How Does D'Alembert's Principle Determine Static Equilibrium?

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In summary, d'Alembert's principle can be used to find the conditions of static equilibrium by considering the forces and coordinates of the system. The principle states that the net force acting on a body is equal to its mass times its acceleration, and in the case of static equilibrium, this simplifies to the sum of the applied force, tension in the string, and force of gravity being equal to zero.
  • #1
dowjonez
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Q. use d'alemberts principal to find the condition of static equilibrium

so

i prolly want to look at the coordinates of the system with respect to theta

x = L sin Theta where L is the length of the string

y = - L cos theta


(Fapplied - Finertial) delta r = 0

Im guessing the F applied is both the horizontal force and the force of gravity

and that the inertial force is m * L * theta (double dot)


delta r = L * delta theta


so I am just wildly guessing that

(Fapplied - Finertial) delta r = 0
(Fsin theta + mg cos theta - m * L * theta (double dot) ) delta r = 0


i know I am wrong but maybe someone can tell me what I am doing wrong
 
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  • #2


Hello,

Thank you for your question. The d'Alembert's principle is a fundamental principle in classical mechanics that states that the net force acting on a body is equal to its mass times its acceleration. In the context of static equilibrium, this principle can be used to find the conditions under which a system is in equilibrium.

To apply d'Alembert's principle, we first need to define the forces acting on the system. In this case, we have a mass attached to a string, so the forces acting on the system are the tension in the string, the force of gravity, and any applied forces.

Next, we need to define the coordinates of the system. In this case, we can use the coordinates you mentioned, x = L sin Theta and y = -L cos Theta.

Now, we can write out the d'Alembert's principle as follows:

(Fapplied + T - mg) + m * (x double dot + y double dot) = 0

Where T is the tension in the string, mg is the force of gravity, and m * (x double dot + y double dot) represents the inertial force.

Since we are looking for the conditions of static equilibrium, we know that the acceleration of the system is zero, so we can simplify the equation to:

(Fapplied + T - mg) = 0

This means that for the system to be in equilibrium, the sum of the applied force, the tension in the string, and the force of gravity must be equal to zero.

I hope this helps to clarify how to use d'Alembert's principle to find the conditions of static equilibrium. Let me know if you have any further questions. Good luck with your research!
 
  • #3



I can provide a more accurate explanation of D'alembert's Principal and how it can be used to find the condition of static equilibrium. D'alembert's Principal is a fundamental principle in classical mechanics that states that for any system in equilibrium, the sum of the applied forces and the inertial forces must equal zero. In other words, the net force on the system must be zero for it to be in a state of static equilibrium.

To use D'alembert's Principal to find the condition of static equilibrium, we first need to define our coordinate system. In the given example, the coordinates are defined with respect to theta, with x = L sin theta and y = -L cos theta. This means that the position of the system can be described by the angle theta.

Next, we need to consider the forces acting on the system. In this case, there are two forces - the applied force (Fapplied) and the inertial force (Finertial). The applied force can be broken down into its x and y components, Fapplied = Fsin theta + mg cos theta, where F is the horizontal force and mg is the force of gravity acting downward.

The inertial force is given by m * L * theta (double dot), where m is the mass of the system and theta (double dot) is the angular acceleration. This represents the force needed to accelerate the system from its current position to its equilibrium position.

Now, applying D'alembert's Principal, we can write the equation:

(Fapplied - Finertial) delta r = 0

Substituting in the values for Fapplied and Finertial, we get:

(Fsin theta + mg cos theta - m * L * theta (double dot)) delta r = 0

Since delta r = L * delta theta, we can simplify the equation to:

(Fsin theta + mg cos theta - m * L * theta (double dot)) = 0

This is the condition for static equilibrium, where the net force on the system is equal to zero.

In conclusion, D'alembert's Principal is a useful tool for analyzing systems in equilibrium and can help us determine the condition for static equilibrium. By considering the applied forces and the inertial forces, we can use this principle to find the equilibrium condition for a given system.
 

Related to How Does D'Alembert's Principle Determine Static Equilibrium?

What is D'alembert's Principal?

D'alembert's Principal is a principle in classical mechanics that states that the net force acting on a system is equal to the mass of the system multiplied by its acceleration, or F=ma. It is often used to solve problems involving the motion of particles or rigid bodies.

Who developed D'alembert's Principal?

D'alembert's Principal was developed by the French mathematician and physicist Jean le Rond d'Alembert in the 18th century.

How is D'alembert's Principal used in mechanics?

D'alembert's Principal is used to simplify problems involving the motion of particles or rigid bodies by reducing them to a single equation, F=ma. This can help in solving for unknown forces or accelerations in a system.

What are the limitations of D'alembert's Principal?

D'alembert's Principal is based on the assumption that the system is in equilibrium or moving at a constant velocity, and does not account for non-conservative forces such as friction. It also only applies to systems with constant mass and does not take into account relativistic effects.

What are some real-world applications of D'alembert's Principal?

D'alembert's Principal is used in various fields of engineering, such as structural analysis, dynamics, and fluid mechanics. It is also used in the design of mechanical systems, such as engines and vehicles, to predict the forces and accelerations acting on different components.

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