The tip of a flashlight bulb is touching the top of a 3 V battery as shown in Figure Q23. l. Does the bulb light? Why or why not?
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Textbook Solutions for College Physics: A Strategic Approach
Question
A real battery is not just an emf. We can model a real 1.5 V battery as a 1.5 V emf in series with a resistor known as the "internal resistance," as shown in Figure P23.55. A typical battery has 1.0 fl internal resistance due to imperfections that limit current through the battery. When there's no voltage drop across the internal resistance, the potential difference between its terminals is 1.5 V, the value of the emf. Suppose the terminals of this battery are connected to a 2.0 fl resistor.a. What is the potential difference between the terminals of the battery? b. What fraction of the battery's power is dissipated by the internal resistance.
Solution
The first step in solving 23 problem number 55 trying to solve the problem we have to refer to the textbook question: A real battery is not just an emf. We can model a real 1.5 V battery as a 1.5 V emf in series with a resistor known as the "internal resistance," as shown in Figure P23.55. A typical battery has 1.0 fl internal resistance due to imperfections that limit current through the battery. When there's no voltage drop across the internal resistance, the potential difference between its terminals is 1.5 V, the value of the emf. Suppose the terminals of this battery are connected to a 2.0 fl resistor.a. What is the potential difference between the terminals of the battery? b. What fraction of the battery's power is dissipated by the internal resistance.
From the textbook chapter Circuits you will find a few key concepts needed to solve this.
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