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Size of a Light-Bulb Filament. The operating temperature of a tungsten filament in an incandescent light bulb is \(2450 \mathrm{~K},\) and its emissivity is \(0.350 .\) Find the surface area of the filament of a \(150 \mathrm{~W}\) bulb if all the electrical energy consumed by the bulb is radiated by the filament as electromagnetic waves. (Only a fraction of the radiation appears as visible light.)

Short Answer

Expert verified
The size of the filament of a 150 W bulb is approximately 0.00192 m², considering all the electrical energy being radiated as electromagnetic waves.

Step by step solution

01

Understand the given values

In this exercise, the power \(P = 150\) W, the temperature \(T = 2450\) K, and the emissivity \(e = 0.350\). It is known that the Stefan-Boltzmann constant \(\sigma = 5.670367(13) × 10^{-8} W m^{-2} K^{-4}\). Our goal is to find the surface area of the filament (A).
02

Use the Stefan-Boltzmann law

The Stefan-Boltzmann law is represented as \(P = e \sigma A T^{4}\). We need to solve this equation for A.
03

Rearrange the Stefan-Boltzmann law

Rearranging the equation to find A, we get \(A = \frac{P}{e \sigma T^{4}}\).
04

Substitute the given values into the equation for A

Substitute the given values into the equation for \(A\): \(A = \frac{150 W}{0.350 × 5.670367(13) × 10^{-8} W m^{-2} K^{-4} × (2450 K)^{4}}\).
05

Evaluate the equation

Solve the equation to obtain the value of A.

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Key Concepts

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

Thermal Radiation
Thermal radiation is a form of energy emitted by an object which is due to the object’s temperature. This process is a type of electromagnetic radiation and follows the principles of thermodynamics. An everyday example of thermal radiation is the warmth felt from the sun or a fireplace. Unlike conduction and convection, thermal radiation does not require a medium to transfer heat; it can occur in a vacuum.

Every object at a temperature above absolute zero emits this type of radiation. The amount of radiation emitted depends on the surface temperature of the object and its ability to emit thermal radiation, which is characterized by a property called emissivity. Importantly, thermal radiation encompasses all wavelengths of light, not just visible light, and is therefore broader than what our eyes can detect.

An interesting application of these principles can be seen in the operation of an incandescent light bulb. The filament inside the bulb gets heated to high temperatures, and while it does emit some visible light, a large portion of the energy is emitted as infrared radiation, which is a component of thermal radiation.
Physical Properties of Light
Light is a fascinating and complex phenomenon with both wave-like and particle-like properties, a duality captured in quantum mechanics. Light is a form of electromagnetic radiation and can be categorized by its wavelength or frequency. The light that we can see is only a small segment of the electromagnetic spectrum, which includes radio waves, microwaves, infrared radiation, ultraviolet rays, X-rays, and gamma rays.

In the context of thermal radiation, light behaves according to Planck's law, which expresses the spectral distribution of electromagnetic radiation emitted by a black body in thermal equilibrium at a definite temperature. The spectrum of thermal radiation is smooth and continuous, with the peak of the spectrum shifting to shorter wavelengths as the temperature increases – a phenomenon described by Wien's displacement law.

Emissivity and its Role in Light Emission

In terms of emission, the emissivity of a material affects how well it emits light as a form of energy. Materials with high emissivity are efficient at emitting radiation, whereas materials with low emissivity, such as metallic surfaces, are less efficient and reflect more radiation.

The visible light emitted by the filament in a light bulb is a result of the thermal radiation process, where the filament's temperature dictates the color and intensity of the emitted light. Hence, understanding the physical properties of light is crucial when analyzing phenomena like the operation of light bulbs and energy consumption.
Emissivity of Materials
Emissivity is a measure of a material's ability to emit thermal radiation compared to an ideal black body, which is a theoretical object that perfectly absorbs and emits all wavelengths of thermal radiation. The emissivity of a material can range from 0 to 1, with 1 indicating that the material is a perfect emitter and 0 signifying that it reflects all radiation.

Materials with high emissivity, such as non-metals and dark-colored surfaces, emit thermal radiation efficiently. Low emissivity materials, like shiny metals, tend to reflect radiation, making them good thermal insulators. In practical applications, the concept of emissivity is crucial for controlling heating and cooling processes, designing energy-efficient buildings, and in our case, understanding the energy distribution of a light bulb.

When considering the textbook exercise where a light bulb filament's surface area is to be determined, the emissivity has a direct impact on the calculation. Since the filament of an incandescent light bulb emits electromagnetic waves, its emissivity must be accounted for in the Stefan-Boltzmann law to accurately determine how much energy is radiated as heat instead of light. This highlights the importance of considering the emissivity of materials when calculating thermal radiation for practical applications.

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Most popular questions from this chapter

An unknown liquid has density \(\rho\) and coefficient of volume expansion \(\beta\). A quantity of heat \(Q\) is added to a volume \(V\) of the liquid, and the volume of the liquid increases by an amount \(\Delta V\). There is no phase change. In terms of these quantities, what is the specific heat capacity \(c\) of the liquid?

Consider a poor lost soul walking at \(5 \mathrm{~km} / \mathrm{h}\) on a hot day in the desert, wearing only a bathing suit. This person's skin temperature tends to rise due to four mechanisms: (i) energy is generated by metabolic reactions in the body at a rate of \(280 \mathrm{~W},\) and almost all of this energy is converted to heat that flows to the skin; (ii) heat is delivered to the skin by convection from the outside air at a rate equal to \(k^{\prime} A_{\mathrm{skin}}\left(T_{\mathrm{air}}-T_{\mathrm{skin}}\right),\) where \(k^{\prime}\) is \(54 \mathrm{~J} / \mathrm{h} \cdot \mathrm{C}^{\circ} \cdot \mathrm{m}^{2},\) the exposed skin area \(A_{\text {skin }}\) is \(1.5 \mathrm{~m}^{2},\) the air temperature \(T_{\text {air }}\) is \(47^{\circ} \mathrm{C},\) and the skin temperature \(T_{\text {skin }}\) is \(36^{\circ} \mathrm{C} ;\) (iii) the skin absorbs radiant energy from the sun at a rate of \(1400 \mathrm{~W} / \mathrm{m}^{2} ;\) (iv) the skin absorbs radiant energy from the environment, which has temperature \(47^{\circ} \mathrm{C}\). (a) Calculate the net rate (in watts) at which the person's skin is heated by all four of these mechanisms. Assume that the emissivity of the skin is \(e=1\) and that the skin temperature is initially \(36^{\circ} \mathrm{C}\). Which mechanism is the most important? (b) At what rate (inL/h) must perspiration evaporate from this person's skin to maintain a constant skin temperature? (The heat of vaporization of water at \(36^{\circ} \mathrm{C}\) is \(2.42 \times 10^{6} \mathrm{~J} / \mathrm{kg} .\) ) (c) Suppose the person is protected by light-colored clothing \((e \approx 0)\) and only \(0.45 \mathrm{~m}^{2}\) of skin is exposed. What rate of perspiration is required now? Discuss the usefulness of the traditional clothing worn by desert peoples.

In a container of negligible mass, \(0.200 \mathrm{~kg}\) of ice at an initial temperature of \(-40.0^{\circ} \mathrm{C}\) is mixed with a mass \(m\) of water that has an initial temperature of \(80.0^{\circ} \mathrm{C}\). No heat is lost to the surroundings. If the final temperature of the system is \(28.0^{\circ} \mathrm{C},\) what is the mass \(m\) of the water that was initially at \(80.0^{\circ} \mathrm{C}\) ?

A steel wire has density \(7800 \mathrm{~kg} / \mathrm{m}^{3}\) and mass \(2.50 \mathrm{~g}\). It is stretched between two rigid supports separated by \(0.400 \mathrm{~m}\). (a) When the temperature of the wire is \(20.0^{\circ} \mathrm{C}\), the frequency of the fundamental standing wave for the wire is \(440 \mathrm{~Hz}\). What is the tension in the wire? (b) What is the temperature of the wire if its fundamental standing wave has frequency \(460 \mathrm{~Hz}\) ? For steel the coefficient of linear expansion is \(1.2 \times 10^{-5} \mathrm{~K}^{-1}\) and Young's modulus is \(20 \times 10^{10} \mathrm{~Pa}\)

(a) Normal body temperature. The average normal body temperature measured in the mouth is \(310 \mathrm{~K}\). What would Celsius and Fahrenheit thermometers read for this temperature? (b) Elevated body temperature. During very vigorous exercise, the body's temperature can go as high as \(40^{\circ} \mathrm{C}\). What would Kelvin and Fahrenheit thermometers read for this temperature? (c) Temperature difference in the body. The surface temperature of the body is normally about \(7 \mathrm{C}^{\circ}\) lower than the internal temperature. Express this temperature difference in kelvins and in Fahrenheit degrees. (d) Blood storage. Blood stored at \(4.0^{\circ} \mathrm{C}\) lasts safely for about 3 weeks, whereas blood stored at \(-160^{\circ} \mathrm{C}\) lasts for 5 years. Express both temperatures on the Fahrenheit and Kelvin scales. (e) Heat stroke. If the body's temperature is above \(105^{\circ} \mathrm{F}\) for a prolonged period, heat stroke can result. Express this temperature on the Celsius and Kelvin scales.

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