You drop an object of mass m from a tall building. Suppose the only forces affecting its motion are gravity, and air resistance proportional to the object's speed with positive constant of proportionality k. Let g denote gravitational acceleration (a positive constant). Express the total force in terms of m, g, and the object's velocity v, where upward displacement is considered positive. F - Newton's second law tells us that force is equal to mass x acceleration, F = ma. Relating mg - kv acceleration to velocity, rewrite the equation for total force above as a first order differential equation for v as a function of t. Denote v' as dv dt dv dt this is not an equation. m v(t): = Solve this differential equation for v(t) with the initial condition v(0) = V0. mg k 1 e X m Find the terminal velocity. Terminal velocity = mg k X syntax error: X X

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**Understanding Motion with Air Resistance**

When you drop an object of mass \( m \) from a tall building, the primary forces affecting its motion are gravity and air resistance. Air resistance is proportional to the object's speed with a positive constant of proportionality \( k \). Let \( g \) represent gravitational acceleration (a positive constant).

**Expressing Total Force**

To express the total force \( F \) in terms of \( m \), \( g \), and the object's velocity \( v \) (considering upward displacement as positive), the equation is:

\[
F = mg - kv
\]

**Newton’s Second Law**

According to Newton’s second law, force equals mass times acceleration, expressed as \( F = ma \). By relating acceleration to velocity, we can rewrite the total force equation as a first-order differential equation for \( v \) as a function of time \( t \). Denote acceleration \( v' \) as \( \frac{dv}{dt} \).

**Differential Equation**

To solve the differential equation,

\[
m \left(-\frac{dv}{dt}\right) 
\]

results in a syntax error indicating that this is not an equation as presented.

**Solving for Velocity**

Given the initial condition \( v(0) = v_0 \), solving the differential equation gives:

\[
v(t) = \frac{mg}{k} \left(1 - e^{-\frac{k}{m}t}\right)
\]

**Finding Terminal Velocity**

The terminal velocity is determined when the object's speed stops changing:

\[
\text{Terminal velocity} = \frac{mg}{k}
\]

*Note: The boxes above indicate where certain expressions need correction.*
Transcribed Image Text:**Understanding Motion with Air Resistance** When you drop an object of mass \( m \) from a tall building, the primary forces affecting its motion are gravity and air resistance. Air resistance is proportional to the object's speed with a positive constant of proportionality \( k \). Let \( g \) represent gravitational acceleration (a positive constant). **Expressing Total Force** To express the total force \( F \) in terms of \( m \), \( g \), and the object's velocity \( v \) (considering upward displacement as positive), the equation is: \[ F = mg - kv \] **Newton’s Second Law** According to Newton’s second law, force equals mass times acceleration, expressed as \( F = ma \). By relating acceleration to velocity, we can rewrite the total force equation as a first-order differential equation for \( v \) as a function of time \( t \). Denote acceleration \( v' \) as \( \frac{dv}{dt} \). **Differential Equation** To solve the differential equation, \[ m \left(-\frac{dv}{dt}\right) \] results in a syntax error indicating that this is not an equation as presented. **Solving for Velocity** Given the initial condition \( v(0) = v_0 \), solving the differential equation gives: \[ v(t) = \frac{mg}{k} \left(1 - e^{-\frac{k}{m}t}\right) \] **Finding Terminal Velocity** The terminal velocity is determined when the object's speed stops changing: \[ \text{Terminal velocity} = \frac{mg}{k} \] *Note: The boxes above indicate where certain expressions need correction.*
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