Physics 2 Cheat Sheet
Coulomb's Law and Electric Forces
Coulomb's Law: Describes the force between two charges.
\[ F = k \frac{|q_1 q_2|}{r^2} \]
Where:
- \( k = 8.99 \times 10^9 \, \text{Nm}^2/\text{C}^2 \)
- \( q_1, q_2 \) are the magnitudes of the charges.
- \( r \) is the distance between the charges.
Types of Charge
Positive and negative charges attract, while like charges repel.
Properties of Charges
Conductors: Allow free movement of electrons.
Insulators: Electrons are bound and cannot move freely.
Electric Field
Electric Field (E): A field around a charged object where other charges experience a force.
Formula: The electric field due to a point charge is given by:
\[ \vec{E} = k_e \frac{q}{r^2} \hat{r} \]
Where:
- \( \vec{E} \) is the electric field vector.
- \( k_e \) is Coulomb's constant (\( 8.99 \times 10^9 \, \text{N m}^2/\text{C}^2 \)).
- \( q \) is the source charge.
- \( r \) is the distance from the charge.
- \( \hat{r} \) is the unit vector in the direction from the charge to the point of interest.
Electric Field Lines
Electric field lines represent the direction of the electric field. They point away from positive charges and toward negative charges. The density of the lines represents the strength of the field.
Superposition Principle
The net electric field caused by multiple charges is the vector sum of the electric fields due to individual charges:
\[ \vec{E}_{net} = \vec{E}_1 + \vec{E}_2 + \vec{E}_3 + \dots \]
Electric Potential
Electric Potential (V): The work done per unit charge to move a test charge from infinity to a point in space.
Formula: For a point charge:
\[ V = k_e \frac{q}{r} \]
Where:
- \( V \) is the electric potential.
- \( k_e \) is Coulomb's constant.
- \( q \) is the source charge.
- \( r \) is the distance from the charge.
Relation Between Electric Field and Electric Potential
The electric field is the negative gradient of the electric potential:
\[ \vec{E} = -\nabla V \]
This indicates that the electric field points in the direction of decreasing potential.
Capacitance
Capacitance (C): The ability of a system to store charge per unit voltage.
Formula: Capacitance is defined as:
\[ C = \frac{Q}{V} \]
Where:
- \( C \) is the capacitance.
- \( Q \) is the charge stored on the capacitor.
- \( V \) is the voltage across the capacitor.
Capacitance of a Parallel Plate Capacitor
The capacitance of a parallel plate capacitor is given by:
\[ C = \frac{\epsilon_0 A}{d} \]
Where:
- \( \epsilon_0 \) is the permittivity of free space (\( 8.85 \times 10^{-12} \, \text{F/m} \)).
- \( A \) is the area of one of the plates.
- \( d \) is the separation between the plates.
Energy Stored in a Capacitor
The energy \( U \) stored in a capacitor is given by:
\[ U = \frac{1}{2} C V^2 \]
Current and Resistance
Electric Current (I): The flow of electric charge through a conductor.
Formula: Current is defined as:
\[ I = \frac{dQ}{dt} \]
Where:
- \( I \) is the current (in amperes).
- \( Q \) is the charge.
- \( t \) is the time.
Ohm's Law
Ohm's Law relates the voltage \( V \), current \( I \), and resistance \( R \) in a circuit:
\[ V = IR \]
Resistance of a Material
The resistance of a material is given by:
\[ R = \rho \frac{L}{A} \]
Where:
- \( R \) is the resistance.
- \( \rho \) is the resistivity of the material.
- \( L \) is the length of the conductor.
- \( A \) is the cross-sectional area of the conductor.
Power in Electric Circuits
The power dissipated in a resistor is given by:
\[ P = IV = I^2R = \frac{V^2}{R} \]
Direct Current (DC) Circuits
DC circuits consist of resistors, capacitors, and batteries. The current flows in a single direction.
Resistors in Series
For resistors in series, the equivalent resistance \( R_{eq} \) is the sum of the individual resistances:
\[ R_{eq} = R_1 + R_2 + R_3 + \dots \]
Resistors in Parallel
For resistors in parallel, the reciprocal of the equivalent resistance \( R_{eq} \) is the sum of the reciprocals of the individual resistances:
\[ \frac{1}{R_{eq}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + \dots \]
Capacitors in Series and Parallel
For capacitors in series:
\[ \frac{1}{C_{eq}} = \frac{1}{C_1} + \frac{1}{C_2} + \frac{1}{C_3} + \dots \]
For capacitors in parallel:
\[ C_{eq} = C_1 + C_2 + C_3 + \dots \]
Magnetism
Magnetic Field (\( \vec{B} \)): A field that exerts a force on moving charges and current-carrying wires.
Units: Tesla (T), where 1 T = 1 N/(A·m).
Magnetic Force on a Moving Charge
The magnetic force \( \vec{F}_B \) on a charge \( q \) moving with velocity \( \vec{v} \) in a magnetic field \( \vec{B} \) is given by:
\[ \vec{F}_B = q\vec{v} \times \vec{B} \]
The direction of the force is given by the right-hand rule.
Magnetic Force on a Current-Carrying Wire
The force on a straight current-carrying wire of length \( L \) in a uniform magnetic field is given by:
\[ \vec{F} = I\vec{L} \times \vec{B} \]
Where:
- \( I \) is the current in the wire.
- \( L \) is the length of the wire.
- \( \vec{B} \) is the magnetic field.
Biot-Savart Law
The Biot-Savart Law describes the magnetic field generated by a steady current:
\[ d\vec{B} = \frac{\mu_0 I d\vec{L} \times \hat{r}}{4\pi r^2} \]
Where:
- \( d\vec{B} \) is the infinitesimal magnetic field.
- \( \mu_0 \) is the permeability of free space (\( 4\pi \times 10^{-7} \, \text{T·m/A} \)).
- \( I \) is the current.
- \( d\vec{L} \) is the infinitesimal length element of the current-carrying wire.
- \( \hat{r} \) is the unit vector from the current element to the point of interest.
- \( r \) is the distance from the current element to the point of interest.
Ampère's Law
Ampère's Law relates the magnetic field around a closed loop to the total current passing through the loop:
\[ \oint \vec{B} \cdot d\vec{l} = \mu_0 I_{\text{enc}} \]
Where \( I_{\text{enc}} \) is the total current enclosed by the loop.
Electromagnetic Induction
Faraday's Law of Electromagnetic Induction: A changing magnetic field induces an electromotive force (EMF) in a circuit:
\[ \mathcal{E} = -\frac{d\Phi_B}{dt} \]
Where:
- \( \mathcal{E} \) is the induced EMF.
- \( \Phi_B \) is the magnetic flux.
Magnetic Flux
Magnetic flux through a surface is given by:
\[ \Phi_B = \int \vec{B} \cdot d\vec{A} \]
Where:
- \( \vec{B} \) is the magnetic field.
- \( d\vec{A} \) is the area element vector perpendicular to the surface.
Lenz's Law
Lenz's Law states that the direction of the induced EMF and current will oppose the change in magnetic flux that produced it.
Inductance
Inductance (L): The property of a circuit element that opposes changes in current flowing through it.
Self-Inductance: The induced EMF in a coil is proportional to the rate of change of current through the coil:
\[ \mathcal{E} = -L \frac{dI}{dt} \]
Inductance of a Solenoid
The inductance of a solenoid is given by:
\[ L = \frac{\mu_0 N^2 A}{l} \]
Where:
- \( \mu_0 \) is the permeability of free space.
- \( N \) is the number of turns of the solenoid.
- \( A \) is the cross-sectional area of the solenoid.
- \( l \) is the length of the solenoid.
Energy Stored in an Inductor
The energy \( U \) stored in an inductor is given by:
\[ U = \frac{1}{2} L I^2 \]
Alternating Current (AC) Circuits
Alternating Current (AC): Current that varies sinusoidally with time.
AC Voltage: The voltage in an AC circuit is given by:
\[ V(t) = V_0 \sin(\omega t) \]
Where:
- \( V_0 \) is the peak voltage.
- \( \omega \) is the angular frequency (\( \omega = 2\pi f \)).
- \( t \) is the time.
Resistors in AC Circuits
For a resistor in an AC circuit, the current and voltage are in phase. The voltage across the resistor is:
\[ V_R(t) = I_0 R \sin(\omega t) \]
Inductors in AC Circuits
For an inductor in an AC circuit, the current lags the voltage by 90 degrees. The voltage across the inductor is:
\[ V_L(t) = I_0 \omega L \cos(\omega t) \]
Capacitors in AC Circuits
For a capacitor in an AC circuit, the current leads the voltage by 90 degrees. The voltage across the capacitor is:
\[ V_C(t) = \frac{I_0}{\omega C} \cos(\omega t) \]
Impedance in AC Circuits
Impedance (Z): The total opposition to current in an AC circuit, combining resistance, inductive reactance, and capacitive reactance.
Formula:
\[ Z = \sqrt{R^2 + \left( \omega L - \frac{1}{\omega C} \right)^2} \]
Power in AC Circuits
The average power delivered to an AC circuit is given by:
\[ P_{avg} = \frac{1}{2} V_0 I_0 \cos(\phi) \]
Where \( \phi \) is the phase angle between the voltage and current.
Electromagnetic Waves
Electromagnetic Waves: Waves of electric and magnetic fields that propagate through space. They are transverse waves and travel at the speed of light in a vacuum.
Speed of Light: The speed of electromagnetic waves in a vacuum is:
\[ c = 3.00 \times 10^8 \, \text{m/s} \]
Wave Equation for Electromagnetic Waves
The electric and magnetic fields in an electromagnetic wave satisfy the wave equation:
\[ \frac{\partial^2 E}{\partial x^2} = \frac{1}{c^2} \frac{\partial^2 E}{\partial t^2} \]
And similarly for the magnetic field \( B \).
Energy in Electromagnetic Waves
The energy density \( u \) of an electromagnetic wave is given by:
\[ u = \frac{1}{2} \epsilon_0 E^2 + \frac{1}{2} \frac{B^2}{\mu_0} \]
Where \( \epsilon_0 \) is the permittivity of free space and \( \mu_0 \) is the permeability of free space.
Intensity of Electromagnetic Waves
The intensity \( I \) of an electromagnetic wave is the power per unit area:
\[ I = \frac{P}{A} = \frac{c \epsilon_0 E_0^2}{2} \]
Where \( E_0 \) is the peak electric field.
Optics
Reflection: The bouncing back of light when it hits a surface.
Law of Reflection: The angle of incidence equals the angle of reflection (\( \theta_i = \theta_r \)).
Refraction
Snell's Law: The relationship between the angles of incidence and refraction when light passes from one medium to another:
\[ n_1 \sin \theta_1 = n_2 \sin \theta_2 \]
Where \( n_1 \) and \( n_2 \) are the indices of refraction of the two media.
Lens and Mirror Equations
The lens and mirror equation relates the object distance (\( d_o \)), the image distance (\( d_i \)), and the focal length (\( f \)):
\[ \frac{1}{f} = \frac{1}{d_o} + \frac{1}{d_i} \]
Magnification
Magnification \( M \) is the ratio of the height of the image (\( h_i \)) to the height of the object (\( h_o \)):
\[ M = \frac{h_i}{h_o} = -\frac{d_i}{d_o} \]