Conceptual Questions Fluids and Simple Harmonic motion

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SUMMARY

This discussion addresses the simultaneous use of the equation of continuity and Bernoulli's equation in fluid dynamics, specifically in problems involving streamlined fluid flow, such as flow through pipes with varying height and cross-sectional area. It also clarifies the phase relationship in simple harmonic motion, explaining that the velocity of an oscillating object is shifted to the left of the displacement by π/2 radians. This phase shift occurs because maximum velocity coincides with zero displacement at the equilibrium point of the oscillation.

PREREQUISITES
  • Understanding of Bernoulli's equation and its applications in fluid dynamics.
  • Familiarity with the equation of continuity (A1V1 = A2V2).
  • Knowledge of simple harmonic motion and its mathematical representation (x(t) = xmaxcos(wt + phi)).
  • Basic concepts of oscillation and phase relationships in sinusoidal functions.
NEXT STEPS
  • Study the applications of Bernoulli's equation in real-world fluid flow scenarios.
  • Explore the derivation and implications of the equation of continuity in fluid mechanics.
  • Investigate the mathematical properties of simple harmonic motion, focusing on phase shifts and their graphical representations.
  • Learn about the energy transformations in simple harmonic motion and their relation to displacement and velocity.
USEFUL FOR

Students studying physics, particularly those focusing on fluid dynamics and oscillatory motion, as well as educators seeking to clarify these concepts for their learners.

vivekfan
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Homework Statement



1. Do you use the equation of continuity and Bernoulli's equation simultaneously in a question? When do you use them?

2. In simple harmonic motion, why is the velocity shifted to left of the displacement by pi/4?

Homework Equations



pressure + .5density x velocity ^2 + density x g x y (initial)= the same thing (final)

A1V1=A2V2 (continuity)

x(t)=xmaxcos(wt + phi) here w=omega


The Attempt at a Solution



I've been reading my book, but I am confused about these issues. Please help.
 
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vivekfan said:
1. Do you use the equation of continuity and Bernoulli's equation simultaneously in a question?
Sure.
When do you use them?
In all sorts of problems involving streamlined fluid flow. For example, flow through a pipe of varying height and cross-sectional area.

2. In simple harmonic motion, why is the velocity shifted to left of the displacement by pi/4?
I think you mean pi/2. To see this, imagine a ball on a spring oscillating back and forth along the x axis. When it passes through the equilibrium point (going towards +x, say) its speed is at its maximum positive value while the displacement is at zero. When it gets to maximum displacement, the speed now is zero. When it returns to equilibrium, its displacement is again zero, but the speed is maximum negative. And so on. Sketch out the diagrams of displacement and velocity (both sinusoids) and you'll see that the velocity graph looks exactly like the displacement graph, just slid over to the left by pi/2.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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