Answer:
Now, think on the electrons flowing through a conductor (we can think on the resistor as a simple conductor, like a piece of metal)
Inside the conductor, we have some "fixed" (they do not flow with the current) electrons, such that as the current flows in the conductor, the flowing electrons can interact with the fixed ones in the conductor. Then we can have collisions inside the conductor.
In those collisions, the flowing electrons leave energy in the conductor, and as we know, heat is a form of energy. Then when we have a lot of these collisions, the temperature of the conductor increases.
That is why electronic devices get hot.
Also, as the temperature of a conductor increases, the electrons inside of it start to move more, then the probability of an interaction with the flowing electrons increases.
Answer:
(a). The draw-down at a distance 200 m from the well after pumping for 50 hr is 5.383 m.
(b). The draw-down at a distance 200 m from the well after pumping for 50 hr is 6.707 m.
Explanation:
Given that,
Energy ![Q=300\ m^3/hr](https://tex.z-dn.net/?f=Q%3D300%5C%20m%5E3%2Fhr)
Transmissivity ![T = 25\ m^2/hr](https://tex.z-dn.net/?f=T%20%3D%2025%5C%20m%5E2%2Fhr)
Storage coefficient ![S=2.5\times10^{-4}](https://tex.z-dn.net/?f=S%3D2.5%5Ctimes10%5E%7B-4%7D)
Distance r= 200 m
We need to calculate the draw-down at a distance 200 m from the well after pumping for 50 hr
Using formula of draw-down
![s= \dfrac{Q}{4\pi T}(-0.5772-ln\dfrac{r^2S}{4tT})](https://tex.z-dn.net/?f=s%3D%20%5Cdfrac%7BQ%7D%7B4%5Cpi%20T%7D%28-0.5772-ln%5Cdfrac%7Br%5E2S%7D%7B4tT%7D%29)
Put the value into the formula
![s=\dfrac{300}{4\pi\times25}(-0.5772-ln\dfrac{(200)^2\times2.5\times10^{-4}}{4\times25\times50})](https://tex.z-dn.net/?f=s%3D%5Cdfrac%7B300%7D%7B4%5Cpi%5Ctimes25%7D%28-0.5772-ln%5Cdfrac%7B%28200%29%5E2%5Ctimes2.5%5Ctimes10%5E%7B-4%7D%7D%7B4%5Ctimes25%5Ctimes50%7D%29)
![s=5.383\ m](https://tex.z-dn.net/?f=s%3D5.383%5C%20m)
We need to calculate the draw-down at a distance 200 m from the well after pumping for 200 hr
Using formula of draw-down
![s= \dfrac{Q}{4\pi T}(-0.5772-ln\dfrac{r^2S}{4tT})](https://tex.z-dn.net/?f=s%3D%20%5Cdfrac%7BQ%7D%7B4%5Cpi%20T%7D%28-0.5772-ln%5Cdfrac%7Br%5E2S%7D%7B4tT%7D%29)
Put the value into the formula
![s=\dfrac{300}{4\pi\times25}(-0.5772-ln\dfrac{(200)^2\times2.5\times10^{-4}}{4\times25\times200})](https://tex.z-dn.net/?f=s%3D%5Cdfrac%7B300%7D%7B4%5Cpi%5Ctimes25%7D%28-0.5772-ln%5Cdfrac%7B%28200%29%5E2%5Ctimes2.5%5Ctimes10%5E%7B-4%7D%7D%7B4%5Ctimes25%5Ctimes200%7D%29)
![s=6.707\ m](https://tex.z-dn.net/?f=s%3D6.707%5C%20m)
Hence, (a). The draw-down at a distance 200 m from the well after pumping for 50 hr is 5.383 m.
(b). The draw-down at a distance 200 m from the well after pumping for 200 hr is 6.707 m.
Answer:
total work is = 52450 J
Explanation:
given data
mass = 5000-lb
density = 10 lb/ft
height = 50 ft
solution
as we will treat here cable and ball are separate
and
here work need to lift cable is
w = (10Δy )(9.8 y ) j
and
now summing all segment of cable
so passing limit Δy to 0
so total work need
=
=
= 2450J
so lifting 5000 lb wrcking 50 m required additional 5000 + 2450
so total work is = 52450 J
<span>Of course.
Throw a ball into the air. Right after you release it, the velocity is upward, but the acceleration is downward.
Later, the velocity falls to zero; the acceleration is still downward.
Still later, the velocity goes downward; the acceleration is still downward.</span>