Problem 59
Question
The period \(T\) of a pendulum of length \(L\) that swings under the influence only of gravity is given approximately by \(T=2 \pi \sqrt{L / g}\), where \(g=9.8\) meters per second squared. a. Write \(L\) as a function of \(T\). b. The length of the Foucault pendulum at the Smithsonian Institution is approximately \(21.8\) meters. Determine its period.
Step-by-Step Solution
Verified Answer
a. \( L(T) = g \left(\frac{T}{2\pi}\right)^2 \)
b. The period is approximately \( 9.37 \) seconds.
1Step 1: Rearrange the Period Formula
The formula for the period of a pendulum is given by \( T = 2\pi \sqrt{\frac{L}{g}} \). To express \( L \) as a function of \( T \), we need to solve for \( L \). First, divide both sides by \( 2\pi \) to isolate the square root: \( \frac{T}{2\pi} = \sqrt{\frac{L}{g}} \).
2Step 2: Eliminate the Square Root
Square both sides of the equation to remove the square root: \( \left(\frac{T}{2\pi}\right)^2 = \frac{L}{g} \).
3Step 3: Solve for L
Multiply both sides by \( g \) to solve for \( L \): \( L = g \left(\frac{T}{2\pi}\right)^2 \). Thus, \( L \) as a function of \( T \) is \( L(T) = g \left(\frac{T}{2\pi}\right)^2 \).
4Step 4: Solve for Period Using Given Length
We need to find the period \( T \) when \( L = 21.8 \) meters. Use the period formula: \( T = 2\pi \sqrt{\frac{L}{g}} \). Substitute \( L = 21.8 \) meters and \( g = 9.8 \text{ m/s}^2 \): \( T = 2\pi \sqrt{\frac{21.8}{9.8}} \).
5Step 5: Calculate the Period
First, calculate the expression inside the square root: \( \frac{21.8}{9.8} \approx 2.2245 \). Then take the square root: \( \sqrt{2.2245} \approx 1.4915 \). Multiply by \( 2\pi \): \( 2\pi \times 1.4915 \approx 9.37 \). Therefore, the period is approximately \( 9.37 \) seconds.
Key Concepts
Solving equationsPhysical constantsRearranging formulas
Solving equations
Solving equations is all about manipulating them to find the value of an unknown variable. If we have an equation, like the pendulum period formula, we follow a series of steps to isolate the desired variable on one side. In our problem, the equation \( T = 2\pi \sqrt{\frac{L}{g}} \) needs to be solved for \( L \) in terms of \( T \). This involves rearranging the equation step by step.
To start, you'd divide both sides by \( 2\pi \), giving you \( \frac{T}{2\pi} = \sqrt{\frac{L}{g}} \). This step isolates the square root term. Next, you must eliminate the square root to solve for \( L \). You achieve this by squaring both sides, resulting in \( \left(\frac{T}{2\pi}\right)^2 = \frac{L}{g} \).
Finally, solve for \( L \) by multiplying both sides by \( g \), leading to \( L = g \left(\frac{T}{2\pi}\right)^2 \). Now, \( L \) is expressed directly as a function of \( T \). Solving equations often uses such systematic steps, allowing us to tackle even complex symbols and expressions.
To start, you'd divide both sides by \( 2\pi \), giving you \( \frac{T}{2\pi} = \sqrt{\frac{L}{g}} \). This step isolates the square root term. Next, you must eliminate the square root to solve for \( L \). You achieve this by squaring both sides, resulting in \( \left(\frac{T}{2\pi}\right)^2 = \frac{L}{g} \).
Finally, solve for \( L \) by multiplying both sides by \( g \), leading to \( L = g \left(\frac{T}{2\pi}\right)^2 \). Now, \( L \) is expressed directly as a function of \( T \). Solving equations often uses such systematic steps, allowing us to tackle even complex symbols and expressions.
Physical constants
Physical constants play a crucial role in equations linking multiple physical quantities. In the pendulum formula \( T = 2\pi \sqrt{\frac{L}{g}} \), \( g \) represents the acceleration due to gravity, a physical constant with a value of approximately 9.8 meters per second squared on the surface of the Earth. This constant characterizes the downward acceleration imparted by gravity on freely falling objects.
Using constants like \( g \) makes calculations reliable because they provide a universal reference point for comparing and predicting results. In any pendulum equation,\( g \) helps in understanding how fast an object will swing under the sole influence of gravity, without any external force.
Thus, physical constants are fundamental to applying laws of physics across various scenarios, ensuring consistency in scientific predictions and equations.
Using constants like \( g \) makes calculations reliable because they provide a universal reference point for comparing and predicting results. In any pendulum equation,\( g \) helps in understanding how fast an object will swing under the sole influence of gravity, without any external force.
Thus, physical constants are fundamental to applying laws of physics across various scenarios, ensuring consistency in scientific predictions and equations.
Rearranging formulas
Rearranging formulas is essential to express quantities differently, often needed in solving physics problems. Here, the pendulum period formula \( T = 2\pi \sqrt{\frac{L}{g}} \) needs rearrangement to solve for different variables. This flexibility is valuable when the problem gives quantities we must use differently from how the formula is originally presented.
To rearrange, we follow these principles:
Rearranging formulas is therefore not only a technical skill but also a conceptual tool to illuminate relationships between different academic subjects, like mathematics and physics.
To rearrange, we follow these principles:
- Isolate the term containing the variable of interest (e.g., \( L \)).
- Use algebraic operations such as division, multiplication, and squaring to further manipulate the formula.
- Maintain equality by applying the same operation to both sides of the formula.
Rearranging formulas is therefore not only a technical skill but also a conceptual tool to illuminate relationships between different academic subjects, like mathematics and physics.
Other exercises in this chapter
Problem 59
Solve the inequality. $$ |x-2|
View solution Problem 59
Sketch the region in the plane satisfying the given conditions. \(x4\)
View solution Problem 59
The gravitational force \(F\) that the earth exerts on a unit mass depends on whether the mass is inside or outside the earth. Let \(R\) denote the radius of th
View solution Problem 60
Show that the points twice as far from the point \((2,-3)\) as from the point \((-1,0)\) form a circle, and find the center and radius of that circle.
View solution