Answer:
Explanation:
We shall apply conservation of momentum law in vector form to solve the problem .
Initial momentum = 0
momentum of 12 g piece
= .012 x 37 i since it moves along x axis .
= .444 i
momentum of 22 g
= .022 x 34 j
= .748 j
Let momentum of third piece = p
total momentum
= p + .444 i + .748 j
so
applying conservation law of momentum
p + .444 i + .748 j = 0
p = - .444 i - .748 j
magnitude of p
= √ ( .444² + .748² )
= .87 kg m /s
mass of third piece = 58 - ( 12 + 22 )
= 24 g = .024 kg
if v be its velocity
.024 v = .87
v = 36.25 m / s .
Answer:
<u>Searching in google I found the total mass and the radius of the ball (m = 1.5 kg and r = 10 cm) which are needed to solve the problem!</u>
The ball rotates 6.78 revolutions.
Explanation:
<u>Searching in google I found the total mass and the radius of the ball (m = 1.5 kg and r = 10 cm) which are needed to solve the problem!</u>
At the bottom the ball has the following angular speed:
![\omega_{f} = \frac{v_{f}}{r} = \frac{4.9 m/s}{0.10 m} = 49 rad/s](https://tex.z-dn.net/?f=%20%5Comega_%7Bf%7D%20%3D%20%5Cfrac%7Bv_%7Bf%7D%7D%7Br%7D%20%3D%20%5Cfrac%7B4.9%20m%2Fs%7D%7B0.10%20m%7D%20%3D%2049%20rad%2Fs%20)
Now, we need to find the distance traveled by the ball (L) by using θ=28° and h(height) = 2 m:
To find the revolutions we need the time, which can be found using the following equation:
(1)
So first, we need to find the acceleration:
(2)
By entering equation (2) into (1) we have:
![t = \frac{v_{f} - v_{0}}{\frac{v_{f}^{2} - v_{0}^{2}}{2L}}](https://tex.z-dn.net/?f=%20t%20%3D%20%5Cfrac%7Bv_%7Bf%7D%20-%20v_%7B0%7D%7D%7B%5Cfrac%7Bv_%7Bf%7D%5E%7B2%7D%20-%20v_%7B0%7D%5E%7B2%7D%7D%7B2L%7D%7D%20)
Since it starts from rest (v₀ = 0):
![t = \frac{2L}{v_{f}} = \frac{2*4.26 m}{4.9 m/s} = 1.74 s](https://tex.z-dn.net/?f=%20t%20%3D%20%5Cfrac%7B2L%7D%7Bv_%7Bf%7D%7D%20%3D%20%5Cfrac%7B2%2A4.26%20m%7D%7B4.9%20m%2Fs%7D%20%3D%201.74%20s%20)
Finally, we can find the revolutions:
![\theta_{f} = \frac{1}{2} \omega_{f}*t = \frac{1}{2}*49 rad/s*1.74 s = 42.63 rad*\frac{1 rev}{2\pi rad} = 6.78 rev](https://tex.z-dn.net/?f=%20%5Ctheta_%7Bf%7D%20%3D%20%5Cfrac%7B1%7D%7B2%7D%20%5Comega_%7Bf%7D%2At%20%3D%20%5Cfrac%7B1%7D%7B2%7D%2A49%20rad%2Fs%2A1.74%20s%20%3D%2042.63%20rad%2A%5Cfrac%7B1%20rev%7D%7B2%5Cpi%20rad%7D%20%3D%206.78%20rev%20)
Therefore, the ball rotates 6.78 revolutions.
I hope it helps you!
Answer:
The number of oxygen molecules in the left container greater than the number of hydrogen molecules in the right container.
Explanation:
Given:
Molar mass of oxygen, ![M_O=32](https://tex.z-dn.net/?f=M_O%3D32)
Molar mass of hydrogen, ![M_H=2](https://tex.z-dn.net/?f=M_H%3D2)
We know ideal gas law as:
![PV=nRT](https://tex.z-dn.net/?f=PV%3DnRT)
where:
P = pressure of the gas
V = volume of the gas
n= no. of moles of the gas molecules
R = universal gs constant
T = temperature of the gas
∵![n=\frac{m}{M}](https://tex.z-dn.net/?f=n%3D%5Cfrac%7Bm%7D%7BM%7D)
where:
m = mass of gas in grams
M = molecular mass of the gas
∴Eq. (1) can be written as:
![PV=\frac{m}{M}.RT](https://tex.z-dn.net/?f=PV%3D%5Cfrac%7Bm%7D%7BM%7D.RT)
![P=\frac{m}{V}.\frac{RT}{M}](https://tex.z-dn.net/?f=P%3D%5Cfrac%7Bm%7D%7BV%7D.%5Cfrac%7BRT%7D%7BM%7D)
as: ![\frac{m}{V}=\rho\ (\rm density)](https://tex.z-dn.net/?f=%5Cfrac%7Bm%7D%7BV%7D%3D%5Crho%5C%20%28%5Crm%20density%29)
So,
![P=\rho.\frac{RT}{M}](https://tex.z-dn.net/?f=P%3D%5Crho.%5Cfrac%7BRT%7D%7BM%7D)
Now, according to given we have T,P,R same for both the gases.
![P_O=P_H](https://tex.z-dn.net/?f=P_O%3DP_H)
![\rho_O.\frac{RT}{M_O}=\rho_H.\frac{RT}{M_H}](https://tex.z-dn.net/?f=%5Crho_O.%5Cfrac%7BRT%7D%7BM_O%7D%3D%5Crho_H.%5Cfrac%7BRT%7D%7BM_H%7D)
![\Rightarrow \frac{\rho_O}{32}=\frac{\rho_H}{2}](https://tex.z-dn.net/?f=%5CRightarrow%20%5Cfrac%7B%5Crho_O%7D%7B32%7D%3D%5Cfrac%7B%5Crho_H%7D%7B2%7D)
![\rho_O=16\rho_H](https://tex.z-dn.net/?f=%5Crho_O%3D16%5Crho_H)
∴The molecules of oxygen are more densely packed than the molecules of hydrogen in the same volume at the same temperature and pressure. So, <em>the number of oxygen molecules in the left container greater than the number of hydrogen molecules in the right container.</em>
Answer:
The average induced emf around the border of the circular region is
.
Explanation:
Given that,
Radius of circular region, r = 1.5 mm
Initial magnetic field, B = 0
Final magnetic field, B' = 1.5 T
The magnetic field is pointing upward when viewed from above, perpendicular to the circular plane in a time of 125 ms. We need to find the average induced emf around the border of the circular region. It is given by the rate of change of magnetic flux as :
![\epsilon=\dfrac{-d\phi}{dt}\\\\\epsilon=A\dfrac{-d(B'-B)}{dt}\\\\\epsilon=\pi (1.5\times 10^{-3})^2\times \dfrac{1.5}{0.125}\\\\\epsilon=8.48\times 10^{-5}\ V](https://tex.z-dn.net/?f=%5Cepsilon%3D%5Cdfrac%7B-d%5Cphi%7D%7Bdt%7D%5C%5C%5C%5C%5Cepsilon%3DA%5Cdfrac%7B-d%28B%27-B%29%7D%7Bdt%7D%5C%5C%5C%5C%5Cepsilon%3D%5Cpi%20%281.5%5Ctimes%2010%5E%7B-3%7D%29%5E2%5Ctimes%20%5Cdfrac%7B1.5%7D%7B0.125%7D%5C%5C%5C%5C%5Cepsilon%3D8.48%5Ctimes%2010%5E%7B-5%7D%5C%20V)
So, the average induced emf around the border of the circular region is
.