Accelerated Pendulum: Exploring Fh & Fd

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In summary: The string exerts a horizontal force Fh on the pendulum, and a vertical force Fv at the fulcrum. The pendulum also experiences an acceleration due to the downward pull of the string.
  • #1
mrueedi
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I have a strange question and have internet-wide not found answers:

An ideal pendulum hanging straight down gets a sidewards force Fh attacking at the pivot point.
The whole pendulum starts accelerating along Fh.

Fh: sidewarts force at the pivot point
Fd: horizontal force attacking at the pendulum C/G that causes the pendulum to deflect
alpha: deflection angle
m: pendulum mass

Fd = m*g / tan (alpha)

Now, how much does the pendulum deflect?

The feelings says the pendulum remains deflected as long as Fh causes a constant acceleration.

But, when the pendulum is deflected from where comes the force Fd (deflection force, opposite direction of Fh)? Fd can not be equal to Fh (because that would cause the acceleration to stop).
Is Fd smaller than Fh causing a slower acceleration (compared to Fh attacking directly a body with mass m)?
Is there a Fd at all? If not, remains the pendulum really hanging straight down?

Only a constant Fh shall be considered (no dynamic deflections because of the initial Fh step).
 
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  • #2
mrueedi said:
I have a strange question and have internet-wide not found answers:

An ideal pendulum hanging straight down gets a sidewards force Fh attacking at the pivot point.
The whole pendulum starts accelerating along Fh.

Fh: sidewarts force at the pivot point
Fd: horizontal force attacking at the pendulum C/G that causes the pendulum to deflect
alpha: deflection angle
m: pendulum mass

Fd = m*g / tan (alpha)

Now, how much does the pendulum deflect?

The feelings says the pendulum remains deflected as long as Fh causes a constant acceleration.
I imagine a massless support free to slide along a frictionless table, from which the pendulum hangs. A horizontal force acts on the support.
But, when the pendulum is deflected from where comes the force Fd (deflection force, opposite direction of Fh)?
Viewed from an inertial frame, there's no need for a "deflection force"--the pendulum is being accelerated.
Fd can not be equal to Fh (because that would cause the acceleration to stop).
Is Fd smaller than Fh causing a slower acceleration (compared to Fh attacking directly a body with mass m)?
Viewed from the non-inertial frame of the pendulum, there will be a "pseudoforce" exactly equal and opposite to Fh acting on the pendulum bob. Note that Fh does not act on the bob, it acts on the support, so those two forces don't "cancel out".
 
  • #3
Thank you very much for the answer!
Doc Al said:
Viewed from the non-inertial frame of the pendulum, there will be a "pseudoforce" exactly equal and opposite to Fh acting on the pendulum bob. Note that Fh does not act on the bob, it acts on the support, so those two forces don't "cancel out".

Ok, but once the deflection becomes stable that "pseudoforce" Fd works against Fh (if I observe from an inertial frame). But because the whole pendulum is accelerating, a net force to the side must exist.

I would expect that any Fd reduces the achievable acceleration. At the same time Fd can not have the equal and opposite size as Fh otherwise the whole pendulum would stop accelerating.
 
  • #4
mrueedi said:
Ok, but once the deflection becomes stable that "pseudoforce" Fd works against Fh (if I observe from an inertial frame). But because the whole pendulum is accelerating, a net force to the side must exist.
If you observe from an inertial frame, there is no pseudoforce. (The pseudoforce is only an artifact of observing things in a non-inertial frame.) There is certainly a net force to the side: Fh.
I would expect that any Fd reduces the achievable acceleration. At the same time Fd can not have the equal and opposite size as Fh otherwise the whole pendulum would stop accelerating.
Again, the pseudoforce (what you call Fd) only exists within the non-inertial frame of the pendulum. But with respect to that frame, the pendulum is not accelerating: the net force (including both real and pseudo forces) is zero.
 
  • #5
Thanks for your patience. I still am unsure. My focus is on the deflection.

Doc Al said:
If you observe from an inertial frame, there is no pseudoforce. (The pseudoforce is only an artifact of observing things in a non-inertial frame.) There is certainly a net force to the side: Fh.

If there is no pseudoforce (looking from inertial frame): -> no deflection? Is that right?

Imagine a crane with a trolley (like on this link
http://www.towercranetraining.co.uk/towercranetypes_files/image004.jpg ):

M is loaded on the hook and the trolley starts accelerating steadily to the right:
Is there a steady deflection alpha from the vertical for the hook & m?
 
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  • #6
mrueedi said:
If there is no pseudoforce (looking from inertial frame): -> no deflection? Is that right?
I don't understand what you are trying to say.

There is never a pseudoforce when viewing from an inertial frame. Pseudoforces only arise in non-inertial frames.

No matter which frame you use to describe the situation, everyone agrees (of course!) that the pendulum bob is deflected when the apparatus is accelerated.

Try this: Describe the forces that are exerted on the pendulum bob. (Use an inertial frame.)

Imagine a crane with a trolley (like on this link
http://www.towercranetraining.co.uk/towercranetypes_files/image004.jpg ):

M is loaded on the hook and the trolley starts accelerating steadily to the right:
Is there a steady deflection alpha from the vertical for the hook & m?
Sure. (Ignoring oscillations, of course.)
 
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1. What is an accelerated pendulum?

An accelerated pendulum is a type of pendulum that is subject to an additional force, called the driving force (Fd), that causes it to move faster than a traditional pendulum. This force can be applied at different points in the pendulum's motion, resulting in different patterns and behaviors.

2. What is the relationship between Fh and Fd in an accelerated pendulum?

Fh and Fd are both forces that act on an accelerated pendulum, but they have different effects. Fh, or the restoring force, is what brings the pendulum back to its equilibrium position. Fd, or the driving force, is what causes the pendulum to accelerate and move faster. The relationship between the two forces determines the behavior of the pendulum.

3. How can an accelerated pendulum be used to explore Fh and Fd?

By varying the amplitude and frequency of the driving force, and observing how the pendulum responds, we can gain a better understanding of the relationship between Fh and Fd. We can also use mathematical models and simulations to analyze and predict the behavior of the pendulum under different conditions.

4. What are the real-world applications of studying accelerated pendulums?

Studying accelerated pendulums can have applications in fields such as physics, engineering, and mechanics. It can help us better understand the behavior of systems subject to external forces and how they respond to different stimuli. This knowledge can be applied to various technologies and machines, such as clocks, engines, and bridges.

5. What are some factors that can affect the behavior of an accelerated pendulum?

The behavior of an accelerated pendulum can be influenced by several factors, such as the amplitude and frequency of the driving force, the length of the pendulum, and the presence of other external forces, such as air resistance. Additionally, the material and design of the pendulum can also affect its behavior and response to Fh and Fd.

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