Answer:
C
Explanation:
got a one hundred on the test
Answer:
the electroscope separate by the presence of charge carriers
Explanation:
Metal bodies are characterized by having free (mobile) electrons. In the electroscope the plates are in balance; when the external metal ball is touched, a charge is introduced into the device, when the body that touched the ball is separated, an excess charge remains. This charge, being a metal, is distributed over the entire surface, giving a uniform density and an electric force of repulsion is created between the two charged sheets, which tends to separate the sheets. This force is counteracted by the tension component as the sheets are separated at a given angle, the separation reaches the point where
Fe - Tx = 0
Fe = Tx
In summary, the electroscope separate its leaves by the presence of charge carriers
Given:
Uniform distributed load with an intensity of W = 50 kN / m on an overhang beam.
We need to determine the maximum shear stress developed in the beam:
τ = F/A
Assuming the area of the beam is 100 m^2 with a length of 10 m.
τ = F/A
τ = W/l
τ = 50kN/m / 10 m
τ = 5kN/m^2
τ = 5000 N/ m^2<span />
Answer:
Please refer to the figure.
Explanation:
The crucial point here is to calculate the enclosed current. If the current I is flowing through the whole cross-sectional area of the wire, the current density is
![J = \frac{I}{\pi R^2}](https://tex.z-dn.net/?f=J%20%3D%20%5Cfrac%7BI%7D%7B%5Cpi%20R%5E2%7D)
The current density is constant for different parts of the wire. This idea is similar to that of the density of a glass of water is equal to the density of a whole bucket of water.
So,
![J = \frac{I}{\pi R^2} = \frac{I_{enc}}{\pi r^2}\\I_{enc} = \frac{Ir^2}{R^2}](https://tex.z-dn.net/?f=J%20%3D%20%5Cfrac%7BI%7D%7B%5Cpi%20R%5E2%7D%20%3D%20%5Cfrac%7BI_%7Benc%7D%7D%7B%5Cpi%20r%5E2%7D%5C%5CI_%7Benc%7D%20%3D%20%5Cfrac%7BIr%5E2%7D%7BR%5E2%7D)
This enclosed current is now to be used in Ampere’s Law.
![\mu_o I_{enc} = \int {B} \, dl](https://tex.z-dn.net/?f=%5Cmu_o%20I_%7Benc%7D%20%3D%20%5Cint%20%7BB%7D%20%5C%2C%20dl)
Here,
represents the circular path of radius r. So we can replace the integral with the circumference of the path,
.
As a result, the magnetic field is
![B = \frac{\mu_0}{2\pi}\frac{Ir}{R^2}](https://tex.z-dn.net/?f=B%20%3D%20%5Cfrac%7B%5Cmu_0%7D%7B2%5Cpi%7D%5Cfrac%7BIr%7D%7BR%5E2%7D)