Answer
Verified
386.4k+ views
Hint: The device shown is a very common phenomenon that we are observing in our daily lives. Once, the liquid starts coming it continues until all the liquid from the container becomes empty. This flow of water happens due to the difference of pressure at the two ends of the pipe. We know the pressure difference led to many phenomena like lift in an airplane, etc.
Formula used: We make use of Bernoulli’s theorem to solve this problem.
$ P+\dfrac{\rho {{v}^{2}}}{2}+\rho gh=k $ , where k is a constant.
Complete step by step solution:
Applying Bernoulli's theorem at points $ 1 $ and $ 2 $ the height is being measured from the point $ 1 $ only, and the velocity of the liquid is zero at point $ 1 $ because the liquid is at rest. So,
$ {{P}_{1}}+\dfrac{\rho {{v}_{1}}^{2}}{2}+\rho g{{h}_{1}}={{P}_{2}}+\dfrac{\rho {{v}_{2}}^{2}}{2}+\rho g{{h}_{2}} \\
\Rightarrow {{P}_{1}}+0+0={{P}_{2}}+\dfrac{\rho {{v}_{2}}^{2}}{2}+\rho g{{h}_{2}} \\
\Rightarrow {{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}}=\dfrac{\rho {{v}_{2}}^{2}}{2} \\
\Rightarrow v_{2}^{2}=\dfrac{2({{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}})}{\rho } \\
\therefore {{v}_{2}}=\sqrt{\dfrac{2({{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}})}{\rho }} \\ $
So, we have found out the velocity of the liquid at point $ 2 $ , but for maximum possible height, the velocity at that height must be equal to zero, thus,
$ {{v}_{2}}=\sqrt{\dfrac{2({{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}})}{\rho }} \\
\Rightarrow \sqrt{\dfrac{2({{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}})}{\rho }}=0 \\
\Rightarrow {{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}}=0 \\
\Rightarrow \rho g{{h}_{2}}={{P}_{1}}-{{P}_{2}} \\
\Rightarrow {{h}_{2}}=\dfrac{{{P}_{1}}-{{P}_{2}}}{\rho g} \\ $
But the pressure, $ {{P}_{2}}=0 $
Thus, $ {{h}_{2}}=\dfrac{{{P}_{1}}}{\rho g} $ , putting the values of atmospheric pressure, acceleration due to gravity and density we get,
$ \therefore {{h}_{2}}=\dfrac{{{10}^{5}}}{1000\times 10}=10m $
So, the correct option is (B).
Note:
Sometimes these kinds of problems are also solved using Pascal's law of pressure. Pascal law states that pressure remains the same at the same horizontal level in a liquid. Both the columns are exposed to the atmosphere and the height of the liquid is also given. But that way the problem becomes too complex and that’s why we have invoked Bernoulli's principle here.
Formula used: We make use of Bernoulli’s theorem to solve this problem.
$ P+\dfrac{\rho {{v}^{2}}}{2}+\rho gh=k $ , where k is a constant.
Complete step by step solution:
Applying Bernoulli's theorem at points $ 1 $ and $ 2 $ the height is being measured from the point $ 1 $ only, and the velocity of the liquid is zero at point $ 1 $ because the liquid is at rest. So,
$ {{P}_{1}}+\dfrac{\rho {{v}_{1}}^{2}}{2}+\rho g{{h}_{1}}={{P}_{2}}+\dfrac{\rho {{v}_{2}}^{2}}{2}+\rho g{{h}_{2}} \\
\Rightarrow {{P}_{1}}+0+0={{P}_{2}}+\dfrac{\rho {{v}_{2}}^{2}}{2}+\rho g{{h}_{2}} \\
\Rightarrow {{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}}=\dfrac{\rho {{v}_{2}}^{2}}{2} \\
\Rightarrow v_{2}^{2}=\dfrac{2({{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}})}{\rho } \\
\therefore {{v}_{2}}=\sqrt{\dfrac{2({{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}})}{\rho }} \\ $
So, we have found out the velocity of the liquid at point $ 2 $ , but for maximum possible height, the velocity at that height must be equal to zero, thus,
$ {{v}_{2}}=\sqrt{\dfrac{2({{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}})}{\rho }} \\
\Rightarrow \sqrt{\dfrac{2({{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}})}{\rho }}=0 \\
\Rightarrow {{P}_{1}}-{{P}_{2}}-\rho g{{h}_{2}}=0 \\
\Rightarrow \rho g{{h}_{2}}={{P}_{1}}-{{P}_{2}} \\
\Rightarrow {{h}_{2}}=\dfrac{{{P}_{1}}-{{P}_{2}}}{\rho g} \\ $
But the pressure, $ {{P}_{2}}=0 $
Thus, $ {{h}_{2}}=\dfrac{{{P}_{1}}}{\rho g} $ , putting the values of atmospheric pressure, acceleration due to gravity and density we get,
$ \therefore {{h}_{2}}=\dfrac{{{10}^{5}}}{1000\times 10}=10m $
So, the correct option is (B).
Note:
Sometimes these kinds of problems are also solved using Pascal's law of pressure. Pascal law states that pressure remains the same at the same horizontal level in a liquid. Both the columns are exposed to the atmosphere and the height of the liquid is also given. But that way the problem becomes too complex and that’s why we have invoked Bernoulli's principle here.
Recently Updated Pages
State and explain the law of conservation of linear class 11 physics CBSE
State and explain the law of conservation of linear class 11 physics CBSE
State and explain the how of conservation of linear class 11 physics CBSE
State and explain Newtons second law of motion Derive class 11 physics CBSE
State and explain law of equipartition of energy class 11 physics CBSE
State and explain Keplers law of planetary motion Draw class 11 physics CBSE
Trending doubts
Which are the Top 10 Largest Countries of the World?
Fill the blanks with the suitable prepositions 1 The class 9 english CBSE
Difference Between Plant Cell and Animal Cell
Write a letter to the principal requesting him to grant class 10 english CBSE
What is the full form of AD a After death b Anno domini class 6 social science CBSE
Difference between Prokaryotic cell and Eukaryotic class 11 biology CBSE
Give 10 examples for herbs , shrubs , climbers , creepers
Change the following sentences into negative and interrogative class 10 english CBSE
What is pollution? How many types of pollution? Define it