Answer:
Option C
Explanation:
According to the question:
Force exerted by the team towards south, F = 10 N
Force exerted by the opposite team towards North, F' = 17 N
Net Force, ![\vec{F_{net}} = \vec{F'} - \vec{F}](https://tex.z-dn.net/?f=%5Cvec%7BF_%7Bnet%7D%7D%20%3D%20%5Cvec%7BF%27%7D%20-%20%5Cvec%7BF%7D)
![\vec{F_{net}} = \vec{F'} - \vec{F} = 17 - 10 = 7 N](https://tex.z-dn.net/?f=%5Cvec%7BF_%7Bnet%7D%7D%20%3D%20%5Cvec%7BF%27%7D%20-%20%5Cvec%7BF%7D%20%3D%2017%20-%2010%20%3D%207%20N)
Thus the force will be along the direction of force whose magnitude is higher
Therefore,
towards North
To solve this problem we will apply the concepts related to wavelength, as well as Rayleigh's Criterion or Optical resolution, the optical limit due to diffraction can be calculated empirically from the following relationship,
![sin\theta = 1.22\frac{\lambda}{d}](https://tex.z-dn.net/?f=sin%5Ctheta%20%3D%201.22%5Cfrac%7B%5Clambda%7D%7Bd%7D)
Here,
= Wavelength
d= Diameter of aperture
= Angular resolution or diffraction angle
Our values are given as,
![\theta = 11\°](https://tex.z-dn.net/?f=%5Ctheta%20%3D%2011%5C%C2%B0)
The frequency of the sound is ![f = 9100 Hz](https://tex.z-dn.net/?f=f%20%3D%209100%20Hz)
The speed of the sound is ![v = 343 m/s](https://tex.z-dn.net/?f=v%20%3D%20343%20m%2Fs)
The wavelength of the sound is
![\lambda = \frac{v}{f}](https://tex.z-dn.net/?f=%5Clambda%20%3D%20%5Cfrac%7Bv%7D%7Bf%7D)
Here,
v = Velocity of the wave
f = Frequency
Replacing,
![\lambda = \frac{(343 m/s)}{(9100 Hz)}](https://tex.z-dn.net/?f=%5Clambda%20%3D%20%5Cfrac%7B%28343%20m%2Fs%29%7D%7B%289100%20Hz%29%7D)
![\lambda = 0.0377 m](https://tex.z-dn.net/?f=%5Clambda%20%3D%200.0377%20m)
The diffraction condition is then,
![sin\theta = 1.22\frac{\lambda}{d}](https://tex.z-dn.net/?f=sin%5Ctheta%20%3D%201.22%5Cfrac%7B%5Clambda%7D%7Bd%7D)
Replacing,
![sin(11\°) = 1.22\frac{(0.0377 m)}{(d)}](https://tex.z-dn.net/?f=sin%2811%5C%C2%B0%29%20%3D%201.22%5Cfrac%7B%280.0377%20m%29%7D%7B%28d%29%7D)
d = 0.24 m
Therefore the diameter should be 0.24m
Answer:
Option D: 1.5in in front of the target
Explanation:
The object distance is
.
Because the surface is flat, the radius of curvature is infinity .
The incident index is
and the transmitted index is
.
The single interface equation is ![\frac{n_i}{y}+\frac{n_t}{y^i}=\frac{n_t-n_i}{r}](https://tex.z-dn.net/?f=%5Cfrac%7Bn_i%7D%7By%7D%2B%5Cfrac%7Bn_t%7D%7By%5Ei%7D%3D%5Cfrac%7Bn_t-n_i%7D%7Br%7D)
Substituting the quantities given in the problem,
![\frac{\frac{4}{3}}{6in}+\frac{1}{y^i}= 0](https://tex.z-dn.net/?f=%5Cfrac%7B%5Cfrac%7B4%7D%7B3%7D%7D%7B6in%7D%2B%5Cfrac%7B1%7D%7By%5Ei%7D%3D%200)
The image distance is then ![y^i=-\frac{18}{4}in =-4.5in](https://tex.z-dn.net/?f=y%5Ei%3D-%5Cfrac%7B18%7D%7B4%7Din%20%3D-4.5in)
Therefore, the coin falls
in front of the target
Answer:
no Jake arm is high so the weight of an object become high due to potential energy.
so, option A is correct ) Jake did more work