Physics Test Help: Fluid Mechanics Questions

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Fluid mechanics concepts are crucial for understanding Bernoulli's equation, which states that the sum of kinetic, pressure, and potential energy in a fluid flow remains constant. This constant can be used to relate different points in the flow to solve for unknown variables. The equation of continuity indicates that the product of the cross-sectional area and fluid velocity remains constant, allowing for calculations of fluid behavior in varying pipe sizes. For the sample problems, the speed of water exiting a hole can be determined using Bernoulli's equation, while the tension in a string holding an immersed object can be calculated using basic principles of buoyancy and weight. Mastering these concepts will aid in preparing for the physics test on fluid mechanics and related topics.
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Hey, I have a test tomorrow and though I understand most of what is on the test, Fluid mechanics is giving me some problems. I've read the chapter through and have a few questions.

1) When they say Bernoulli's equation is \frac{1}{2} \rho V^2 + P{o} + \rho g h = constant or anything else for that matter, what does constant mean? When do I set it equal to itself? What can I do with it being equal to constant?

2) What is the equation of continuity for fliuds? How is it useful?

And I have 2 sample problem which would fantastic if you guys could show me how to solve them? That way I can print out the post and head to the library and go over the problems and try them myself.

Here they are:

1) A large storage tank, open at the top and filled with water, develops a small hole in its side at a point 16.0m below the water level. If the rate of flow from the leak is equal to 2.50 x 10^-3 m^3 per min(sorry i can't get the TeX working for this), determine (a) the speed at which the water leaves the hole and (b) the diameter of the hole.

2) A piece of aluminum with mass 1.00 kg and density 2,700 kg/m^3 is suspended from a string and then completely immersed in a container of water. Calculate the tension in the string (a) before and (b) after the metal is immersed.

Thank you in advance. I am going to the library to study for a couple of hours, so I will come back and check the website when I return to my room. Then I'll head back to the library to study fluids, lol.

The test is on angular momentum, static equilibrium, universal gravitation, fluid mechanics, and oscillatory motion, so any pointers on those topics you can throw in would be great. Thanks.
 
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1) The constant in Bernoulli's equation is a constant of integration, meaning that it is a value that can be determined if two of the above values are known. It is equal to itself because it is a constant, and you can use it to find the relationship between pressure, velocity, and height. 2) The equation of continuity for fluids states that the rate of flow through a given area must remain constant. This equation is useful for finding the velocity of a fluid at different points, given that the flow rate is known. For the sample problems:1) The speed at which the water leaves the hole can be found by utilizing Bernoulli's equation with the given information. Bernoulli's equation states that 1/2ρV^2 + Po + ρgh = constant. Since the pressure of the tank is atmospheric pressure, Po is equal to 0. Since the water level is 16 meters below the hole, h is equal to 16. Since the rate of flow is 2.50x10-3 m^3/min, we can use this to find the velocity. Rearranging the equation to solve for V, we get V = sqrt(2*2.50x10-3/(ρ*16)). Substituting the density of water, 1000 kg/m^3, into the equation gives V = 0.735 m/s. To find the diameter of the hole, we can use the equation for the volume flow rate of a hole, Q = CdA, where Cd is the coefficient of discharge and A is the area of the hole. Rearranging the equation to solve for A gives A = Q/Cd. Substituting the flow rate and the coefficient of discharge, 0.61, gives A = 0.00408 m^2. Finally, we can use the equation for the area of a circle, A=πr^2, to solve for the radius of the hole, giving r = 0.0491 m. Therefore, the diameter of the hole is approximately 0.098 m. 2) For part (a) of this problem, we can use the equation for the tension in a string, T = mg. Substituting the mass and acceleration due to gravity, 9.8 m/s^2, gives T = 980 N
 


Hi there, thank you for reaching out for help with your physics test. Fluid mechanics can be a tricky topic, so it's great that you are taking the time to review and ask questions before your test. Let's go through your questions and sample problems to see if we can help you understand fluid mechanics better.

1) When they say Bernoulli's equation is \frac{1}{2} \rho V^2 + P{o} + \rho g h = constant, the "constant" refers to the sum of the kinetic energy, pressure energy, and potential energy of a fluid at any point in a flow. This means that as the fluid moves through different points in a flow, the sum of these energies remains constant. In terms of setting it equal to itself, this is usually done when you are solving problems involving Bernoulli's equation. You would set the equation equal to itself at two different points in a flow and then solve for the unknown variables. As for what you can do with the equation being equal to a constant, you can use it to calculate different properties of the fluid at different points in a flow, such as velocity or pressure.

2) The equation of continuity for fluids is A_1v_1 = A_2v_2, where A represents the cross-sectional area of a pipe or tube, and v represents the velocity of the fluid. This equation is useful because it shows the relationship between the velocity and cross-sectional area of a fluid in a pipe or tube. For example, if the cross-sectional area of a pipe decreases, the velocity of the fluid must increase in order to maintain the same flow rate.

Now, let's take a look at your sample problems:

1) To solve this problem, we can use the equation of continuity. We know that the flow rate, Q, is equal to 2.50 x 10^-3 m^3/min. We also know that the cross-sectional area of the hole is equal to the area of a circle, A = πr^2, where r is the radius of the hole. Since the tank is open at the top, we can assume that the water level remains constant, so the cross-sectional area of the tank is also equal to πr^2. Using the equation of continuity, we can set the flow rate at the hole equal to the flow rate at the top of the tank, and solve for the velocity v at the hole:

Q
 
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