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What is the radiation pressure due to Betelgeuse (which has a luminosity, or power output, 10,000 times that of the Sun) at a distance equal to that of Uranus's orbit from it?

Short Answer

Expert verified
Answer: The radiation pressure due to Betelgeuse at a distance equal to Uranus's orbit is approximately 7.42 x 10^(-9) N/m^2.

Step by step solution

01

Constants

Write down the constants: Luminosity of the Sun (L_sun) = 3.8 x 10^26 W Luminosity of Betelgeuse (L_B) = 10,000 x L_sun Distance of Uranus's orbit from the Sun (d) = 2.9 x 10^12 m Speed of light (c) = 3.0 x 10^8 m/s
02

Calculate the luminosity of Betelgeuse

Calculate the luminosity of Betelgeuse by multiplying the given factor by the solar luminosity: L_B = 10,000 × L_sun = 10,000 × (3.8 × 10^26 W) = 3.8 × 10^30 W
03

Calculate the radiation pressure

Use the formula for radiation pressure and substitute the values: P = L_B / (4 * π * d^2 * c) Substitute the values: P = (3.8 × 10^30 W) / (4 * π * (2.9 x 10^12 m)^2 * 3.0 x 10^8 m/s)
04

Solve for P

Calculate the radiation pressure: P ≈ 7.42 × 10^(-9) N/m^2 So the radiation pressure due to Betelgeuse at a distance equal to that of Uranus's orbit from it is approximately 7.42 x 10^(-9) N/m^2.

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Key Concepts

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

Luminosity of Stars
When we talk about the luminosity of stars, we're referring to the amount of energy a star emits per second. It is effectively the star's power output, measured in units of watts (W). This property is a crucial indicator of many other stellar characteristics, including mass and temperature. For instance, our Sun has a luminosity of approximately 3.8 x 10^26 W, which may seem formidable, but is moderate compared to some other stars.

Now, consider Betelgeuse, a red supergiant star, whose luminosity is a staggering 10,000 times that of the Sun. To calculate Betelgeuse's luminosity, we multiply this factor by the Sun's luminosity to yield a luminous near 3.8 x 10^30 W. This immense energy output is central to understanding the impacts Betelgeuse can have, including radiation pressure exerted at a distance, as seen in our exercise.
Distance and Radiation Relationship
The relationship between distance and the radiation received from a star is a fundamental principle of astrophysics known as the inverse-square law. This law states that the intensity of an effect (such as gravity, light, sound, or in our case, radiation pressure) is inversely proportional to the square of the distance from the source of that effect.

In simpler terms, if you double the distance from the star, the radiation pressure you experience is not just halved; it is reduced to a quarter of its original value. This radical decrement is due to the dispersion of radiation over a larger area as you move away from the source. This concept is why the potentially devastating radiation from Betelgeuse, at a distance equivalent to Uranus's orbit, is lessened to a pressure that's much easier to comprehend (and far less hazardous!).
Radiation Pressure Formula
The formula for radiation pressure is given by: \( P = \frac{L}{4 \pi d^2 c} \) where \( P \) is the radiation pressure, \( L \) is the luminosity of the star, \( d \) is the distance from the star, and \( c \) is the speed of light. Here, the formula encapsulates the essence of both the inverse-square law and the direct proportionality of pressure to the star's luminosity, mitigated by the constant that is the speed of light.

To solve for \( P \) in the context of our exercise involving Betelgeuse and its staggering luminosity, we plugged in the appropriate values and determined the radiation pressure on a hypothetical object located at the distance of Uranus's orbit. The calculation demonstrates a direct application of the formula and provides an understanding of the immense power of stellar objects, even at vast distances.

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Most popular questions from this chapter

At the surface of the Earth, the Sun delivers an estimated \(1.00 \mathrm{~kW} / \mathrm{m}^{2}\) of energy. Suppose sunlight hits a \(10.0 \mathrm{~m}\) by \(30.0 \mathrm{~m}\) roof at an angle of \(90.0^{\circ}\) a) Estimate the total power incident on the roof. b) Find the radiation pressure on the roof.

A resistor consists of a solid cylinder of radius \(r\) and length \(L\). The resistor has resistance \(R\) and is carrying current \(i\). Use the Poynting vector to calculate the power radiated out of the surface of the resistor.

If two communication signals were sent at the same time to the Moon, one via radio waves and one via visible light, which one would arrive at the Moon first?

Quantum theory says that electromagnetic waves actually consist of discrete packets-photons-each with energy \(E=\hbar \omega,\) where \(\hbar=1.054573 \cdot 10^{-34} \mathrm{~J} \mathrm{~s}\) is Planck's reduced constant and \(\omega\) is the angular frequency of the wave. a) Find the momentum of a photon. b) Find the angular momentum of a photon. Photons are circularly polarized; that is, they are described by a superposition of two plane-polarized waves with equal field amplitudes, equal frequencies, and perpendicular polarizations, one-quarter of a cycle \(\left(90^{\circ}\right.\) or \(\pi / 2\) rad \()\) out of phase, so the electric and magnetic field vectors at any fixed point rotate in a circle with the angular frequency of the waves. It can be shown that a circularly polarized wave of energy \(U\) and angular frequency \(\omega\) has an angular momentum of magnitude \(L=U / \omega .\) (The direction of the angular momentum is given by the thumb of the right hand, when the fingers are curled in the direction in which the field vectors circulate. c) The ratio of the angular momentum of a particle to \(\hbar\) is its spin quantum number. Determine the spin quantum number of the photon.

The voltage across a cylindrical conductor of radius \(r\), length \(L\), and resistance \(R\) varies with time. The timevarying voltage causes a time-varying current, \(i\), to flow in the cylinder. Show that the displacement current equals \(\epsilon_{0} \rho d i / d t,\) where \(\rho\) is the resistivity of the conductor.

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