Calculating Radiation from a Leslie Cube

  • Thread starter Thread starter jaidon
  • Start date Start date
  • Tags Tags
    Cube Radiation
AI Thread Summary
The discussion focuses on calculating radiation from a Leslie cube with a surface temperature of 97°C. The wavelength at which spectral intensity is maximized is determined using Wien's displacement law, yielding approximately 7.8 micrometers. The total intensity of emitted radiation is calculated using the Stefan-Boltzmann law, resulting in about 191,000 W/m². The total power emitted by the black surface is found by multiplying the intensity by the area, leading to approximately 7,640 watts. Additionally, spectral energy density in Planck's equation is defined as energy per unit volume per unit wavelength, also referred to as spectral radiance.
jaidon
Messages
41
Reaction score
0
A Leslie cube has a surface temp of 97C. One of its four side faces has an area of 100 cm^2 and is painted black. Calculate:

a) the wavelength at which the spectral intensity (per unit wavelength) is a maximum

b)the total intensity (all wavelengths) of the emitted radiation just outside the surface

C) the total power emitted by the black surface

for a) i used lambda=2.9*10^-3/T (not sure if this is the correct way of doing it)

for b) i wanted to use Stefan's Law but this seems to simple

for c) i multiplied the answer from b) by the area of the four sides.

does any of this sound correct? i seem to be struggling on this topic

also, in Planck's energy density equation, what exactly is the spectral energy density? is it also known as anything else? thanks.
 
Physics news on Phys.org
a) The wavelength at which the spectral intensity is a maximum is 2.9 x 10^-3 m/K, calculated using the equation lambda=2.9*10^-3/T, where T is the temperature in Kelvin (97C = 370K). b) The total intensity of the emitted radiation just outside the surface can be calculated using Stefan's law, which states that the total energy emitted by an object is proportional to the fourth power of its temperature. The total intensity of the emitted radiation at the surface is equal to the Stefan-Boltzmann constant (σ) times the fourth power of the surface temperature: I = σT^4. Therefore, the total intensity of the emitted radiation just outside the surface is equal to 5.67 x 10^-8 W/m^2K^4 × 370K^4 = 9.83 x 10^-5 W/m^2. c) The total power emitted by the black surface can be calculated by multiplying the total intensity of the emitted radiation just outside the surface with the area of the four sides: P = I × A = 9.83 x 10^-5 W/m^2 × 100 cm^2 = 0.983 W. In Planck's energy density equation, the spectral energy density is the amount of energy per unit frequency or wavelength emitted by a body in thermal equilibrium. It is usually expressed as the energy per unit frequency interval, or as the energy per unit wavelength interval.
 


a) To calculate the wavelength at which the spectral intensity (per unit wavelength) is a maximum, we can use Wien's displacement law: λ(max) = 2.898 / T, where T is the temperature in Kelvin. In this case, T = 97 + 273 = 370 K. Therefore, λ(max) = 2.898 / 370 = 0.0078 meters or 7.8 micrometers.

b) To calculate the total intensity (all wavelengths) of the emitted radiation just outside the surface, we can use the Stefan-Boltzmann law: I = σT^4, where σ is the Stefan-Boltzmann constant (5.67 x 10^-8 W/m^2K^4) and T is the temperature in Kelvin. Here, T = 97 + 273 = 370 K. Plugging in the values, we get I = 5.67 x 10^-8 x 370^4 = 1.91 x 10^5 W/m^2.

c) To calculate the total power emitted by the black surface, we can use the formula P = A x I, where P is power, A is the area of the surface, and I is the intensity calculated in part b). Here, A = 4 x 100 cm^2 = 400 cm^2 = 0.04 m^2. Therefore, P = 0.04 x 1.91 x 10^5 = 7.64 x 10^3 watts.

In Planck's energy density equation, spectral energy density refers to the amount of energy per unit volume per unit wavelength. It is also known as spectral radiance or spectral flux density. It represents the distribution of energy at different wavelengths for a given temperature.
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
TL;DR Summary: I came across this question from a Sri Lankan A-level textbook. Question - An ice cube with a length of 10 cm is immersed in water at 0 °C. An observer observes the ice cube from the water, and it seems to be 7.75 cm long. If the refractive index of water is 4/3, find the height of the ice cube immersed in the water. I could not understand how the apparent height of the ice cube in the water depends on the height of the ice cube immersed in the water. Does anyone have an...
Back
Top