Understanding the Terminal Velocity Equation with Solved Examples

Understanding the Terminal Velocity Equation with Solved Examples

When objects fall through air or water, why do they stop accelerating and move at a constant speed? This constant speed, known as terminal velocity, is a concept many of you might struggle to fully grasp. Balancing forces like gravity and drag can seem complex, but understanding the terminal velocity equation provides clarity. In fact, real-world applications of this principle span skydiving, engineering, and even particle dynamics, making it an essential topic for students and professionals alike.

Did you know that a skydiver in free fall typically reaches a terminal velocity of 195 km/h in a belly-down position? This highlights the practical significance of mastering this equation. You’ll see how this knowledge applies to everyday scenarios and complex systems by breaking down the components and solving examples. Let us dive into the blog and explore solutions for better understanding.

Breaking Down the Terminal Velocity Equation

Terminal velocity results from the balance between gravitational and drag forces acting on an object in motion. Here's a step-by-step derivation of the equation that defines this equilibrium.

Gravitational Force (mg): This is the weight of the object, where m is mass and g is acceleration due to gravity.

Drag Force (FD): This is the fluid’s resistance, represented by FD = 1/2 ρ C A v^2, where:- ρ: Density of the fluid- C: Drag coefficient (depends on the object's shape)- A: Cross-sectional area- v: Velocity

At terminal velocity, gravitational force equals drag force:mg = (1/2) ρ C A v_T^2

Rearranging this, the terminal velocity equation becomes:v_T = √(2mg / ρ C A)

Now that you understand the basics of the terminal velocity equation, let’s explore the factors that influence it.

Factors Influencing Terminal Velocity

Understanding terminal velocity requires analyzing the factors that determine its value. These include:

1. Object Shape and Size

Streamlined shapes, such as aerodynamic designs, reduce the resistance caused by drag, allowing objects to achieve higher terminal velocities. This principle is used in designing aircraft, bullets, and high-speed vehicles.

Larger surface areas create more contact with the fluid, leading to increased drag force and slower terminal speeds. For instance, a flat sheet of paper falls slower than a crumpled ball of paper due to its larger surface area facing the fluid.

Example: Skydivers adjust their body position to control their descent speed. By spreading their arms and legs, they increase their surface area, creating more drag and slowing down. Conversely, tucking in their limbs reduces surface area and drag, allowing them to accelerate.

2. Fluid Density and Viscosity

The density of the fluid through which an object moves significantly impacts terminal velocity. Heavier fluids like water create more resistance compared to lighter fluids like air, leading to reduced terminal speeds. This is why objects fall slower in water than in air.

Viscosity, or the "thickness" of a fluid, also plays a critical role. High-viscosity fluids, such as honey or oil, produce greater resistance to motion, causing objects to fall more slowly.

Temperature changes can further influence viscosity. For example, warmer fluids tend to be less viscous, reducing drag and allowing objects to move faster through them. This is observable in liquids like syrup, which flows more freely when heated.

Example: Divers in deep-sea environments experience reduced terminal speeds due to the high density and viscosity of water compared to air.

3. Drag Coefficient

The drag coefficient is a measure of how easily an object moves through a fluid. It depends on factors such as the object's shape, surface texture, and orientation.

Smoother objects, like a polished sphere or a streamlined car, have lower drag coefficients, enabling them to achieve higher terminal velocities. Conversely, rough or irregularly shaped objects, like a crumpled ball or parachute, experience greater drag, reducing their terminal speed.

Example: The sleek design of sports cars minimizes drag, allowing for higher speeds. Parachutes, on the other hand, are designed with large surface areas and high drag coefficients to slow down a person's descent safely.

These factors set the stage for real-world applications of the terminal velocity equation. Let’s explore how it’s used.

Applications of Terminal Velocity

Whether optimizing athletic performance or adjusting freefall speed, understanding terminal velocity has practical applications in real-world scenarios. Let us understand how terminal velocity influences both sports and skydiving.

1. Sports and Engineering

Terminal velocity is a crucial factor in sports and engineering, especially in activities where speed and resistance play significant roles.

  • Athletics: In sports like cycling and skiing, athletes aim to reduce drag by adopting aerodynamic postures or wearing streamlined suits. This helps them achieve higher speeds by lowering air resistance. Cyclists often hunch forward, while skiers wear tightly fitted suits and helmets to cut through the air efficiently.

  • Vehicle Design: Engineers use terminal velocity principles to create vehicles with streamlined shapes that minimize drag. For instance, high-performance sports cars and race cars are designed with low drag coefficients to maximize speed and fuel efficiency. Wind tunnels are frequently employed to test and refine these designs.

2. Skydiving

Skydiving is one of the most iconic applications of terminal velocity. As skydivers fall, they experience an increase in speed until the drag force equals their weight, achieving terminal velocity.

  • Adjusting Speed: Skydivers can control their descent rate by changing body positions. A belly-down pose, which increases surface area and drag, results in a terminal velocity of approximately 195 km/h. On the other hand, a head-down pose reduces drag, allowing speeds of up to 320 km/h. These adjustments are critical for maneuvering in the air or coordinating with other divers.

  • Safety Measures: Parachutes drastically increase drag, reducing terminal velocity to about 15-20 km/h, ensuring a safe landing. The understanding of terminal velocity is vital in designing parachutes for both recreational and emergency purposes.

Flashcards on the ZuAI platform make memorizing such real-world terminal velocity examples effortless, helping you connect theory to practice. Next, let’s dive into worked examples to solidify your understanding of terminal velocity calculations.

Solved Examples of Terminal Velocity Calculations

From skydivers to small particles like pollen grains, these examples highlight the application of key formulas in different contexts.

Here’s a real-world calculation of terminal velocity for a skydiver based on key factors like mass, air density, and drag coefficient. 

Example 1: Terminal Velocity of a Skydiver

Calculate the terminal velocity of a 70 kg skydiver in free fall, given:

- Fluid density (ρ) = 1.2 kg/m³- Drag coefficient (C) = 1.0- Cross-sectional area (A) = 0.7 m²

Solution: 

Using the formula:v_T = √(2mg / ρ C A)

Substitute the values:v_T = √(2(70)(9.8) / (1.2)(1.0)(0.7))v_T ≈ 53.4 m/s

Example 2: Terminal Velocity of a Falling Raindrop

A raindrop has a mass of 0.002 kg and a cross-sectional area of 0.0005 m². Calculate its terminal velocity assuming:- Fluid density (ρ) = 1.2 kg/m³- Drag coefficient (C): 0.5

Solution:

Using the formula:v_T = √(2mg / ρ C A)

Substitute the values:v_T = √2(0.002)(9.8) / (1.2)(0.5)(0.0005)

v_T ≈ 11.5m/s

But what happens when objects are smaller? Let’s discuss Stokes' Law and its role in terminal velocity.

Stokes' Law

Stokes' Law governs terminal velocity for small, spherical objects moving in low-speed conditions. The equation is expressed as:

vT = (2r²(ρp - ρf)g) / (9η)

Here:- r = radius of the particle- ρp = particle density- ρf = fluid density- η = fluid viscosity- g = acceleration due to gravity

Stokes’ Law finds applications in understanding sedimentation, aerosol dynamics, and even biological processes like the movement of microorganisms. It highlights how smaller objects experience different forces compared to larger ones, with viscosity playing a dominant role. With mock exams on ZuAI, you can practice solving terminal velocity problems for both large and small objects, ensuring complete readiness for IB exams.

Smaller objects, like a pollen grain, experience terminal velocity differently. Using Stokes' Law, we can calculate the drag force acting on tiny particles in the air.

Example 1: Small Steel Ball Falling Through Glycerin

A small steel ball of radius 0.1 cm falls through glycerin with a terminal velocity of 4 cm/s. Calculate the viscosity of glycerin. Given:

- Radius of ball, r = 0.1 cm = 0.001 m- Terminal velocity, v = 4 cm/s = 0.04 m/s- Acceleration due to gravity, g = 9.8 m/s²- Density of steel, ρs = 7800 kg/m³- Density of glycerin, ρg = 1260 kg/m³

Solution:

Using the formula:

vT = (2r²(ρp - ρf)g) / (9η)

Substitute the values:

vT = 2(0.001)2(7800−1260)(9.8) / 9(0.04)

vT ≈ 0.355 Pa·s.

Finally, let’s touch upon advanced concepts for those eager to delve deeper.

Advanced Concepts in Terminal Velocity

For higher accuracy, advanced terminal velocity calculations often require the application of calculus. This approach considers velocity-dependent frictional forces, leading to differential equations that describe speed over time. 

Such equations help in modeling motion in resistive environments, like an object falling through thick oil or atmospheric layers. The differential equation governing such motion can be written as:

m(dv/dt) = mg - kv

Here:- m = mass of the object- dv/dt = acceleration- g = acceleration due to gravity- k = proportionality constant related to drag force

You can derive velocity as a function of time, enabling a deeper understanding of dynamic systems by solving this equation. Fields like astrophysics, aerodynamics, and fluid mechanics frequently employ these calculations.

Also read: How to Ace Your IB Mathematics IA: A Complete Guide for N24 and M25 Students

Conclusion

The terminal velocity equation, v_T = √(2mg / ρ C A), unravels the delicate balance between gravity and drag that governs motion through fluids. From understanding the aerodynamics of skydiving to studying the behavior of tiny particles in dense media, this equation finds applications across diverse fields like engineering, sports, and environmental science. Its relevance extends far beyond academics, making it an essential concept for problem-solving in the real world.

ZuAI empowers you to go beyond just understanding—allowing you to master terminal velocity and related concepts with innovative learning tools. With AI-powered support, customizable mock exams, and interactive flashcards, ZuAI turns complex theories into manageable and engaging challenges. Why settle for average when you can excel? Take your IB Physics and Mathematics preparation to the next level with ZuAI. Try ZuAI today and see the difference in your learning journey!

FAQs

Q1: Can terminal velocity vary for the same object?Yes, terminal velocity depends on factors like fluid density, object orientation, and surface texture. Changing any of these factors can alter the terminal velocity.

Q2: Is terminal velocity the same for all objects?No, terminal velocity varies depending on an object's mass, shape, cross-sectional area, and the density of the fluid it is moving through.

Q3: What is the terminal velocity of a skydiver?The terminal velocity of a skydiver in a belly-down position is approximately 195 km/h, while a head-down position can increase it to around 320 km/h.

Q4: Why is terminal velocity important in engineering?Terminal velocity helps engineers design aerodynamic vehicles, optimize sports equipment, and create safer structures that reduce drag and improve efficiency.

Q5: How is terminal velocity calculated for small particles?For small objects like droplets or dust particles, Stokes' Law is used to calculate terminal velocity, which accounts for viscous forces dominating over inertial forces.