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Physics 12 Final Exam - Cheatsheet

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Physics 12 Final Exam - Cheatsheet

STUDY GUIDE

๐ŸŽ“ Physics 12 Final Exam - Study Guide

๐Ÿ“‹ Course Structure

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๐Ÿ“š Physics 12 โ”œโ”€โ”€ ๐Ÿ“– Chapter 1: Electric Charges and Fields โ”‚ โ”œโ”€โ”€ ๐Ÿ”น Electric Charge and its Properties โ”‚ โ”œโ”€โ”€ ๐Ÿ”น Coulomb's Law โ”‚ โ””โ”€โ”€ ๐Ÿ”น Forces between Multiple Charges: Superposition Principle โ”œโ”€โ”€ ๐Ÿ“– Chapter 2: Electric Field โ”‚ โ”œโ”€โ”€ ๐Ÿ”น Definition and Properties of Electric Field โ”‚ โ”œโ”€โ”€ ๐Ÿ”น Electric Field Lines โ”‚ โ”œโ”€โ”€ ๐Ÿ”น Electric Dipole and its Field โ”‚ โ””โ”€โ”€ ๐Ÿ”น Dipole in a Uniform External Field โ”œโ”€โ”€ ๐Ÿ“– Chapter 3: Gauss's Law and its Applications โ”‚ โ”œโ”€โ”€ ๐Ÿ”น Electric Flux โ”‚ โ”œโ”€โ”€ ๐Ÿ”น Gauss's Law โ”‚ โ””โ”€โ”€ ๐Ÿ”น Applications of Gauss's Law: Infinite Wire, Plane Sheet, and Spherical Shell
Section 2

๐Ÿ“– Chapter 1: Electric Charges and Fields

What this chapter covers: This chapter introduces the fundamental concepts of electric charge, its properties, and the force between charges as described by Coulomb's law. It explains the concepts of additivity, conservation, and quantization of charge. It also introduces the electric field and the superposition principle for calculating forces between multiple charges.

๐Ÿ”‘ Essential Concepts & Formulas

Concept/FormulaDefinition/EquationWhen to UseQuick Check
Quantization of Chargeq=neq = ne, where nn is an integer and e=1.602ร—10โˆ’19e = 1.602 \times 10^{-19} CCalculating charge on an object due to excess or deficit of electrons.Check if the calculated charge is an integer multiple of ee.
Coulomb's Law (Scalar)F=kq1q2r2F = \frac{k q_1 q_2}{r^2}, where k=14ฯ€ฯต0โ‰ˆ9ร—109Nm2/C2k = \frac{1}{4\pi\epsilon_0} \approx 9 \times 10^9 Nm^2/C^2Calculating the magnitude of the force between two point charges.Ensure charges are in Coulombs and distance is in meters. Check for reasonable magnitude of force.
Coulomb's Law (Vector)F12=kq1q2r2r^21\mathbf{F}_{12} = \frac{k q_1 q_2}{r^2} \hat{\mathbf{r}}_{21}Calculating the force vector between two point charges.Ensure correct direction is used. r^21\hat{\mathbf{r}}_{21} is the unit vector from q2q_2 to q1q_1.
Superposition PrincipleF1=โˆ‘i=2nF1i\mathbf{F}_1 = \sum_{i=2}^{n} \mathbf{F}_{1i}Calculating the net force on a charge due to multiple other charges.Vectorially add all forces acting on the charge.

๐Ÿ› ๏ธ Problem Types

Type A: Calculating Net Force on a Charge due to Multiple Charges

Setup: "When you encounter a system of three or more point charges and need to find the net force on one of them."

Method: "Apply the superposition principle. Calculate the force on the charge due to each of the other charges individually using Coulomb's law. Then, find the vector sum of all these forces to get the net force."

Example: "Three charges, q1=1ฮผCq_1 = 1 \mu C, q2=2ฮผCq_2 = 2 \mu C, and q3=โˆ’3ฮผCq_3 = -3 \mu C, are placed at the vertices of an equilateral triangle with side length 10 cm. Find the net force on q1q_1."

Type B: Determining Equilibrium Position of a Charge

Setup: "If presented with two fixed charges and asked to find where a third charge must be placed for it to be in equilibrium (net force is zero)."

Method: "Set up a coordinate system. Write out the force equations on the third charge due to the other two. Solve for the position where the net force is zero. Consider the signs of the charges to determine if the equilibrium point is between the charges or outside."

Example: "Two charges, +q+q and +4q+4q, are separated by a distance rr. Find the location of a third charge, โˆ’q-q, such that the net force on it is zero."

๐Ÿงฎ Solved Example

Problem: Two point charges, q1=+10nCq_1 = +10 nC and q2=โˆ’20nCq_2 = -20 nC, are separated by a distance of 5 cm. Find the magnitude and direction of the electrostatic force on q1q_1.

Given: q1=10ร—10โˆ’9Cq_1 = 10 \times 10^{-9} C, q2=โˆ’20ร—10โˆ’9Cq_2 = -20 \times 10^{-9} C, r=0.05mr = 0.05 m

Steps:

  1. Identify what you're solving for: The electrostatic force F12\mathbf{F}_{12} on q1q_1 due to q2q_2.
  2. Apply Coulomb's Law: F=kโˆฃq1q2โˆฃr2F = \frac{k \lvert q_1 q_2 \rvert}{r^2}
  3. Perform calculations: F=(9ร—109Nm2/C2)โˆฃ(10ร—10โˆ’9C)(โˆ’20ร—10โˆ’9C)โˆฃ(0.05m)2=7.2ร—10โˆ’4NF = \frac{(9 \times 10^9 Nm^2/C^2) \lvert (10 \times 10^{-9} C)(-20 \times 10^{-9} C) \rvert}{(0.05 m)^2} = 7.2 \times 10^{-4} N
  4. Determine direction: Since q1q_1 is positive and q2q_2 is negative, the force is attractive. Therefore, the force on q1q_1 is directed towards q2q_2.
"
โœ…
Answer: The magnitude of the force is 7.2ร—10โˆ’4N7.2 \times 10^{-4} N, and the direction is towards q2q_2.

โš ๏ธ Common Mistakes

โŒ Mistake 1: Forgetting to use consistent units (e.g., using cm instead of meters in Coulomb's law).

โœ… How to avoid: Always convert all quantities to SI units (meters, Coulombs, etc.) before plugging them into formulas.

โŒ Mistake 2: Incorrectly adding forces vectorially when using the superposition principle.

โœ… How to avoid: Draw a free-body diagram showing all the forces acting on the charge. Resolve each force into its components and then add the components separately.

๐Ÿ’ก Study Tip

Practice drawing free-body diagrams for electrostatic problems. This will help you visualize the forces and ensure that you are adding them correctly.

๐Ÿ“– Chapter 2: Electric Field

What this chapter covers: This chapter introduces the concept of the electric field, which is the force per unit charge. It describes how to calculate the electric field due to point charges and charge distributions. It also covers electric field lines and the behavior of electric dipoles in electric fields.

๐Ÿ”‘ Essential Concepts & Formulas

Concept/FormulaDefinition/EquationWhen to UseQuick Check
Electric FieldE=Fq\mathbf{E} = \frac{\mathbf{F}}{q}Calculating the electric field at a point due to a test charge.Ensure the test charge is small enough not to disturb the source charge.
Electric Field (Point Charge)E=14ฯ€ฯต0Qr2r^\mathbf{E} = \frac{1}{4\pi\epsilon_0} \frac{Q}{r^2} \hat{\mathbf{r}}Calculating the electric field due to a single point charge.Check the direction of the electric field (away from positive, towards negative).
Electric Dipole Momentp=q(2a)\mathbf{p} = q(2\mathbf{a})Calculating the dipole moment of a pair of equal and opposite charges.The direction of p\mathbf{p} is from the negative to the positive charge.
Torque on a Dipoleฯ„=pร—E\boldsymbol{\tau} = \mathbf{p} \times \mathbf{E}Calculating the torque on a dipole in a uniform electric field.The torque tends to align the dipole with the field.

๐Ÿ› ๏ธ Problem Types

Type A: Calculating Electric Field due to a Collection of Point Charges

Setup: "When you have multiple point charges and need to find the electric field at a specific location."

Method: "Calculate the electric field due to each point charge individually. Then, find the vector sum of all these electric fields to get the net electric field."

Example: "Two charges, q1=+5nCq_1 = +5 nC and q2=โˆ’10nCq_2 = -10 nC, are located at (0, 0) and (4 cm, 0), respectively. Find the electric field at the point (2 cm, 0)."

Type B: Determining the Motion of a Charged Particle in an Electric Field

Setup: "If a charged particle is placed in an electric field, it will experience a force and accelerate."

Method: "Use F=qE\mathbf{F} = q\mathbf{E} to find the force on the particle. Then, use Newton's second law (F=ma\mathbf{F} = m\mathbf{a}) to find the acceleration. Use kinematics equations to determine the particle's motion."

Example: "An electron is released from rest in a uniform electric field of 2.0ร—104N/C2.0 \times 10^4 N/C. Determine the acceleration of the electron."

๐Ÿงฎ Solved Example

Problem: A point charge of +2.0ฮผC+2.0 \mu C is placed at the origin. What is the magnitude of the electric field at a point 3.0 m away on the x-axis?

Given: Q=2.0ร—10โˆ’6CQ = 2.0 \times 10^{-6} C, r=3.0mr = 3.0 m

Steps:

  1. Identify what you're solving for: The magnitude of the electric field EE at a distance rr from the charge.
  2. Apply the formula for the electric field due to a point charge: E=14ฯ€ฯต0โˆฃQโˆฃr2E = \frac{1}{4\pi\epsilon_0} \frac{\lvert Q \rvert}{r^2}
  3. Perform calculations: E=(9ร—109Nm2/C2)2.0ร—10โˆ’6C(3.0m)2=2000N/CE = (9 \times 10^9 Nm^2/C^2) \frac{2.0 \times 10^{-6} C}{(3.0 m)^2} = 2000 N/C
"
โœ…
Answer: The magnitude of the electric field is 2000N/C2000 N/C.

โš ๏ธ Common Mistakes

โŒ Mistake 1: Confusing electric field and electric force.

โœ… How to avoid: Remember that the electric field is the force per unit charge.

โŒ Mistake 2: Forgetting that the electric field is a vector quantity and must be added vectorially.

โœ… How to avoid: Resolve the electric field into components and add the components separately.

๐Ÿ’ก Study Tip

Practice sketching electric field lines for various charge configurations. This will help you visualize the electric field and understand its properties.

๐Ÿ“– Chapter 3: Gauss's Law and its Applications

What this chapter covers: This chapter introduces Gauss's law, a powerful tool for calculating electric fields in situations with symmetry. It defines electric flux and presents Gauss's law as a relationship between the electric flux through a closed surface and the enclosed charge. The chapter then applies Gauss's law to calculate the electric field due to various symmetric charge distributions.

๐Ÿ”‘ Essential Concepts & Formulas

Concept/FormulaDefinition/EquationWhen to UseQuick Check
Electric Fluxฮฆ=โˆซEโ‹…dA\Phi = \int \mathbf{E} \cdot d\mathbf{A}Calculating the electric flux through a surface.Ensure the surface is closed for Gauss's law.
Gauss's LawโˆฎEโ‹…dA=Qencฯต0\oint \mathbf{E} \cdot d\mathbf{A} = \frac{Q_{enc}}{\epsilon_0}Relating the electric flux through a closed surface to the enclosed charge.Choose a Gaussian surface that takes advantage of the symmetry of the charge distribution.
Electric Field (Infinite Wire)E=ฮป2ฯ€ฯต0rE = \frac{\lambda}{2\pi\epsilon_0 r}Calculating the electric field due to an infinitely long charged wire.rr is the perpendicular distance from the wire.
Electric Field (Infinite Plane)E=ฯƒ2ฯต0E = \frac{\sigma}{2\epsilon_0}Calculating the electric field due to an infinitely large charged plane.The electric field is uniform and perpendicular to the plane.
Electric Field (Spherical Shell)E=14ฯ€ฯต0Qr2E = \frac{1}{4\pi\epsilon_0} \frac{Q}{r^2} (for r>Rr > R), E=0E = 0 (for r<Rr < R)Calculating the electric field due to a uniformly charged spherical shell.RR is the radius of the shell.

๐Ÿ› ๏ธ Problem Types

Type A: Applying Gauss's Law to Calculate Electric Field for Symmetric Charge Distributions

Setup: "When you have a charge distribution with sufficient symmetry (spherical, cylindrical, planar) and need to find the electric field."

Method: "Choose a Gaussian surface that matches the symmetry of the charge distribution. Apply Gauss's law to relate the electric flux through the Gaussian surface to the enclosed charge. Solve for the electric field."

Example: "A long, straight wire has a uniform linear charge density of ฮป\lambda. Find the electric field at a distance rr from the wire."

Type B: Determining the Charge Enclosed within a Gaussian Surface

Setup: "If you know the electric field on a closed surface, you can use Gauss's law to find the total charge enclosed by the surface."

Method: "Calculate the electric flux through the closed surface. Then, use Gauss's law to relate the electric flux to the enclosed charge: Qenc=ฯต0โˆฎEโ‹…dAQ_{enc} = \epsilon_0 \oint \mathbf{E} \cdot d\mathbf{A}"

Example: "The electric field on the surface of a sphere of radius 0.2 m is measured to be 1000 N/C and points radially inward. Determine the net charge enclosed within the sphere."

๐Ÿงฎ Solved Example

Problem: A uniformly charged solid sphere of radius RR has a total charge QQ. Find the electric field at a point outside the sphere (r>Rr > R).

Given: Total charge QQ, sphere radius RR, r>Rr > R

Steps:

  1. Identify what you're solving for: The electric field EE at a distance rr from the center of the sphere.
  2. Choose a Gaussian surface: A sphere of radius rr centered at the center of the charged sphere.
  3. Apply Gauss's Law: โˆฎEโ‹…dA=Qencฯต0\oint \mathbf{E} \cdot d\mathbf{A} = \frac{Q_{enc}}{\epsilon_0}. Since the electric field is radial and constant on the Gaussian surface, E(4ฯ€r2)=Qฯต0E(4\pi r^2) = \frac{Q}{\epsilon_0}
  4. Solve for E: E=14ฯ€ฯต0Qr2E = \frac{1}{4\pi\epsilon_0} \frac{Q}{r^2}
"
โœ…
Answer: The electric field outside the sphere is E=14ฯ€ฯต0Qr2E = \frac{1}{4\pi\epsilon_0} \frac{Q}{r^2}.

โš ๏ธ Common Mistakes

โŒ Mistake 1: Choosing the wrong Gaussian surface.

โœ… How to avoid: Choose a surface that takes advantage of the symmetry of the charge distribution and on which the electric field is constant and either parallel or perpendicular to the surface.

โŒ Mistake 2: Forgetting that Gauss's law only applies to closed surfaces.

โœ… How to avoid: Make sure that the surface you are using is closed.

๐Ÿ’ก Study Tip

Practice applying Gauss's law to different symmetric charge distributions. This will help you develop a better understanding of how to choose the appropriate Gaussian surface and apply the law correctly.

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