MCAT Physics: Circuits, Magnetism, Waves, and Sound

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47 Terms

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Junction Rule

the sum of all currents entering a junction must equal the sum of the currents leaving (conservation of charge)

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Elements in Series have equal

current

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loop rule

The sum of the potential differences (voltages) across all the elements around any closed circuit loop must be zero

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elements in parallel have equal

voltage

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Power output by a battery

P=IV

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Power dissipated across resistors due to thermal energy

P=I^2R=V^2/R

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magnitude of force by a magnetic field

F=qvBsin(theta) (theta= angle between v and B)

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right hand rule for the force by a magnetic wave

1. point your hand in the direction of velocity of the particle

2. curl fingers toward B

3. thumb will be in the direction of the force for a positive particle. MUST FLIP DIRECTION FOR A NEGATIVE CHARGE

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The Force of the magnetic field is always perpendicular to

both the velocity and magnetic field

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In a uniform magnetic field, an accelerated particle will exhibit

uniform circular motion; direction depends on the charge of the particle

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Work done by a magnetic field

0

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magnetic fields are created by

moving electric charges, like a current

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the direction of a magnetic field for a current in a long wire

point your thumb in the direction of the current and curl your fingers around the wire. Your fingers represent the direction of the magnetic field around the wire.

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the magnetic field at a point in space is __ compared to the field line

tangent

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simple harmonic motion

back and forth motion with a restoring force proportional to displacement

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Hooke's Law

F=-kx; restoring force is opposite the displacement from equilibrium and proportional to that displacement and the spring constant

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amplitude

+/-A: the greatest displacement from equilibrium during oscillation

<p>+/-A: the greatest displacement from equilibrium during oscillation</p>
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energy stored in a spring as it stretches/compresses

PE=1/2 kx^2

<p>PE=1/2 kx^2</p>
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work done by the spring

= - delta PE

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conservation of mechanical energy

KE₁ + PE₁ = KE₂ + PE₂; where there is no friction or air resistance (or other non-conservative forces)

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period

time it takes to complete one cycle (returning to the same position and velocity); independent of amplitude

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frequency

number of cycles that occur in one second (Hz)

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relationship between frequency and period

f = 1/T

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frequency of a spring

f = (1/2π)√(k/m)

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propagating oscillations that transfer energy

the medium is not propagated with the energy and oscillates with a series of identical oscillations, slightly out of phase

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wavelength

length of one cycle

<p>length of one cycle</p>
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wave speed

the speed at which a wave travels through a medium. proportional to the wavelength times the frequency

<p>the speed at which a wave travels through a medium. proportional to the wavelength times the frequency</p>
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transverse waves

medium oscillate perpendicular to the direction of wave propagation. Ex: ocean waves, waves on a string, electromagnetic waves

<p>medium oscillate perpendicular to the direction of wave propagation. Ex: ocean waves, waves on a string, electromagnetic waves</p>
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longitudinal waves

medium oscillates parallel to the direction of wave propagation. Ex: sound

<p>medium oscillates parallel to the direction of wave propagation. Ex: sound</p>
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the speed of a wave in a medium depends on the type of wave and physical properties of the medium

this means that v is constant in a medium regardless of the frequency or the wavelength

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a wave moving from one medium to another will maintain the same frequency

the speed can change but the frequency of the wave doesn't change in relation to a change in medium

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speed of sound waves in medium

slowest in gases, faster and liquids, and fastest in solids

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standing waves

waves that are trapped where the endpoints determine which wavelengths can be trapped

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node

point of zero oscillation on a standing wave

<p>point of zero oscillation on a standing wave</p>
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antinode

point of maximum oscillation on a standing wave

<p>point of maximum oscillation on a standing wave</p>
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Standing waves in strings

displacement node at each end

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frequency of a standing wave

f = nf1 (f1=frequency of the first harmonic) (n=harmonic integer)

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first harmonic

fundamental frequency; longest wavelength standing wave that can exist on the string

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wavelength of a standing wave

λ = 2L/n

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Intensity

I=power/area

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intensity of a spherical wave

I is proportional to 1/r^2

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Intensity and amplitude

intensity is proportional to the amplitude squared

<p>intensity is proportional to the amplitude squared</p>
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sound level

beta = 10 (log intensity +12)

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For every increase in the intensity by a factor of 10

add 10 to the sound level

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for every decrease in the intensity by a factor of 10

subtract 10 from the sound level

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doppler shift

shift in the detected frequency of a wave due to the relative motion between the detector and the sound source.

In general:

as they get closer: higher frequency is detected

as they get further: lower frequency is detected

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doppler shift equation (frequency detected)

fd=fs ((350+/-vd)/(350-/+vs))

- "top" sign is towards

- bottom sign is away