The amplitude of an oscillating electric field at your cell phone is 4.0 μV/m when you are 10 km east of the broadcast antenna. To find the electric field amplitude when you are 20 km east of the antenna, we can use the inverse square law. The electric field amplitude when you are 20 km east of the antenna is 1.0 μV/m.
The inverse square law states that the intensity of a field is inversely proportional to the square of the distance from the source. In this case, the electric field is directly proportional to the amplitude.
Let's denote the electric field amplitude when you are 20 km east of the antenna as E2. We can set up the following equation using the inverse square law:
(E1 / E2) = (d2^2 / d1^2)
Where E1 is the initial electric field amplitude (4.0 μV/m), E2 is the unknown electric field amplitude, d1 is the initial distance (10 km), and d2 is the new distance (20 km).
Simplifying the equation, we get:
(4.0 μV/m / E2) = (20 km^2 / 10 km^2)
(4.0 μV/m / E2) = 4
Cross-multiplying, we find:
E2 = 4.0 μV/m / 4
E2 = 1.0 μV/m
Therefore, the electric field amplitude when you are 20 km east of the antenna is 1.0 μV/m.
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m. c. gonzalez-garcia and m. maltoni, phenomenology with massive neutrinos, phys. rept. 460 (2008) 1–129, [arxiv:0704.1800].
The paper by Gonzalez-Garcia and Maltoni provides a comprehensive overview of the phenomenology of massive neutrinos. It is an important resource for researchers .
The paper titled "Phenomenology with Massive Neutrinos" by M. C. Gonzalez-Garcia and M. Maltoni, published in Physical Reports in 2008, provides a comprehensive review of the phenomenology of massive neutrinos.
The paper is an authoritative source that discusses the theoretical framework and experimental evidence for the existence of neutrino masses.
Neutrinos are elementary particles that were originally thought to be massless.
However, experimental observations have shown that neutrinos undergo flavor oscillations, which implies that they must have non-zero masses. This discovery has profound implications for particle physics and cosmology.
The paper explores various aspects of neutrino phenomenology, including the measurement of neutrino masses and mixing angles, the implications for the Standard Model of particle physics, and the role of neutrinos in astrophysics and cosmology.
In conclusion, the paper by Gonzalez-Garcia and Maltoni provides a comprehensive overview of the phenomenology of massive neutrinos. It is an important resource for researchers and students interested in understanding the properties and implications of neutrino masses.
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Why did it take more generations of complete selection to reduce q from 0.1 to 0.01 (a 0.09 change) compared that for a 0.5 to 0.1 reduction (a larger, 0.4 change)? explain.
In conclusion, the starting frequency of a trait determines how many generations of complete selection are needed to reduce its frequency. A higher starting frequency allows for a faster reduction, while a lower starting frequency requires more generations for the same amount of change.
The reason it took more generations of complete selection to reduce q from 0.1 to 0.01 compared to reducing it from 0.5 to 0.1 is because of the starting frequencies of q.
When starting with a higher frequency of q, such as 0.5, there is a larger pool of individuals with the desired trait. This means that there are more individuals available for selection and reproduction, which can lead to a faster reduction in the frequency of q.
In contrast, starting with a lower frequency of q, such as 0.1, means that there are fewer individuals with the desired trait. This smaller pool of individuals results in a slower rate of selection and reproduction, leading to a slower reduction in the frequency of q.
To put it simply, it is easier and faster to reduce a trait that is more common in a population compared to one that is less common.
In conclusion, the starting frequency of a trait determines how many generations of complete selection are needed to reduce its frequency. A higher starting frequency allows for a faster reduction, while a lower starting frequency requires more generations for the same amount of change.
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trons accelerated by a potential difference of 12.3 v pass through a gas of hydrogen atoms at room temperature.
When trons are accelerated by a potential difference of 12.3 V, they pass through a gas of hydrogen atoms at room temperature.
In this scenario, the potential difference of 12.3 V is causing the trons to move or accelerate. The trons then interact with the hydrogen atoms in the gas.
At room temperature, hydrogen exists as individual atoms rather than molecules. Each hydrogen atom consists of a single proton and one electron. When the trons pass through the gas of hydrogen atoms, they may collide with the hydrogen atoms and interact with their electrons.
These interactions between the trons and hydrogen atoms can have various outcomes. For example, the trons may transfer energy to the hydrogen atoms, causing them to become excited or even ionized. This transfer of energy can lead to the emission of light or the formation of ions.
To summarize, when trons are accelerated by a potential difference of 12.3 V and pass through a gas of hydrogen atoms at room temperature, they can interact with the hydrogen atoms, causing various outcomes such as excitation or ionization. This interaction between the trons and hydrogen atoms is influenced by the energy transfer between them.
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