Problem 72
Question
MODELING Speed of a Skydiver If air resistance is not ignored during free fall, then the speed (in feet per second) of a skydiver after \(t\) seconds is given by $$ f(t)=176\left(1-e^{-a 2 t}\right) $$ Calculate \(\lim _{t \rightarrow x^{\infty}} f(t)\) and give an interpretation of its value. (IMAGES CANNOT COPY).
Step-by-Step Solution
Verified Answer
The limit is 176; it represents the skydiver's terminal velocity.
1Step 1: Understanding the Limit
The problem asks for the limit of the function \( f(t) = 176(1 - e^{-a2t}) \) as \( t \) approaches infinity. The goal is to find the behavior of the function when \( t \) becomes very large.
2Step 2: Analyzing the Exponential Term
As \( t \to \infty \), the term \( e^{-a2t} \) will tend to zero because \( e^{-x} \to 0 \) as \( x \to \infty \). This is a key property of exponential decay.
3Step 3: Substitute and Simplify
By substituting as \( t \to \infty \), the expression becomes: \[ f(t) = 176 \times (1 - 0) = 176. \] Thus, the limit is 176.
4Step 4: Interpretation of the Limit
The limit of 176 represents the terminal velocity of the skydiver. This is the maximum speed the skydiver can reach when air resistance balances out gravitational acceleration.
Key Concepts
Exponential DecayTerminal VelocityFree Fall Dynamics
Exponential Decay
In many natural processes, exponential decay plays a crucial role in governing how quickly things change over time. It appears when something decreases at a rate proportional to its current value. A primary example of this is seen in the decay term of the function, where we use the expression \(e^{-a2t}\).
This expression indicates that as time \(t\) increases, the term \(e^{-a2t}\) becomes very small, closely approaching zero. This happens because the exponent is negative and increasingly large, driving the entire term toward zero.
This expression indicates that as time \(t\) increases, the term \(e^{-a2t}\) becomes very small, closely approaching zero. This happens because the exponent is negative and increasingly large, driving the entire term toward zero.
- Exponential decay ensures that quantities decrease rapidly at first, but the rate of decrease slows over time.
- The remaining term in the function, \(176(1 - e^{-a2t})\), allows us to determine the speed of the skydiver.
- The "\(-a2t\)" signifies how powerful the decay effect is, which depends on the specific constant values like air resistance and other dynamic variables.
Terminal Velocity
Terminal velocity refers to the constant speed that a falling object eventually reaches when the force of gravity is balanced by the resistive forces, like air resistance. In the scenario of skydivers falling through the air, terminal velocity is reached when air resistance negates further acceleration due to gravity.
This is evident in the limit of the skydiver's speed function, where as time progresses towards infinity, the function's value stabilizes. The formula \( f(t) = 176 \times (1 - e^{-a2t}) \) simplifies to \(176\) as the exponential term vanishes. Here's what this means:
This is evident in the limit of the skydiver's speed function, where as time progresses towards infinity, the function's value stabilizes. The formula \( f(t) = 176 \times (1 - e^{-a2t}) \) simplifies to \(176\) as the exponential term vanishes. Here's what this means:
- The speed settles at 176 feet per second, which is the terminal velocity.
- The balance occurs because the accelerating force of gravity is opposed by the increasing force of air resistance.
- This maximum speed is unique to each scenario, factoring in mass and surface area.
Free Fall Dynamics
Free fall dynamics describes the motion of objects when gravity is the only force acting on them. However, in real-world conditions, air resistance significantly affects this motion.
In the case of a skydiver, the free fall is modified by factors like air friction, leading to the actual movement modeled by functions such as \( f(t) = 176(1 - e^{-a2t}) \). Let's explore these dynamics further:
In the case of a skydiver, the free fall is modified by factors like air friction, leading to the actual movement modeled by functions such as \( f(t) = 176(1 - e^{-a2t}) \). Let's explore these dynamics further:
- Initially, the skydiver accelerates rapidly due to gravity when air resistance is minimal.
- As they gain speed, air resistance increases, reducing the net force and slowing acceleration.
- Eventually, terminal velocity is achieved, and speed levels off.
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