A water heater consisting of a metal coil that is connected across the terminals of a 15 -V power supply is able to heat \(250 \mathrm{~mL}\) of water from room temperature to boiling point in \(45 \mathrm{~s}\). What is the resistance of the coil?

Short Answer

Expert verified
Answer: The resistance of the metal coil in the water heater is approximately 0.121 Ω.

Step by step solution

01

Identify given information

We are given the following information: - Power supply voltage (V): 15 V - Volume of water being heated (V_water): 250 mL = 0.25 L - Time taken to heat water to boiling point (t): 45 s
02

Calculate the heat energy required

To find the heat energy needed to raise the water from room temperature to boiling point, we can use the formula for heat energy (Q): \(Q = mc\Delta T\) where, - Mass (m) can be calculated by multiplying the volume of water with its density, so for water, \(m = V_{water} \times \rho\), with \(\rho = 1000 \frac{kg}{m^3}\) - Specific heat capacity of water (c): 4186 J/kg·K - Temperature change (\(\Delta T\)): This is an estimation, as we do not know the exact room temperature. We can assume that the average room temperature is around 20°C and boiling point at 100°C, so the temperature change (\(\Delta T\)) is approximately 80°C. First, we calculate the mass of water: \(m = 0.25 \frac {L} {1 m^3} \times 1000 \frac {kg} {m^3}= 0.25 kg\) Now, we can calculate the heat energy required (Q): \(Q = (0.25 kg)(4186 \frac{J}{kg \cdot K})(80 K) = 83720 J\)
03

Calculate the electrical power

The heat energy we found is equal to the electrical energy supplied by the power supply. So we can use the formula for electrical power (P) to find the electrical power of the water heater: \(P = \frac{Q}{t}\) where t is the time taken to heat the water. \(P = \frac{83720 \mathrm{~J}}{45 \mathrm{~s}} = 1860 \mathrm{~W}\)
04

Apply Ohm's law and find the resistance

Using Ohm's law, we can find the current (I): \(I = \frac{P}{V}\) \(I = \frac{1860 \mathrm{~W}}{15 \mathrm{~V}} = 124 \mathrm{~A}\) Now applying Ohm's law once again, we can get the resistance (R): \(R = \frac{V}{I}\) \(R = \frac{15 \mathrm{~V}}{124 \mathrm{~A}} = 0.121 \Omega\) The resistance of the coil is approximately 0.121 \(\Omega\).

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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 \(\vec{J}\). (This is the precise form of Ohm's Law.) Suppose in some material an electric field, \(\vec{E}\), produces current density, \(\vec{J},\) 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 \(\vec{E}\) and \(\vec{J}\) related via Ohm's Law, that is, in an ohmic material with conductivity \(\sigma\) or resistivity \(\rho .\)

Ohm's Law states that the potential difference across a device is equal to a) the current flowing through the device times the resistance of the device. b) the current flowing through the device divided by the resistance of the device. c) the resistance of the device divided by the current flowing through the device. d) the current flowing through the device times the crosssectional area of the device. e) the current flowing through the device times the length of the device.

A light bulb is connected to a source of emf. There is a \(6.20 \mathrm{~V}\) drop across the light bulb, and a current of 4.1 A flowing through the light bulb. a) What is the resistance of the light bulb? b) A second light bulb, identical to the first, is connected in series with the first bulb. The potential drop across the bulbs is now \(6.29 \mathrm{~V},\) and the current through the bulbs is \(2.9 \mathrm{~A}\). Calculate the resistance of each light bulb. c) Why are your answers to parts (a) and (b) not the same?

A \(12.0 \mathrm{~V}\) battery with an internal resistance \(R_{\mathrm{j}}=4.00 \Omega\) is attached across an external resistor of resistance \(R\). Find the maximum power that can be delivered to the resistor.

Show that the power supplied to the circuit in the figure by the battery with internal resistance is maximum when the resistance of the resistor in the circuit, \(R\), is equal to \(R_{i}\). Determine the power supplied to \(R\). For practice, calculate the power dissipated by a \(12.0-\mathrm{V}\) battery with an internal resistance of \(2.00 \Omega\) when \(R=1.00 \Omega, R=2.00 \Omega,\) and \(R=3.00 \Omega\)

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