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A 1.00 -m-diameter mirror focuses the Sun's rays onto an absorbing plate \(2.00 \mathrm{cm}\) in radius, which holds a can containing \(1.00 \mathrm{L}\) of water at \(20.0^{\circ} \mathrm{C}\) (a) If the solar intensity is \(1.00 \mathrm{kW} / \mathrm{m}^{2},\) what is the intensity on the absorbing plate? (b) What are the maximum magnitudes of the fields \(\mathbf{E}\) and \(\mathbf{B} ?\) (c) If \(40.0 \%\) of the energy is absorbed, how long does it take to bring the water to its boiling point?

Short Answer

Expert verified
The intensity on the absorbing plate is a value derived from the ratio of the areas of the absorbing plate to the mirror, multiplied by the solar intensity. The maximum magnitudes of the electric and magnetic fields are calculated on the basis of the Poynting vector. Lastly, the time required to heat up the volume of water to its boiling point is determined based on the energy needed and the effective power available, considering only 40% energy absorption.

Step by step solution

01

Calculate the Intensity on the Absorbing Plate

The intensity \(I_{sun}\) of the sunlight is given as 1.00 kW/m². This intensity is focused onto an absorbing plate that has a smaller area than the original diameter of the sunlight. The ratio of the area of the absorbing plate \(A_{absorb} = \pi (0.02)^2 m²\) to that of the mirror \(A_{mirror} = \pi (0.5)^2 m² \), multiplied by the intensity of sunlight, will provide the intensity on the absorbing plate \(I_{absorb}\). Hence, \( I_{absorb} = I_{sun} * (A_{absorb}/A_{mirror}) \).
02

Calculate Maximum Magnitudes of Electric and Magnetic Fields

The relationship between intensity \(I\) and the maximum values of electric field \(E_{max}\) and magnetic field \(B_{max}\) can be described by the Poynting vector. Using the formula \(I = \frac{1}{2} c \epsilon_0 E_{max}^2\) for electric field and \(B_{max} = E_{max}/c\) for magnetic field wherein \(c\) is the speed of light and \(\epsilon_0\) is the permittivity of free space, the maximum magnitudes can be calculated.
03

Calculate the Time Required to Heat Water to its Boiling Point

First, the energy required to heat up the water from 20°C to 100°C (boiling point) needs to be calculated using the formula \(Q = mc(T_{final} - T_{initial})\), where \(m\) is the mass of the water, \(c\) is the specific heat capacity, and \(T_{final}\) and \( T_{initial}\) are the final and initial temperatures, respectively. Then, as 40% of the solar energy is absorbed, the effective power is \(P_{effective} = 40% * I_{absorb} * A_{absorb}\). The time \(t\) required to heat the water can then be calculated with the formula \(t = Q / P_{effective}\).

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Key Concepts

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

Intensity of Sunlight
Where does the heat in your hot chocolate or your warming tea come from? Often, it's the energy from the Sun, a vast nuclear reactor in the sky. The intensity of sunlight is a measure of the power the Sun delivers to a specific area, such as a square meter of the Earth's surface. Think of it as the solar energy budget for each tiny patch of the Earth.

In our exercise, the sunlight's intensity is given as 1.00 kW/m², or 1.00 kilowatts of energy per square meter, a value that's quite typical for a sunny day. This energy gets concentrated when we use a mirror to focus it onto an absorbing plate, which happens in many solar-powered devices. The absorber's size matters a lot: if it's smaller than the reflective surface, like in our problem, it means all that solar goodness gets packed into a tighter space, ramping up the intensity and making the resulting hot spot hotter than a chili pepper!
Poynting Vector
Ok, so what's the big deal with the Poynting vector, aside from its quirky name? It might sound like some obscure concept, but it's quite the VIP in the world of physics. This is a mathematical wizard that shows you the flow of electromagnetic energy through a given area. It's a bit like a traffic cop for energy, directing the where and how much of power transfer.

To understand the punch packed by electric and magnetic fields, we deploy the Poynting vector. It's expressed as the cross product of the electric field vector and the magnetic field vector. Without getting tangled in any heavy math, just know that for this problem, the Poynting vector helps us link the sunlight's intensity to the maximum strength of the electric and magnetic fields. Think of electric and magnetic fields as two dancers in a salsa of light; the Poynting vector sets the rhythm for their dance, which directly relates to how intense or soft the light is.
Specific Heat Capacity
Ever wonder why it takes an eternity for the ocean to warm up, yet your morning coffee turns cold in no time? That's where specific heat capacity plays a starring role in our everyday lives. It's the amount of heat energy required to raise the temperature of a substance by one degree Celsius. Different substances play by different rules; water, our understated hero, holds a ton of heat without breaking much of a sweat, hence why it's great at keeping things warm.

In our scenario, water's specific heat capacity is our golden ticket to understanding how much energy is needed to turn tepid tap water into a rolling boil. The specific heat capacity tells us that water doesn't give up easily; it takes a lot of energy to get those water molecules dancing fast enough to reach the boiling point. And that energy comes from our focused sunlight. By calculating the amount of energy absorbed and the specific heat capacity of water, we can predict how long it will take for our can of water to start bubbling away.

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Most popular questions from this chapter

One goal of the Russian space program is to illuminate dark northern cities with sunlight reflected to Earth from a \(200-\mathrm{m}\) diameter mirrored surface in orbit. Several smaller prototypes have already been constructed and put into orbit. (a) Assume that sunlight with intensity \(1340 \mathrm{W} / \mathrm{m}^{2}\) falls on the mirror nearly perpendicularly and that the atmosphere of the Earth allows \(74.6 \%\) of the energy of sunlight to pass through it in clear weather. What is the power received by a city when the space mirror is reflecting light to it? (b) The plan is for the reflected sunlight to cover a circle of diameter \(8.00 \mathrm{km} .\) What is the intensity of light (the average magnitude of the Poynting vector) received by the city? (c) This intensity is what percentage of the vertical component of sunlight at Saint Petersburg in January, when the sun reaches an angle of \(7.00^{\circ}\) above the horizon at noon?

Consider a small, spherical particle of radius \(r\) located in space a distance \(R\) from the Sun. (a) Show that the ratio \(F_{\mathrm{rad}} / F_{\mathrm{grav}}\) is proportional to \(1 / r,\) where \(F_{\mathrm{rad}}\) is the force exerted by solar radiation and \(F_{\mathrm{grav}}\) is the force of gravitational attraction. (b) The result of part (a) means that, for a sufficiently small value of \(r,\) the force exerted on the particle by solar radiation exceeds the force of gravitational attraction. Calculate the value of \(r\) for which the particle is in equilibrium under the two forces. (Assume that the particle has a perfectly absorbing surface and a mass density of \(1.50 \mathrm{g} / \mathrm{cm}^{3} .\) Let the particle be located \(3.75 \times 10^{11} \mathrm{m}\) from the Sun, and use \(214 \mathrm{W} / \mathrm{m}^{2}\) as the value of the solar intensity at that point.)

An astronaut, stranded in space \(10.0 \mathrm{m}\) from his spacecraft and at rest relative to it, has a mass (including equipment) of 110 kg. Because he has a \(100-W\) light source that forms a directed beam, he considers using the beam as a photon rocket to propel himself continuously toward the spacecraft. (a) Calculate how long it takes him to reach the spacecraft by this method. (b) What If? Suppose, instead, that he decides to throw the light source away in a direction opposite the spacecraft. If the mass of the light source is \(3.00 \mathrm{kg}\) and, after being thrown, it moves at \(12.0 \mathrm{m} / \mathrm{s}\) relative to the recoiling astronaut, how long does it take for the astronaut to reach the spacecraft?

An electromagnetic wave in vacuum has an electric field amplitude of \(220 \mathrm{V} / \mathrm{m} .\) Calculate the amplitude of the corresponding magnetic field.

Two radio-transmitting antennas are separated by half the broadcast wavelength and are driven in phase with each other. In which directions are (a) the strongest and (b) the weakest signals radiated?

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