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Ch. 8 - Integration Techniques
Briggs - Calculus: Early Transcendentals 3rd Edition
Briggs3rd EditionCalculus: Early TranscendentalsISBN: 9780136847243Non è quello che usi tu?Cambia libro di testo
Capitolo 8, Problema 8.5.94c

94. [Use of Tech] Skydiving A skydiver has a downward velocity given by v(t) = V_T [(1 - e^(-2gt/V_T))/(1 + e^(-2gt/V_T))],
where t = 0 is the instant the skydiver starts falling, g = 9.8 m/s² is the acceleration due to gravity, and V_T is the terminal velocity of the skydiver.
c. Verify by integration that the position function is given by
s(t) = V_T t + (V_T²/g) ln[(1 + e^(-2gt/V_T))/2],
where s'(t) = v(t) and s(0) = 0.

Guida verificata passo dopo passo
1
Start with the given velocity function: \(v(t) = V_T \left( \frac{1 - e^{-\frac{2gt}{V_T}}}{1 + e^{-\frac{2gt}{V_T}}} \right)\). Since velocity is the derivative of position, we have \(s'(t) = v(t)\), so to find \(s(t)\), integrate \(v(t)\) with respect to \(t\).
Rewrite the velocity function to simplify the integral. Notice that \(\frac{1 - e^{-x}}{1 + e^{-x}} = \tanh\left( \frac{x}{2} \right)\), where \(x = \frac{2gt}{V_T}\). So, \(v(t) = V_T \tanh\left( \frac{gt}{V_T} \right)\). This substitution makes the integral more straightforward.
Set up the integral for position: \(s(t) = \int v(t) \, dt = \int V_T \tanh\left( \frac{gt}{V_T} \right) dt\). Since \(V_T\) is constant, factor it out: \(s(t) = V_T \int \tanh\left( \frac{gt}{V_T} \right) dt\).
Use substitution to integrate: Let \(u = \frac{gt}{V_T}\), so \(du = \frac{g}{V_T} dt\) or \(dt = \frac{V_T}{g} du\). Rewrite the integral: \(s(t) = V_T \int \tanh(u) \cdot \frac{V_T}{g} du = \frac{V_T^2}{g} \int \tanh(u) du\).
Recall the integral of hyperbolic tangent: \(\int \tanh(u) du = \ln(\cosh(u)) + C\). Therefore, \(s(t) = \frac{V_T^2}{g} \ln(\cosh(u)) + C = \frac{V_T^2}{g} \ln\left( \cosh\left( \frac{gt}{V_T} \right) \right) + C\). Use the initial condition \(s(0) = 0\) to solve for \(C\) and express \(\cosh\) in terms of exponentials to match the given formula.

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Relationship Between Velocity and Position via Integration

Velocity is the derivative of position with respect to time. To find the position function s(t) from a given velocity v(t), you integrate v(t) with respect to time. The constant of integration is determined using initial conditions, such as s(0) = 0 in this problem.
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Integration of Exponential Functions

The velocity function involves exponential terms of the form e^(-2gt/V_T). Integrating such functions requires understanding how to handle exponentials and logarithms, often using substitution methods to simplify the integral into a form involving natural logarithms.
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Initial Conditions and Determining Constants of Integration

When integrating to find position, an arbitrary constant appears. Applying the initial condition s(0) = 0 allows you to solve for this constant, ensuring the position function accurately reflects the physical scenario starting at zero displacement.
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Initial Value Problems Example 1