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(a) Estimate the terminal speed of a wooden sphere (density \(0.830 \mathrm{g} / \mathrm{cm}^{3}\) ) falling through air if its radius is \(8.00 \mathrm{cm}\) and its drag coefficient is \(0.500 .\) (b) From what height would a freely falling object reach this speed in the absence of air resistance?

Short Answer

Expert verified
Firstly, the terminal speed of the wooden sphere falling through air is calculated. Secondly, the distance the wooden sphere would fall freely (without air resistance) to achieve this terminal speed is calculated.

Step by step solution

01

Calculate the Terminal Speed

First, calculate the mass of the wooden sphere using the formula \(m = \rho V\), where \(\rho\) is the density and \(V\) is the volume. The volume of a sphere is calculated with \(V = \frac{4}{3} \pi r^3\). Now, plug in the density and the volume of the sphere to find the mass (m). Next, substitute the mass (m), gravitational constant (g), air density (\(\rho\)), cross-sectional area (A) and drag coefficient (C_d) into the terminal speed equation: \(v_t = \sqrt{{2mg}/{\rho AC_d}}\). We can now calculate the terminal speed.
02

Calculate the Distance

To find the distance that the wooden sphere would have to fall freely in the absence of air resistance to reach its terminal speed, we use the kinematic equation \(v^2 = u^2 + 2gs\) where u is the initial speed (0), v is the final speed (terminal speed), g is the gravitational acceleration, and s is the distance. Solving for s gives us \(s = {v^2}/{2g}\). Inputting the terminal speed and the gravitational constant into this equation will give us the required distance.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Drag Coefficient
The drag coefficient, denoted as \( C_d \), is a dimensionless number that quantifies the resistance of an object as it moves through a fluid, such as air or water. This value plays a crucial role in determining the terminal velocity of an object. Terminal velocity is the steady speed achieved by an object freely falling through a fluid when the force due to gravity is balanced by the drag force acting opposite to the motion.

Understanding \( C_d \) is crucial because it's influenced by several factors:
  • Shape of the Object: Sleek, aerodynamic shapes have lower drag coefficients, which means they experience less air resistance.
  • Surface Roughness: A rougher surface can increase the drag coefficient by affecting the flow of air around the object.
  • Flow Conditions: The speed and viscosity of the fluid also impact the drag coefficient.
To calculate the drag force, the formula is \( F_d = \frac{1}{2} \rho v^2 A C_d \), where \( \rho \) is the fluid density, \( v \) is the speed of the object, and \( A \) is the cross-sectional area. The purpose of understanding the drag coefficient is to accurately determine how much force will slow down the object, thus calculating its terminal velocity with precision.
Gravitational Acceleration
Gravitational acceleration, represented by \( g \), is the rate at which an object accelerates due to the force of gravity near the surface of the Earth. This rate is approximately \( 9.81 \text{ m/s}^2 \). It is crucial for determining how fast an object can potentially fall when other factors like air resistance aren't considered.

When an object is in freefall, the gravitational force acting on it is \( F_g = mg \), where \( m \) is the mass of the object. This force is responsible for the initial acceleration of objects towards the Earth.

In the context of the problem involving terminal velocity, once the drag force equals the gravitational force, an object reaches terminal velocity and ceases to accelerate. Hence, understanding gravitational acceleration helps in calculating the point at which drag force balances with gravitational force, indicating terminal velocity's achievement.
  • Importance in Kinematics: Widely used in kinematic equations to solve problems of motion.
  • Constant Rate: Near Earth's surface, \( g \) is considered a constant to simplify calculations.
Kinematic Equations
Kinematic equations describe the motion of objects without considering the causes (forces) of this motion, focusing instead on the position, velocity, and acceleration of the objects over time. These equations are essential for predicting the future position or velocity of an object if its initial conditions are known.

In the case of the given exercise, we used one specific kinematic equation:
  • \( v^2 = u^2 + 2gs \): This formula allows us to calculate the distance \( s \) an object travels when starting from rest (\( u = 0 \)), assuming only gravitational acceleration acts upon it.
The equation helps find the height from which an object needs to be dropped to reach a certain speed, in this case, the terminal speed, without any air resistance. Here, \( v \) is the final speed (or terminal velocity), \( g \) is gravitational acceleration, and \( s \) is the distance traveled.

Kinematic equations are powerful tools in physics and engineering because they simplify complex motion problems by allowing us to calculate unknown variables if certain parameters of motion are already known. They help break down the motion into simpler parts like displacement, initial velocity, time, and acceleration, aiding in the comprehensive understanding of the motion dynamics.

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Most popular questions from this chapter

A person stands on a scale in an elevator. As the elevator starts, the scale has a constant reading of \(591 \mathrm{N}\). As the elevator later stops, the scale reading is \(391 \mathrm{N}\). Assume the magnitude of the acceleration is the same during starting and stopping, and determine (a) the weight of the person, (b) the person's mass, and (c) the acceleration of the elevator.

Whenever two Apollo astronauts were on the surface of the Moon, a third astronaut orbited the Moon. Assume the orbit to be circular and \(100 \mathrm{km}\) above the surface of the Moon, where the acceleration due to gravity is \(1.52 \mathrm{m} / \mathrm{s}^{2}\) The radius of the Moon is \(1.70 \times 10^{6} \mathrm{m} .\) Determine (a) the astronaut's orbital speed, and (b) the period of the orbit.

The Earth rotates about its axis with a period of \(24.0 \mathrm{h}\) Imagine that the rotational speed can be increased. If an object at the equator is to have zero apparent weight, (a) what must the new period be? (b) By what factor would the speed of the object be increased when the planet is rotating at the higher speed? Note that the apparent weight of the object becomes zero when the normal force exerted on it is zero.

A motorboat cuts its engine when its speed is \(10.0 \mathrm{m} / \mathrm{s}\) and coasts to rest. The equation describing the motion of the motorboat during this period is \(v=v_{i} e^{-c t}\) where \(v\) is the speed at time \(t, v_{i}\) is the initial speed, and \(c\) is a constant. At \(t=20.0 \mathrm{s}\), the speed is \(5.00 \mathrm{m} / \mathrm{s} .\) (a) Find the constant \(c\) (b) What is the speed at \(t=40.0 \mathrm{s} ?\) (c) Differentiate the expression for \(v(t)\) and thus show that the acceleration of the boat is proportional to the speed at any time.

Consider an object on which the net force is a resistive force proportional to the square of its speed. For example, assume that the resistive force acting on a speed skater is \(f=-k m v^{2},\) where \(k\) is a constant and \(m\) is the skater's mass. The skater crosses the finish line of a straight-line race with speed \(u_{0}\) and then slows down by coasting on his skates. Show that the skater's speed at any time \(t\) after crossing the finish line is \(v(t)=u_{0} /\left(1+k t u_{0}\right) .\) This problem also provides the background for the two following problems.

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