Problem 58
Question
An object with weight \(W\) is dragged along a horizontal plane by a force acting along a rope attached to the object. If the rope makes an angle \(\theta\) with the plane, then the magnitude of the force is $$F=\frac{\mu W}{\mu \sin \theta+\cos \theta}$$ where \(\mu\) is a positive constant called the coefficient of friction and where 0\(\leqslant \theta \leqslant \pi / 2 .\) Show that \(F\) is minimized when \(\tan \theta=\mu\)
Step-by-Step Solution
Verified Answer
The force \(F\) is minimized when \(\tan \theta = \mu\).
1Step 1: Understanding the Problem
We need to show that the force \(F = \frac{\mu W}{\mu \sin \theta + \cos \theta}\), is minimized when \(\tan \theta = \mu\). Our goal is to find the condition for \(\theta\) that minimizes \(F\).
2Step 2: Expressing the Function
The function to minimize is \(F(\theta) = \frac{\mu W}{\mu \sin \theta + \cos \theta}\). We'll focus on minimizing the denominator, \(D(\theta) = \mu \sin \theta + \cos \theta\), since \(W\) is constant.
3Step 3: Finding the Derivative of the Denominator
Differentiate the denominator with respect to \(\theta\):\[ D'(\theta) = \mu \cos \theta - \sin \theta \]
4Step 4: Setting the Derivative to Zero for Critical Points
Solve \(D'(\theta) = 0\):\[ \mu \cos \theta = \sin \theta \]This gives us the ratio \(\tan \theta = \mu\).
5Step 5: Second Derivative Test for Minimization
Find the second derivative of \(D(\theta)\):\[ D''(\theta) = -\mu \sin \theta - \cos \theta \]At \(\tan \theta = \mu\), check the sign of \(D''(\theta)\). Since \(D''(\theta)\) results in negative, \(D(\theta)\) is minimized, thus minimizing \(F(\theta)\).
6Step 6: Conclusion
Thus, the force \(F\) is minimized when \(\tan \theta = \mu\). This occurs when the angle \(\theta\) makes \(F(\theta)\) as low as possible.
Key Concepts
Coefficient of FrictionMinimization ProblemTrigonometry in Physics
Coefficient of Friction
The coefficient of friction, denoted as \( \mu \), is a crucial factor in understanding the resistance encountered when two surfaces slide against each other. It is a dimensionless constant that represents the frictional force between two particular surfaces. In this exercise, \( \mu \) affects how much force is required to move an object across a horizontal plane. A higher \( \mu \) indicates greater resistance to movement, requiring more force to drag the object.
- Coefficient of static friction: prevents motion from starting.
- Coefficient of kinetic friction: resists motion while sliding.
Minimization Problem
Solving a minimization problem means finding the point where a function reaches its lowest value. In this case, we are looking for the angle \( \theta \) that minimizes the force \( F \).
- We express \( F = \frac{\mu W}{\mu \sin \theta + \cos \theta} \), relying on trigonometric components to find the minimal force.
- The focus is on the denominator, \( \mu \sin \theta + \cos \theta \), since minimizing the denominator will also minimize \( F \).
- By taking the derivative \( D'(\theta) = \mu \cos \theta - \sin \theta \) and setting it to zero, we find the critical point \( \tan \theta = \mu \).
- Checking the second derivative \( D''(\theta) \) ensures that this critical point is a minimum.
Trigonometry in Physics
Trigonometry allows us to analyze angles and relationships in physical scenarios, especially in calculating forces like in this exercise. Here, angles and trigonometric functions are essential:
- Understanding \( \sin \theta \) and \( \cos \theta \) is critical because they describe the components of the angle \( \theta \).
- Using \( \tan \theta = \frac{\sin \theta}{\cos \theta} \) helps determine the optimal \( \theta \) that minimizes \( F \).
- Tying \( \theta \) to \( \mu \) directly relates friction properties with angular position, thereby optimizing motion control.
Other exercises in this chapter
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