Chapter 2: Problem 27
An 18 -foot ladder leans against a 12 -foot vertical wall, its top extending over the wall. The bottom end of the ladder is pulled along the ground away from the wall at 2 feet per second. (a) Find the vertical velocity of the top end when the ladder makes an angle of \(60^{\circ}\) with the ground. (b) Find the vertical acceleration at the same instant.
Short Answer
Step by step solution
Identify Known Values
Set Up the Right Triangle
Use Trigonometry to Find x and y
Differentiate the Triangle Equation
Solve for Vertical Velocity (dy/dt)
Differentiate the Velocity Equation for Acceleration
Solve for Vertical Acceleration (d²y/dt²)
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Trigonometry
In the exercise, the ladder makes an angle of 60° with the ground. We can use trigonometric functions to find the lengths of the sides adjacent and opposite to the angle. Specifically:
- Cosine gives us the ratio of the adjacent side to the hypotenuse. So, \cos(60°) = \frac{x}{18}\, where \(x\) is the distance from the wall.
- Sine gives the ratio of the opposite side to the hypotenuse. So, \sin(60°) = \frac{y}{18}\, where \(y\) is the vertical height to the wall.
Pythagorean Theorem
In our problem, the ladder represents the hypotenuse of a right triangle formed against a wall. The theorem allows us to express the relationship between the horizontal distance \(x\) and the vertical height \(y\).
For our triangle:
- \(x^2 + y^2 = 18^2\).
- This simplifies to \(x^2 + y^2 = 324\).
Differentiation
The differentiation process begins by applying the Pythagorean relationship: \x^2 + y^2 = 324\. To capture how these lengths vary, we differentiate implicitly with respect to time. The differentiated equation is \2x\frac{dx}{dt} + 2y\frac{dy}{dt} = 0\.
- Here, \(\frac{dx}{dt}\) represents the rate at which the distance \(x\) changes, known to be 2 feet per second.
- \(\frac{dy}{dt}\) is what we solve for, representing the vertical velocity of the ladder.
Kinematics
Once we find the vertical velocity (\(\frac{dy}{dt}\)), we can differentiate again to find the acceleration, using:
- \(\frac{d}{dt}(18\sqrt{3}\frac{dy}{dt}) = 0\).
- This leads to \(18\sqrt{3}\frac{d^2 y}{dt^2} = 0\).