Pendulum involving conservative energy

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SUMMARY

The discussion centers on calculating the maximum height (H) reached by a pendulum-like ball subjected to a constant wind force (F). The derived formula is H = (2L)/(1+(mg/F)^2), where m is the mass of the ball, L is the string length, and g is the acceleration due to gravity (9.8 m/s²). The analysis incorporates the forces acting on the ball, including gravitational force (mg) and the wind force (F), and utilizes the conservation of energy principle to derive the relationship between these variables. The discussion also confirms the validity of the formula for different height scenarios.

PREREQUISITES
  • Understanding of pendulum motion and forces acting on a pendulum
  • Knowledge of conservation of energy principles in physics
  • Familiarity with trigonometric functions and their applications in physics
  • Basic calculus for integrating work done by forces
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  • Study the derivation of the pendulum motion equations, focusing on the effects of external forces
  • Learn about the conservation of energy in mechanical systems and its applications
  • Explore the impact of varying forces on oscillatory motion, particularly in pendulum systems
  • Investigate the mathematical implications of integrating forces in physics problems
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Physics students, educators, and anyone interested in understanding the dynamics of pendulum systems affected by external forces, particularly in mechanics and energy conservation contexts.

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Hey! I need help with this question:
A ball having mass m is connected by a strong string of length L to a pivot point and held in place in a vertical position. A wind exerting constant force of magnitude F is blowing from left to right. If the ball is released from rest, show that the maximum height H reached by the ball, as measured from its initial height, is H= (2L)/(1+(mg/F)^2) Check that the above result is valid both for cases when 0<H,L and for L<H<2L.
So far, I know that I'm supposed to use FLsin(theta)=mgH
and integrate it -> W=(integral)FLcos(theta)d(theta)
But I have no idea at all where to go from here! Please, i really need help now! I don't have much time left for this! :cry:
 
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insertnamehere said:
Hey! I need help with this question:
A ball having mass m is connected by a strong string of length L to a pivot point and held in place in a vertical position. A wind exerting constant force of magnitude F is blowing from left to right. If the ball is released from rest, show that the maximum height H reached by the ball, as measured from its initial height, is H= (2L)/(1+(mg/F)^2) Check that the above result is valid both for cases when 0<H,L and for L<H<2L.
So far, I know that I'm supposed to use FLsin(theta)=mgH
and integrate it -> W=(integral)FLcos(theta)d(theta)
But I have no idea at all where to go from here! Please, i really need help now! I don't have much time left for this! :cry:
The solution to the pendulum motion without the wind is:

[tex]\theta = \theta_0,sin(\omega t)[/tex] where [itex]\omega = \sqrt{g/L}[/itex]

When you add the wind, the energy added on the forward cycle is lost on the reverse cycle so this is equivalent to a new vibration about a different equilibrium position in which the new g' is determined from the vector sum of mg and F.

[tex]g' = \sqrt{g^2 +(F/m)^2}[/tex] and

[tex]\theta_0' [/itex] is the angle that the vector sum of F and mg makes to the vertical. Try working out H from that.<br /> <br /> AM[/tex]
 


Sure, I can help you with this question. Let's break it down step by step.

First, let's define some variables:
m = mass of the ball
L = length of the string
F = magnitude of the wind force
H = maximum height reached by the ball
g = acceleration due to gravity (9.8 m/s^2)

Now, let's look at the forces acting on the ball. We have the weight force (mg) acting downwards, and the wind force (F) acting horizontally. Since the ball is released from rest, there is no initial velocity and no kinetic energy, so all of the energy is in the form of potential energy. This means we can use the conservation of energy principle, which states that the total energy of a system remains constant.

We can express this principle as:
Initial energy = Final energy

At the initial position, the ball is at rest and has no potential energy, so the initial energy is 0. At the final position, the ball has reached its maximum height H and has potential energy equal to mgh. Therefore, we can write:

0 = mgh

Now, let's look at the work done by the wind force. We know that work is equal to force times distance, so we can write:

Work = F * L

But we also know that work is equal to the change in energy, so we can write:

Work = Final energy - Initial energy

Substituting in our values, we get:

F * L = mgh - 0

Solving for h, we get:

h = FL/mg

Now, we can use this value for h in our initial equation and solve for H, the maximum height reached by the ball:

H = FL/mg + L

But we also know that FLsin(theta) = mgH, so we can substitute this in and solve for H:

H = (FLsin(theta))/mg + L

Since sin(theta) is always less than or equal to 1, we can say that:

H ≤ (FL)/mg + L

Now, let's look at the two cases given in the question:
1. 0 < H, L
2. L < H < 2L

For case 1, since L < H, we can say that (FL)/mg + L < H. Therefore, the maximum height reached by the ball is less than the value we calculated, which
 

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