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Visualized Solution
The Sigma Insight: Work Done by Forces
The Setup
Visualizing the Pendulum
Imagine a simple pendulum hanging straight down. Now, we apply a horizontal force to slowly push it aside until it makes a angle with the vertical. Our goal is to find the exact magnitude of this horizontal force in terms of the mass and gravity .
To solve this, we need to look at the energy of the system. Since the mass is displaced slowly, it doesn't gain any speed. This means its initial and final kinetic energies are both zero.
The Master Equation
Work-Energy Theorem
This is a perfect scenario for the Work-Energy Theorem, which states that the net work done by all forces on an object equals its change in kinetic energy:
Since the mass is displaced slowly, . Therefore, the sum of the work done by all forces must be zero.
Breaking Down the Work Done
Let's identify the forces acting on the mass and calculate the work done by each:
1. Tension (): The tension in the string always acts along the string, pointing towards the pivot. As the mass moves along the circular arc, its instantaneous displacement is always tangential to the arc. Since the radius (tension) and tangent (displacement) are always perpendicular, the work done by tension is zero: .
2. Applied Horizontal Force (): Work is defined as force multiplied by the displacement in the direction of the force. The force is purely horizontal. Using basic trigonometry, the horizontal displacement of the mass when it reaches an angle is . Thus, the work done by is positive:
3. Gravity (): Gravity acts straight down. The mass, however, is moving upwards against gravity. The initial vertical depth of the mass is . At , its vertical depth is . The vertical height it has gained is the difference: . Because gravity and the vertical displacement are in opposite directions, the work done by gravity is negative:
The Final Calculation
Now, we plug these work values back into our Work-Energy equation:
Let's substitute the known values for and , which are both :
Notice how the length of the string appears in every term? We can safely cancel it out. This tells us a beautiful physical truth: the required force doesn't depend on how long the string is!
To isolate , we multiply the entire equation by :
And there we have it! The horizontal force required to slowly displace the pendulum to is exactly .
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