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D4.8 - Worked Examples

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Circular Satellite Orbit

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Teacher
Teacher

Today, we are going to explore how we can determine the characteristics of a satellite orbiting Earth. Let's start with the example of a satellite at a given altitude. First, who remembers how we calculate the orbital radius?

Student 1
Student 1

Is it the Earth's radius plus the altitude of the satellite?

Teacher
Teacher

Exactly! The formula is r = R⊕ + h. For our satellite with h = 300 km, and Earth’s radius of about 6,370 km, we get r = 6,670 km. Now, let’s find the orbital speed using the gravitational constant.

Student 2
Student 2

What’s the formula we use for orbital speed?

Teacher
Teacher

Great question! The orbital speed v in a circular orbit is given by v = sqrt(GM/r). Using the values for G and M, we can simplify this to find v. Now, can anyone say what the next step is?

Student 3
Student 3

Do we calculate the orbital period next?

Teacher
Teacher

Exactly! The orbital period T can be calculated using T = 2π√(r³/GM). Let’s take a moment to calculate that. Remember, G is the gravitational constant and M is the mass of Earth.

Student 4
Student 4

And the total mechanical energy in orbit would be important too!

Teacher
Teacher

Yes! The total mechanical energy E can be found by combining kinetic and potential energy: E = K + U. Remember to account for the negative energy indicating a bound state. Let’s summarize what we've learned today.

Electric Field of Two Point Charges

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Teacher
Teacher

Now, let’s explore the electric field produced by two point charges. How do we calculate the electric field at a point due to these charges?

Student 1
Student 1

I think we need to calculate the fields due to each charge separately and then add them.

Teacher
Teacher

Right! That’s the superposition principle. If we have q1 at x=0 and q2 at x=0.5 m, what is the distance to point P located at x=0.25 m?

Student 2
Student 2

Both q1 and q2 are 0.25 m away from P.

Teacher
Teacher

Exactly! Now, how do we find the electric field from q1 at P?

Student 3
Student 3

We can use E = k|q|/r², where k is Coulomb's constant!

Teacher
Teacher

Perfect! And since q1 is positive, the electric field will point away from it. What about for q2, which is negative?

Student 4
Student 4

The electric field points towards q2!

Teacher
Teacher

Correct! Then we add both fields to find the total electric field at point P. Let's summarize our discussion today.

Magnetic Field Around a Long Straight Current

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Teacher
Teacher

Next, let's discuss the magnetic field generated by a long straight wire. Can anyone tell me the formula to calculate the magnetic field around a wire?

Student 1
Student 1

It's B = (μ₀I)/(2πr)!

Teacher
Teacher

Exactly! μ₀ is the permeability of free space, and r is the distance from the wire. If we have a current of 5 A and a distance of 0.1 m, what is the magnetic field?

Student 2
Student 2

Let’s calculate B = (4π × 10⁻⁷ N⋅m²/A² × 5 A)/(2π × 0.1 m).

Teacher
Teacher

That’s the right approach! Don’t forget the units will give you the correct field strength in Tesla. What’s next in terms of direction?

Student 3
Student 3

We can use the right-hand rule to determine the direction!

Teacher
Teacher

Correct! Placing your thumb in the direction of the current will show you how the magnetic field wraps around. Let’s recap today's key points.

Particle in a Velocity Selector

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Teacher
Teacher

Finally, let’s delve into understanding how a proton moves through an electric and magnetic field in a velocity selector. Remember the equation qE = qvB?

Student 1
Student 1

Yes! This equation tells us the speed at which the proton should travel to be undeflected.

Teacher
Teacher

Exactly! What do you get when you rearrange the equation to find the velocity?

Student 2
Student 2

v = E/B!

Teacher
Teacher

Right again! Now, think about what happens when that proton enters a magnetic field only. How do we find the radius of its trajectory?

Student 3
Student 3

We can use the formula r = mv/qB!

Teacher
Teacher

Exactly! So as we solve for radius, we can also illustrate how varying the speed or magnetic field affects the path of the proton. Let’s summarize all our insights.

Introduction & Overview

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Quick Overview

This section presents worked examples that illustrate key concepts related to fields in physics, particularly in gravitational and electromagnetic contexts.

Standard

The section offers several worked examples that highlight important principles in gravitational fields and motion in electromagnetic fields. Each example is broken down step-by-step to enhance understanding and application of the underlying theories.

Detailed

Worked Examples

This section provides a series of worked examples designed to apply and illustrate key physical principles regarding fields in both gravitational and electromagnetic contexts. Each example is structured to show the problem-solving process, demonstrating how to apply theoretical concepts and formulas to real-world scenarios.

  1. Circular Satellite Orbit
  2. Example D1.1 involves a satellite orbiting Earth, demonstrating calculations for orbital radius, speed, period, and total mechanical energy. It illustrates the application of gravitational equations and the practical relevance of Newton's laws in orbital mechanics.
  3. Electric Field of Two Point Charges
  4. Example D2.1 covers the concept of electric fields generated by two point charges, guiding through the computation of the resultant electric field at a specific point. It emphasizes the principles of superposition and vector addition in electric fields.
  5. Magnetic Field Around a Long Straight Current
  6. Example D2.2 explores the magnetic field produced by a straight wire carrying current. The example demonstrates the use of formulas related to magnetic fields and the application of the right-hand rule for directionality.
  7. Particle in a Velocity Selector
  8. Example D3.1 details how a proton behaves in a perpendicular electric and magnetic field. It illustrates the calculations necessary to determine speed and the radius of the particle's circular path as it interacts with the magnetic field.

The detailed step-by-step presentation of these examples is critical for students as they learn to connect theoretical concepts with practical applications.

Audio Book

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Example D1.1 (Circular Satellite Orbit)

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A satellite of mass m=500 kg orbits Earth in a circular orbit at altitude h=300 km above Earth’s surface. Given Earth’s mass M⊕=5.97×10^24 kg and radius R⊕=6.37×10^6 m, find:
1. The orbital radius r.
2. The orbital speed v.
3. The orbital period T.
4. The total mechanical energy of the satellite in orbit.

Detailed Explanation

In this example, we analyze the motion of a satellite around Earth. First, we calculate the orbital radius (r) by adding Earth's radius (R⊕) to the altitude (h) of the satellite. This gives us r = R⊕ + h = 6.37×10^6 m + 3.00×10^5 m = 6.67×10^6 m.

Next, to find the orbital speed (v), we use the formula v = √(G M⊕ / r). We calculate the gravitational constant multiplied by Earth's mass to find G M⊕ ≈ 3.986×10^14 m³/s², then substitute to find v = √(3.986×10^14 m³/s² / 6.67×10^6 m) ≈ 7.73 km/s.

For the orbital period (T), we use the formula T = 2π√(r³ / (G M⊕)). We obtain r³ = (6.67×10^6 m)³ = 2.97×10^20 m³. Substituting this into the formula gives T ≈ 1.51 hours after calculations.

Finally, the total mechanical energy (E) is calculated using E = −(G M⊕ m) / (2 r), resulting in E ≈ −1.495×10^10 J, indicating that the satellite is in a bound state.

Examples & Analogies

Imagine you are launching a ball into the air; the higher you throw it, the faster you need to throw to keep it in orbit instead of falling back to the ground. Similarly, a satellite needs to reach a specific speed and altitude to stay in a stable orbit around the Earth.

Solution Steps for Orbital Radius

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  1. Orbital radius:
    r=R⊕+h=6.37×10^6 m + 3.00×10^5 m = 6.67×10^6 m.

Detailed Explanation

In this step, we determine the orbital radius by simply adding the altitude of the satellite (h) to the radius of Earth (R⊕). Since the satellite orbits above the surface of the Earth, its orbital radius is effectively the sum of the two distances. Thus, r = R⊕ + h gives us the total distance from the center of the Earth to the satellite.

Examples & Analogies

Think of it like measuring your total height from the ground up to the top of your head. If you are on a hill (height h), your total height from sea level (the center of the Earth) would be your height plus the height of the hill.

Solution Steps for Orbital Speed

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  1. Orbital speed:
    v=G M⊕/r=(6.674×10^−11)(5.97×10^24)/6.67×10^6.
    Compute numerator: GM⊕=3.986×10^14 m³/s².
    v=3.986×10^14/6.67×10^6≈7.73 km/s.

Detailed Explanation

To find the speed at which the satellite orbits, we apply the formula for orbital speed v, which is derived from Newton's law of universal gravitation. Here, we rearrange this law to solve for v. First, we compute the product of the gravitational constant G and the mass of Earth M⊕ to find GM⊕. Next, we input the calculated GM⊕ alongside the previously computed orbital radius (r) into the orbital speed formula, leading us to deduce the satellite's speed as approximately 7.73 km/s.

Examples & Analogies

Imagine driving a car around a racetrack; to maintain a stable position on the curve, you must travel at a specific speed that keeps you from sliding out. Similarly, the satellite must travel at a precise speed to maintain its path around Earth.

Solution Steps for Orbital Period

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  1. Orbital period:
    T=2 πr³G M⊕=2 π(6.67×10^6)³/3.986×10^14.
    Compute r³=(6.67×10^6)³=2.97×10^20 m³.
    Thus T≈1.51 hours.

Detailed Explanation

The orbital period T represents the time it takes for the satellite to make one complete revolution around Earth. We calculate T using Kepler's third law for circular orbits. We compute the cube of the orbital radius (r³) first, then substitute this along with GM⊕ into the formula for T. After doing the calculations, we find that T works out to about 1.51 hours, which gives us an idea of how long the satellite takes to circle Earth completely.

Examples & Analogies

It's like timing how long it takes for a train to make a full loop around a circular track. If you know the speed of the train and the distance, you can figure out how long the journey will take.

Solution Steps for Total Mechanical Energy

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  1. Total mechanical energy:
    E=−G M⊕ m/2 r=−(3.986×10^14)(500)/2×6.67×10^6.
    E=−1.495×10^10 J.

Detailed Explanation

To calculate the total mechanical energy (E) in orbit, we utilize the energy equation that combines potential energy and kinetic energy. The negative sign indicates that this amount of energy is for a bound system, which means the satellite is gravitationally held in orbit around Earth. We substitute the known values for GM⊕, the mass of the satellite, and its orbital radius into the equation to compute E and determine it as approximately -1.495×10^{10} J.

Examples & Analogies

Think of total mechanical energy like the energy needed to keep a ball swinging back and forth on a string. The energy consists of the potential energy when it's at the top and the kinetic energy at the bottom. The total energy is continuously exchanged as the ball swings.

Definitions & Key Concepts

Learn essential terms and foundational ideas that form the basis of the topic.

Key Concepts

  • Gravitational Field Strength: The force per unit mass experienced by a mass in a gravitational field.

  • Electric Field: A region around electric charges in which other charges experience forces.

  • Magnetic Field: A vector field around magnetic materials and electric currents within which magnetic force acts.

  • Orbital Mechanics: The study of the motions of objects in space under the influence of gravitational forces.

  • Superposition Principle: A principle that states that the total field at a point is the vector sum of the fields due to each charge.

Examples & Real-Life Applications

See how the concepts apply in real-world scenarios to understand their practical implications.

Examples

  • Determining the orbital characteristics of a satellite given specific masses and distances.

  • Finding the resultant electric field from multiple point charges.

  • Calculating the magnetic field produced by a straight current-carrying wire.

  • Analyzing particle motion in perpendicular electric and magnetic fields.

Memory Aids

Use mnemonics, acronyms, or visual cues to help remember key information more easily.

🎵 Rhymes Time

  • If you want to find the core, let G and M show you more!

📖 Fascinating Stories

  • Once upon a time, a satellite soared far above Earth, calculating its speed and energy through the laws of gravity and motion.

🧠 Other Memory Gems

  • Use 'FEM' to remember: Force, Electric, Magnetic when studying fields.

🎯 Super Acronyms

GEM

  • Gravitational
  • Electric
  • Magnetic fields are essential in physics.

Flash Cards

Review key concepts with flashcards.

Glossary of Terms

Review the Definitions for terms.

  • Term: Gravitational Field

    Definition:

    A region of space around a mass where other masses feel a force.

  • Term: Electric Field

    Definition:

    A region around electric charges where other charges experience a force.

  • Term: Magnetic Field

    Definition:

    A field around a magnet or a current-carrying wire where magnetic forces are exerted.

  • Term: Orbital Speed

    Definition:

    The speed required for an object to remain in orbit around a celestial body.

  • Term: Coulomb's Law

    Definition:

    A law describing the force between two charged objects.

  • Term: Lorentz Force

    Definition:

    The force experienced by a charged particle in an electric and magnetic field.