Answer:
(a) ![3.81\times 10^5\ Pa](https://tex.z-dn.net/?f=3.81%5Ctimes%2010%5E5%5C%20Pa)
(b) ![4.19\times 1065\ Pa](https://tex.z-dn.net/?f=4.19%5Ctimes%201065%5C%20Pa)
Explanation:
<u>Given:</u>
= The first temperature of air inside the tire = ![10^\circ C =(273+10)\ K =283\ K](https://tex.z-dn.net/?f=10%5E%5Ccirc%20C%20%3D%28273%2B10%29%5C%20K%20%3D283%5C%20K)
= The second temperature of air inside the tire = ![46^\circ C =(273+46)\ K= 319\ K](https://tex.z-dn.net/?f=46%5E%5Ccirc%20C%20%3D%28273%2B46%29%5C%20K%3D%20319%5C%20K)
= The third temperature of air inside the tire = ![85^\circ C =(273+85)\ K=358 \ K](https://tex.z-dn.net/?f=85%5E%5Ccirc%20C%20%3D%28273%2B85%29%5C%20K%3D358%20%5C%20K)
= The first volume of air inside the tire
= The second volume of air inside the tire = ![30\% V_1 = 0.3V_1](https://tex.z-dn.net/?f=30%5C%25%20V_1%20%3D%200.3V_1)
= The third volume of air inside the tire = ![2\%V_2+V_2= 102\%V_2=1.02V_2](https://tex.z-dn.net/?f=2%5C%25V_2%2BV_2%3D%20102%5C%25V_2%3D1.02V_2)
= The first pressure of air inside the tire = ![1.01325\times 10^5\ Pa](https://tex.z-dn.net/?f=1.01325%5Ctimes%2010%5E5%5C%20Pa)
<u>Assume:</u>
= The second pressure of air inside the tire
= The third pressure of air inside the tire- n = number of moles of air
Since the amount pof air inside the tire remains the same, this means the number of moles of air in the tire will remain constant.
Using ideal gas equation, we have
![PV = nRT\\\Rightarrow \dfrac{PV}{T}=nR = constant\,\,\,(\because n,\ R\ are\ constants)](https://tex.z-dn.net/?f=PV%20%3D%20nRT%5C%5C%5CRightarrow%20%5Cdfrac%7BPV%7D%7BT%7D%3DnR%20%3D%20constant%5C%2C%5C%2C%5C%2C%28%5Cbecause%20n%2C%5C%20R%5C%20are%5C%20constants%29)
Part (a):
Using the above equation for this part of compression in the air, we have
![\therefore \dfrac{P_1V_1}{T_1}=\dfrac{P_2V_2}{T_2}\\\Rightarrow P_2 = \dfrac{V_1}{V_2}\times \dfrac{T_2}{T_1}\times P_1\\\Rightarrow P_2 = \dfrac{V_1}{0.3V_1}\times \dfrac{319}{283}\times 1.01325\times 10^5\\\Rightarrow P_2 =3.81\times 10^5\ Pa](https://tex.z-dn.net/?f=%5Ctherefore%20%5Cdfrac%7BP_1V_1%7D%7BT_1%7D%3D%5Cdfrac%7BP_2V_2%7D%7BT_2%7D%5C%5C%5CRightarrow%20P_2%20%3D%20%5Cdfrac%7BV_1%7D%7BV_2%7D%5Ctimes%20%5Cdfrac%7BT_2%7D%7BT_1%7D%5Ctimes%20P_1%5C%5C%5CRightarrow%20P_2%20%3D%20%5Cdfrac%7BV_1%7D%7B0.3V_1%7D%5Ctimes%20%5Cdfrac%7B319%7D%7B283%7D%5Ctimes%201.01325%5Ctimes%2010%5E5%5C%5C%5CRightarrow%20P_2%20%3D3.81%5Ctimes%2010%5E5%5C%20Pa)
Hence, the pressure in the tire after the compression is
.
Part (b):
Again using the equation for this part for the air, we have
![\therefore \dfrac{P_2V_2}{T_2}=\dfrac{P_3V_3}{T_3}\\\Rightarrow P_3 = \dfrac{V_2}{V_3}\times \dfrac{T_3}{T_2}\times P_2\\\Rightarrow P_3 = \dfrac{V_2}{1.02V_2}\times \dfrac{358}{319}\times 3.81\times 10^5\\\Rightarrow P_3 =4.19\times 10^5\ Pa](https://tex.z-dn.net/?f=%5Ctherefore%20%5Cdfrac%7BP_2V_2%7D%7BT_2%7D%3D%5Cdfrac%7BP_3V_3%7D%7BT_3%7D%5C%5C%5CRightarrow%20P_3%20%3D%20%5Cdfrac%7BV_2%7D%7BV_3%7D%5Ctimes%20%5Cdfrac%7BT_3%7D%7BT_2%7D%5Ctimes%20P_2%5C%5C%5CRightarrow%20P_3%20%3D%20%5Cdfrac%7BV_2%7D%7B1.02V_2%7D%5Ctimes%20%5Cdfrac%7B358%7D%7B319%7D%5Ctimes%203.81%5Ctimes%2010%5E5%5C%5C%5CRightarrow%20P_3%20%3D4.19%5Ctimes%2010%5E5%5C%20Pa)
Hence, the pressure in the tire after the car i driven at high speed is
.
Answer:
A.c
Explanation:
The chromosphere is above the photosphere, the visible "surface" of the Sun. It lies below the solar corona, the Sun's upper atmosphere, which extends many thousands of kilometers above the chromosphere into space. The plasma (electrically charged gas) in the chromosphere has a very low density.
In basic terms it is the 2nd one out from the core.
Each BB 0.349 grams and 5.386 grains. 349 mg & 5.386 grains each steel BBs.
Answer:
continental drift
Explanation:
Wegener proposed that the continents plowed through crust of ocean basins, which would explain why the outlines of many coastlines look like they fit together like a puzzle
Answer:
they help us allocate a particular place in case one needs to allocate or find a place or something