FISIKA Kelas 12 - Gaya Magnetik | GIA Academy

GIA Academy
12 Oct 202315:30

Summary

TLDRThis YouTube video from Gia Akademi explores the concept of magnetic force, also known as the Lorentz force. Discovered by Dutch physicist Hendrik Antoon Lorentz, it's the force exerted by a magnetic field on an electric current. The video explains how to determine the direction of the Lorentz force using the right-hand rule and discusses its applications in various scenarios, including a current-carrying wire in a magnetic field, a charged particle moving in a magnetic field, and parallel wires carrying current. It also covers the calculations for the force's magnitude and direction, providing examples and solving problems to deepen understanding.

Takeaways

  • 🔊 The script introduces the concept of magnetic force, also known as Lorentz force, which is generated by a magnetic field on an electric current.
  • 🧲 Lorentz force is named after the Dutch physicist Hendrik Antoon Lorentz, who defined it as the force exerted by a magnetic field on an electric current.
  • ✋ The direction of the Lorentz force can be determined using the right-hand rule, where the thumb indicates the direction of the electric current, the index finger shows the direction of the magnetic field, and the middle finger points in the direction of the force.
  • 💡 The Lorentz force can be generated by a current-carrying wire in a magnetic field, a charged particle moving in a magnetic field, or a current-carrying wire parallel to another current-carrying wire.
  • 📐 The formula for Lorentz force on a current-carrying wire in a magnetic field is \( F = B \cdot I \cdot L \cdot \sin(\theta) \), where \( F \) is the force, \( B \) is the magnetic field, \( I \) is the current, \( L \) is the length of the wire, and \( \theta \) is the angle between the field and the current.
  • 🚫 If the magnetic field is parallel to the electric current, the Lorentz force is zero, indicating no force is exerted on the wire.
  • 🌀 For a charged particle moving in a magnetic field, the Lorentz force can cause the particle to move in a circular path, with the force providing the centripetal force necessary for this motion.
  • 🔗 The magnitude of the Lorentz force between two parallel current-carrying wires depends on the direction of the currents; parallel currents attract each other, while anti-parallel currents repel.
  • 📚 The script provides several examples and problems to illustrate the calculation of Lorentz force in different scenarios, helping viewers to understand and apply the concept.
  • 🎓 The video concludes with a summary and an invitation to watch more videos on the channel, emphasizing continuous learning and engagement.

Q & A

  • What is the Lorentz force?

    -The Lorentz force, also known as the magnetic Lorentz force, is the combination of electric and magnetic force on a charged particle moving through a magnetic field. It is given by the equation F = q(E + v × B), where q is the charge, E is the electric field, v is the velocity of the particle, and B is the magnetic field.

  • Who discovered the Lorentz force?

    -The Lorentz force was discovered by the Dutch physicist Hendrik Antoon Lorentz.

  • How can you determine the direction of the Lorentz force using the right-hand rule?

    -Using the right-hand rule, if you point your thumb in the direction of the electric current (I), your index finger in the direction of the magnetic field (B), then your middle finger will point in the direction of the Lorentz force (F).

  • What is the formula for calculating the Lorentz force on a current-carrying wire in a magnetic field?

    -The formula for calculating the Lorentz force (F) on a current-carrying wire of length (l) in a magnetic field (B) with current (I) is F = B * I * l * sin(θ), where θ is the angle between the direction of the current and the magnetic field.

  • What happens when a charged particle moves through a uniform magnetic field?

    -When a charged particle with charge (Q) moves with velocity (V) through a uniform magnetic field (B), it experiences a Lorentz force that is perpendicular to both the velocity and the magnetic field, causing the particle to move in a circular path.

  • What is the relationship between the radius of the path of a charged particle in a magnetic field and the Lorentz force?

    -The radius (r) of the path of a charged particle in a magnetic field is related to the Lorentz force by the equation r = m * v / (q * B), where m is the mass of the particle, v is its velocity, q is its charge, and B is the magnetic field strength.

  • How can you calculate the force between two parallel current-carrying wires in a magnetic field?

    -The force (F) between two parallel current-carrying wires carrying currents I1 and I2, separated by a distance a in a magnetic field, can be calculated using the formula F = (μ0 * I1 * I2 * l) / (2π * a), where μ0 is the permeability of free space.

  • What is the significance of the angle between the direction of the current and the magnetic field in the Lorentz force?

    -The angle between the direction of the current (I) and the magnetic field (B) is significant because the Lorentz force is maximized when this angle is 90 degrees (sin(90) = 1) and is zero when the current and magnetic field are parallel (sin(0) = 0).

  • How does the sign of the charge affect the direction of the Lorentz force?

    -The sign of the charge affects the direction of the Lorentz force. For a positive charge, the force is in the direction of the cross product of the velocity and magnetic field, while for a negative charge, the force is in the opposite direction.

  • What is the formula for calculating the magnetic field strength if the Lorentz force, charge, velocity, and angle are known?

    -If the Lorentz force (F), charge (Q), velocity (V), and angle (θ) are known, the magnetic field strength (B) can be calculated using the formula B = F / (Q * V * sin(θ)).

Outlines

00:00

🔊 Understanding Magnetic Force

This paragraph introduces the concept of magnetic force, specifically Lorentz force, which is generated by a magnetic field on an electric current. It explains that the force can be determined using the right-hand rule, with the thumb indicating the direction of the electric current, the index finger showing the direction of the magnetic field induction, and the middle finger pointing towards the force direction. The paragraph also discusses the Lorentz force on a current-carrying wire in a magnetic field, the force on a moving charge in a magnetic field, and the dependence of the Lorentz force on the type of charge, whether positive or negative.

05:01

🧲 Calculating Lorentz Force in Magnetic Fields

This segment delves into the mathematical calculations of the Lorentz force on a current-carrying wire within a magnetic field. It provides formulas for determining the force when the wire is parallel or perpendicular to the magnetic field and introduces the concept of the force on a moving charge within a homogeneous magnetic field. The description includes the use of the right-hand rule to determine the direction of the force and the implications of the force on the trajectory of charged particles, such as electrons, within a magnetic field.

10:04

🔗 Analyzing Lorentz Force on Parallel Currents

This paragraph discusses the Lorentz force between two parallel wires carrying electric current. It explains how the force can be attractive or repulsive depending on the direction of the currents and provides a formula for calculating the force between the wires. The explanation includes the concept of permeability of free space and its role in the force calculation. The paragraph also presents a problem-solving approach to determine the direction and magnitude of the Lorentz force in given scenarios.

15:10

🎥 Summary and Conclusion on Magnetic Forces

The final paragraph serves as a conclusion to the discussion on magnetic forces. It summarizes the key points covered in the video and encourages viewers to continue watching for more educational content. The paragraph ends with a call to action for viewers to stay engaged with the channel for upcoming videos.

Mindmap

Keywords

💡Speaker

A speaker is a device that converts electrical energy into sound energy. In the context of the video, speakers are used to introduce the concept of electromagnetic force, which is central to the theme of the video. The script mentions speakers in the opening lines to set the stage for discussing the transformation of energy forms, specifically from electrical to sound.

💡Electromagnetic Force

Electromagnetic force, also known as the Lorentz force, is a fundamental interaction in nature that arises from electric and magnetic fields. The video script delves into this concept, explaining how it is responsible for the operation of speakers and other devices. It is a key theme of the video, as it ties into the broader discussion of how forces are generated and interact within electromagnetic fields.

💡Lorentz Force

The Lorentz force is the combination of electric and magnetic force on a charged particle. It is named after the Dutch physicist Hendrik Lorentz and is defined as the force on a charged particle moving through an electric and magnetic field. The video script uses this term to explain the mathematical formula and the physical principles behind the force experienced by charged particles in magnetic fields.

💡Right-Hand Rule

The right-hand rule is a mnemonic for understanding the direction of the Lorentz force. By aligning the fingers of the right hand, one can determine the direction of the force based on the direction of the current and the magnetic field. The video script mentions this rule as a method to visualize and calculate the direction of the Lorentz force, which is crucial for understanding the behavior of particles in magnetic fields.

💡Magnetic Field

A magnetic field is a vector field that describes the magnetic influence on moving electric charges, electric currents, and magnetic materials. The video script discusses the magnetic field in relation to the Lorentz force, explaining how the presence of a magnetic field affects the motion of charged particles and the generation of force.

💡Electric Current

Electric current is the flow of electric charge, often through a conductor such as a wire. In the video, the concept of electric current is integral to understanding how speakers and other devices operate, as well as how the Lorentz force is generated when a current-carrying wire is placed in a magnetic field.

💡Charged Particle

A charged particle is any particle that carries an electric charge, either positive or negative. The video script discusses how charged particles moving in a magnetic field experience the Lorentz force, which can cause them to move in circular paths. This concept is essential for understanding the behavior of particles in various electromagnetic contexts.

💡Magnetic Induction

Magnetic induction refers to the production of an electromotive force across a conductor when it is exposed to a changing magnetic field. While not explicitly mentioned in the script, the concept is related to the discussion of magnetic fields and their interaction with electric currents, which is a central theme of the video.

💡Tesla

Tesla is the unit of measurement for magnetic induction or magnetic flux density. The script uses this term to quantify the strength of the magnetic field in the examples provided, which is crucial for calculating the Lorentz force and understanding the effects of magnetic fields on charged particles.

💡Ampere

The ampere is the base unit of electric current in the International System of Units (SI). The video script mentions amperes when discussing the strength of the electric current flowing through a wire, which is a factor in determining the magnitude of the Lorentz force experienced by the wire in a magnetic field.

💡Permeability

Permeability is a measure of how easily a material can support the formation of a magnetic field. The script refers to the permeability of free space (μ0) when discussing the forces between parallel current-carrying wires in a magnetic field, which is important for understanding the interaction between magnetic fields and materials.

Highlights

Introduction to the concept of magnetic force and its application in speakers to convert electrical energy into sound.

Definition of magnetic force, also known as Lorentz force, discovered by Dutch physicist Hendrik Antoon Lorentz.

Explanation of how the direction of the Lorentz force can be determined using the right-hand rule.

Discussion on the generation of Lorentz force by a current-carrying wire in a magnetic field.

Formula for calculating the Lorentz force on a current-carrying wire in a magnetic field: F = B * I * L * sin(θ).

Explanation of how the Lorentz force is zero when the magnetic field is parallel to the electric current.

Analysis of the Lorentz force on a moving electric charge in a homogeneous magnetic field.

Formula for the Lorentz force on a moving charge: F = B * Q * V * sin(θ).

Description of the trajectory of a charged particle in a magnetic field and the resulting centripetal force.

Calculation of the radius of the trajectory of a charged particle using the Lorentz force.

Discussion on the Lorentz force between parallel current-carrying wires in a magnetic field.

Formula for the force between two parallel current-carrying wires: F = (μ₀ * I1 * I2 * L) / (2π * a).

Practical example of determining the direction of the Lorentz force on a current-carrying wire in a magnetic field.

Problem-solving approach to finding the magnitude and direction of the Lorentz force on a wire in a magnetic field.

Explanation of the direction of the Lorentz force on a negatively charged particle moving through a homogeneous magnetic field.

Calculation of the magnetic field strength using the Lorentz force experienced by a moving electron.

Determination of the velocity of a charged particle moving perpendicular to a magnetic field using the Lorentz force.

Analysis of the force experienced by two parallel current-carrying wires and the conditions for attraction or repulsion.

Final problem involving the calculation of the current in a wire based on the force between two wires in a magnetic field.

Conclusion and invitation to watch more videos on the channel for further understanding of magnetic forces.

Transcripts

play00:01

[Musik]

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[Tepuk tangan]

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[Musik]

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Halo teman-teman selamat datang kembali

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di channel YouTube Gia Akademi Semoga

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teman-teman selalu sehat dan terus

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semangat Pernahkah teman-teman

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menggunakan pengeras suara atau speaker

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speaker dapat mengubah energi listrik

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menjadi energi bunyi untuk menghasilkan

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bunyi speaker menerapkan konsep gaya

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magnetik tahukah teman-teman Apa itu

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gaya magnetik apa saja yang bisa

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menghasilkan gaya magnetik kita akan

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membahasnya secara lengkap di video kali

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ini jadi di video ini kita akan belajar

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tentang gaya magnetik simak terus

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videonya

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ya teman-teman gaya magnet

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yang dikenal juga dengan gaya lorence

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ditemukan oleh Henrik Anton lawence

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seorang Fisikawan Belanda Lawrence

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mendefinisikan gaya magnetik sebagai

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gaya yang ditimbulkan oleh medan

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magnetik pada arus

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listrik arah gaya lorence dapat

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ditentukan dengan menggunakan kaidah

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tangan kanan berikut ibu jari menyatakan

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arah arus listrik yaitu I jari telunjuk

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menyatakan arah induksi magnet yaitu B

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dan jari tengah menyatakan arah gaya

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lorence yaitu

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F selain menggunakan tiga jari arah gaya

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lorence juga dapat ditentukan dengan

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menggunakan kaidah tangan kanan lainnya

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ibu jari menyatakan arah arus listrik

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yaitu i empat jari lainnya menyatakan

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arah induksi magnetik yaitu B telapak

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tangan menyatakan arah gaya lorence

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yaitu F teman-teman bisa memili milh

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salah satunya ya Nah gaya lorens dapat

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ditimbulkan oleh kawat berarus yang

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berada dalam medan magnetik muatan

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listrik yang bergerak dalam medan

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magnetik dan kawat sejajar berarus

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listrik kita akan membahasnya satu

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persatu pertama kita bahas gaya lorens

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pada kawat berarus yang berada dalam

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medan magnetik jika kawat penghantar

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berarus berada dalam Medan magnetk

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arah arus dan arah medan magnetik

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membentuk sudut Teta maka akan

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dihasilkan gaya lorens yang dirumuskan

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dengan persamaan f = b * i * l * Sin

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Teta dengan F gaya lorence satuannya

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Newton B induksi magnetik satuannya

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Tesla I kuat arus listrik satuannya

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amper l panjang kawat penghantar ya

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meter dan Teta sudut antara B dengan I

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ingat ya teman-teman jika B sejajar

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dengan I gaya lorens bernilai

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0 selanjutnya gaya lorens pada muatan

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listrik yang bergerak dalam medan

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magnetik jika muatan listrik sebesar Q

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bergerak dengan kecepatan V dalam sebuah

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medan magnet homogen B dengan arah V dan

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arah B membentuk sudut t

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maka akan dihasilkan gaya lorens yang

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dirumuskan dengan persamaan f = b * Q *

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V * Sin Teta dengan F gaya Loren

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satuannya Newton B induksi magnetik

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satuannya Tesla Q muatan listrik yang

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bergerak satuannya coulom V kecepatan

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gerak muatan listrik satuannya

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met/s dan Teta sudut antara B dengan V

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arah gaya lorens pada muatan listrik

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yang bergerak dalam medan magnetik ini

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bergantung pada jenis muatan partikelnya

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jika muatan Q adalah muatan positif maka

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arah V akan sejajar dengan I sedangkan

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jika muatan Q adalah muatan negatif maka

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arah V berlawanan dengan

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I jika arah medan magnet B tegak lurus

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dengan arah kecepatan V nilai Teta 90

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derajat menyebabkan lintasan muatan

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berbentuk lingkaran sehingga muatan

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mengalami gaya sentripetal yang besarnya

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sama dengan gaya Loren F = FS B * Q * V

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* Sin 90 derajat = m * v² / r sehingga

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besar jari-jari lintasan muatan dapat

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ditentukan dengan persamaan R sama = m *

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v / b * Q dengan F gaya lorens dan FS

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gaya sentripetal keduanya dalam satuan

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Newton B induksi magnetik satuannya

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Tesla Q muatan partikel satuannya coulom

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V kecepatan gerak muatan satuannya

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meter/s m massa partikel muatan

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satuannya kilogram dan r jari-jari

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lintasan muatan satuannya

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meter terakhir gaya lorence pada kawat

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sejajar berarus listrik jika ada dua

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buah kawat yang memiliki panjang l

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kemudian dialiri arus listrik sebesar i

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dan kedua kawat tersebut diletakkan pada

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medan magnetik b maka akan terjadi gaya

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loret jika arah arus searah terjadi gaya

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tarikmenarik yang sama besar sehingga

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bentuk kawat akan cekung jika arah arus

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berlawanan terjadi gaya tolak-menolak

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yang sama besar sehingga bentuk kawat

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akan

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cembung besar gaya lorens pada kawat

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sejajar berarus listrik dapat ditentukan

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dengan persamaan F1 = F2 = 0 * I1 * I2 *

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l / 2P * a dengan F1 dan F2 gaya lorens

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pada masing-masing kawat satuannya

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Newton I1 dan I2 kuat arus listrik pada

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masing-masing kawat satuannya amper mi0

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permeabilitas dalam ruang hampa nilainya

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4P *

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10^-7 weber/ AMPM l panjang

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masing-masing kawat satuannya meter dan

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a Jarak antara kedua kawat satuannya

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meter sampai di sini teman-teman paham

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ya agar teman-teman semakin paham Mari

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kita selesaikan contoh soal

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berikut soal pertama diberikan gambar

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sepotong kawat berarus listrik searah

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sumbu zat positif berada dalam medan

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magnetik homogen searah sumbu y positif

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kita diminta menentukan arah gaya Loren

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untuk menjawab soal ini kita bisa

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menggunakan kaidah tangan kanan ibu jari

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menunjukkan arah arus se arah sumbu z

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positif yaitu ke atas empat jari lain

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menunjukkan arah medan magnetik searah

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sumbu y positif yaitu ke kanan maka arah

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gaya lorens ditunjukkan oleh arah

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telapak tangan searah sumbu x negatif

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yaitu masuk

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bidang soal kedua diberikan gambar kawat

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PQ yang panjangnya l = 1,5 m dialiri

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Arus sebesar i = 3 AMP menembus medan

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magnetik B = 200 m Tesla kita diminta

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menentukan besar dan arah gaya lorens

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pada kawat PQ untuk menentukan besar

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gaya lorens kita bisa menggunakan

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persamaan gaya lorens pada kawat berarus

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yang berada dalam medan magnetik yaitu f

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= b * i * l * Sin Teta kita masukkan

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nilainya 2 * 10^-1

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* 3 * 1,5

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* 1 =

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0,9 n untuk menentukan arah gaya lorence

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kita dapat menggunakan kaidah tangan

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kanan ibu jari menunjukkan arah arus I

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yaitu ke kanan jari telunjuk menunjukkan

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arah medan magnetik B yaitu masuk bidang

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maka jari tengah menunjukkan arah gaya

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lorence X F yaitu ke atas jadi

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jawabannya

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B soal selanjutnya diberikan gambar

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partikel bermuatan negatif yang bergerak

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melintasi medan magnet homogen karena

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muatan Q negatif dan arah kecepatan

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geraknya ke kanan maka arah arus I

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berlawanan dengan kecepatan V sehingga

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arah arus I ke kiri medan magnet homogen

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B diberi tanda silang berarti arahnya

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masuk bidang kita diminta menentukan

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arah gaya magnetik partikel tersebut

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untuk menyelesaikan soal ini kita

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gunakan kaidah tangan kanan ibu jari

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menunjukkan arah I yaitu ke kiri empat

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jari lain menunjukkan arah B yaitu masuk

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bidang maka arah telapak tangan

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menunjukkan arah F yaitu ke bawah maka

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Jawabannya

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d soal keempat diketahui Sebuah elektron

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bergerak dengan kecepatan V =

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4,5

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m/s berada di dalam medan magnet dengan

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arah lintasan elektron dan arah medan

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magnet membentuk sudut Teta 30 derajat

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Jika besar muatan elektron Q = 1,6 *

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10^-19 coulom dan mengalami gaya lorens

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F sebesar 5 n kita di minta menentukan

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besar medan magnet B yang dihasilkan

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untuk menjawab soal ini kita gunakan

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persamaan gaya lorens pada muatan yang

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bergerak dalam medan magnet yaitu f = b

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* Q * V * Sin Teta sehingga b = f / Q *

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V * Sin Teta kita masukkan nilainya dan

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kita lakukan perhitungan kita peroleh

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nilai Medan magnet yang dihasilkan

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sebesar

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1,39 * 10^ 19 Tesla jawabannya

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B soal berikutnya Diketahui suatu muatan

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bermassa M = 9 *

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10^-28 kg bergerak memotong secara tegak

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lurus medan magnetik b = 2 Tesla jika

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muatan Q I = 3 *

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10^-9 coulom dan jari-jari lintasannya r

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= 3 cm kita diminta menentukan besar V

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kecepatan muatan tersebut untuk menjawab

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soal ini kita gunakan persamaan

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jari-jari lintasan muatan r = m * v / b

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* Q sehingga v = r * b * Q / M = 3 *

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10^-2

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* 2 * 3 * 10^-9

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/ dengan 9 *

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10^-28 v = 2 * 10^ 17

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m/s Jawabannya

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a soal keen diberikan gambar dua buah

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kawat 1 dan 2 masing-masing panjangnya l

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= 50 cm dialiri arus listrik

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masing-masing I1 = 4 AMP dan I2 = 5 AMP

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jika kedua kawat terpisah sejauh 10 cm

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dan nilai permeabilitas ruang hampa mi0

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= 4P *

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10^-7 weber/ AMPM kita diminta

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menentukan besar dan jenis Gaya yang

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dialami oleh kedua kawat untuk menjawab

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soal ini kita bisa menggunakan persamaan

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gaya lorens pada kawat sejajar berarus

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listrik yaitu F = 0 * I1 * I2 * l / 2pi

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* a kita masukkan nilainya dan kita

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lakukan perhitungan kita peroleh nilai F

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= 200 * 10 -7 n = 2 *

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10^-5 n karena arah arus pada kedua

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kawat sama-sama ke atas maka jenis Gaya

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yang dialami kedua kawat adalah gaya

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tarik

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menarik soal terakhir diberikan gambar

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dua kawat lurus sejajar berjarak a = 20

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cm Apabila I1 = 6 AMP dan kedua kawat

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mengalami gaya tolak-menolak pers satuan

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panjang f/l sebesar

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4,8 * 10^ -5

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n/m dan nilai permeabilitas ruang hampa

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mi0 = 4pi *

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10^-7 weber/ AMPM kita diminta

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menentukan besar dan arah arus I2 untuk

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menjawab soal ini kita gunakan persamaan

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F = 0 * I1 * I2 * l / 2π * a atau f/l =

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0 * I1 * I2 / 2P * a kita masukkan

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nilainya dan kita lakukan perhitungan

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kita peroleh nilai I2 = 8 AMP karena

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gaya yang terjadi adalah gaya

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tolakmenolak maka arah arus di kedua

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kawat berlawanan ini berarti arah arus

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I2 adalah ke bawah atau dari D ke c

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Oke teman-teman demikianlah pembahasan

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kita tentang gaya magnetik jangan lupa

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tonton terus video-video terbaru di

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channel kita ya sampai jumpa di video

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[Tepuk tangan]

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berikutnya

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