller of the two resistances, \(R_1\) and \(R_2\). Without loss of generality, let us assume that \(R_1 \leq R_2\). The inequality we want to prove is: \[R_{eq} = \frac{R_{1}R_{2}}{R_{1}+R_{2}} < R_{1}\] We will take a cross-multiplication approach to simplify and rearrange the inequality: \[R_{1}R_{2} < R_{1}(R_{1} + R_{2})\] Now, let's distribute \(R_{1}\) to the terms in the parentheses on the right side of the inequality: \[R_{1}R_{2} < R_{1}^2 + R_{1}R_{2}\] Subtracting \(R_{1}R_{2}\) from both sides of the inequality gives: \[0 < R_{1}^2\] Since it is always true that the square of a resistance (a positive value) is greater than zero, the inequality holds, and we have demonstrated that, no matter the actual values of \(R_{1}\) and \(R_{2}\), the equivalent resistance in a parallel connection is always less than the smaller of the two resistances.

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Key Concepts

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

Resistance in Parallel
When dealing with resistance in parallel circuits, it is crucial to understand how they differ from series circuits. In a parallel configuration, multiple paths for the current are created as each resistor is connected separately to the voltage source. This setup influences the total resistance in a way that might seem counterintuitive at first: the combined resistance drops.

To calculate the equivalent resistance (\(R_{eq}\)) of two such resistors, we use the formula: \[\frac{1}{R_{eq}} = \frac{1}{R_{1}} + \frac{1}{R_{2}}\]. By finding a common denominator and adding these fractions, it becomes apparent why \(R_{eq}\) is always lower than either \(R_{1}\) or \(R_{2}\), especially the smallest of them. The simultaneous paths allow electrons to flow more easily compared to having to pass through either resistance alone, which is similar to opening more lanes on a highway; traffic flows better, resulting in lower overall resistance.
Ohm's Law
Ohm’s law is a foundational principle used in circuit analysis. It states a direct proportionality between the voltage across a conductor and the current through it, provided the temperature remains constant. Mathematically, Ohm's law is expressed as \( V = IR \), where \(V\) is the voltage, \(I\) the current, and \(R\) the resistance.

This principle is instrumental when analyzing parallel circuits, as it helps determine the current distribution across the resistors. When coupled with the formula for equivalent resistance, it becomes a powerful tool to analyze various aspects of a circuit, such as voltage drops and power consumption, ensuring each component's operation is understood and effectively predicted.
Circuit Analysis
Circuit analysis is a systematic approach to understanding the behaviors and relationships within an electrical circuit. By applying various principles, such as Ohm’s law and Kirchhoff’s laws, one can deduce how current, voltage, and resistance interact in complex networks.

When finding equivalent resistance in parallel circuits, circuit analysis involves a set of steps that begins with identifying all parallel relationships and then applying the relevant formulas to simplify the circuit to its basics. The goal of such simplification is to create a manageable number of components that can correctly represent the original circuit's behavior. By doing so, predictions can be made about system responses to changes, and optimal designs for desired electrical behavior can be achieved.
Electrical Resistance
Electrical resistance is a measure of the opposition to the flow of electric current within a conductor. The unit of resistance is the ohm, symbolized by \(\Omega\). Essentially, electrical resistance quantifies how much a material reduces the current flow, acting somewhat like a choke point.

Materials with high resistance, such as rubber and glass, are called insulators because they impede the flow of electrons. Conversely, conductors have low resistance and allow current to flow easily. Integrity of materials, temperature, and physical dimensions all impact resistance. Through careful material selection and circuit design, engineers control the amount of resistance in a circuit to safeguard components, manage energy consumption, and ensure stability and efficiency of the electrical system.

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Most popular questions from this chapter

Two conductors are made of the same material and have the same length \(L\). Conductor \(A\) is a hollow tube with inside diameter \(2.00 \mathrm{~mm}\) and outside diameter \(3.00 \mathrm{~mm}\); conductor \(\mathrm{B}\) is a solid wire with radius \(R_{\mathrm{B}}\). What value of \(R_{n}\) is required for the two conductors to have the same resistance measured between their ends?

A 34-gauge copper wire \(\left(A=0.0201 \mathrm{~mm}^{2}\right),\) with a constant potential difference of \(0.100 \mathrm{~V}\) applied across its \(1.00 \mathrm{~m}\) length at room temperature \(\left(20.0^{\circ} \mathrm{C}\right),\) is cooled to liquid nitrogen temperature \(\left(77 \mathrm{~K}=-196^{\circ} \mathrm{C}\right)\) a) Determine the percentage change in the wire's resistance during the drop in temperature. b) Determine the percentage change in current flowing in the wire. c) Compare the drift speeds of the electrons at the two temperatures.

How much money will a homeowner owe an electric company if he turns on a \(100.00-\mathrm{W}\) incandescent light bulb and leaves it on for an entire year? (Assume that the cost of electricity is \(\$ 0.12000 / \mathrm{kWh}\) and that the light bulb lasts that long.) The same amount of light can be provided by a 26.000 - W compact fluorescent light bulb. What would it cost the home owner to leave one of those on for a year?

You make a parallel connection between two resistors, resistor \(A\) having a very large resistance and resistor B having a very small resistance. The equivalent resistance for this combination will be a) slightly greater than the resistance of resistor A. b) slightly less than the resistance of resistor A. c) slightly greater than the resistance of resistor B. d) slightly less than the resistance of resistor B.

In an emergency, you need to run a radio that uses \(30.0 \mathrm{~W}\) of power when attached to a \(10.0-\mathrm{V}\) power supply. The only power supply you have access to provides \(25.0 \mathrm{kV}\), but you do have a large number of \(25.0-\Omega\) resistors. If you want the power to the radio to be as close as possible to \(30.0 \mathrm{~W}\), how many resistors should you use, and how should they be connected (in series or in parallel)?

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