PHYSICS II FINALS

End of an era.


Electric Potential Energy


Conservative Forces

A force is conservative if the work it does on an object moving between two points is independent of the path the objects between the points


F=ΔUΔx=Uf−Uixf−xiF=\frac{\Delta U}{\Delta x}=\frac{U_{f}-U_{i}}{x_{f}-x_{i}}


The work depends only upon the initial and final positions of the objects.

Any conservative force can have a potential energy function.


Work-Energy Theorem


Sample 1

q = 3×10-9 C

m = 4

x1 = 1

x2 = 1.5 m

E = 5 N/C

a. W = qEd

= (3×10-9)(5 N/C)(0.5 m)

= 7.5×10-9 Nm or J


b. ΔU=−7.5⋅10−9J\Delta U=-7.5\cdot10^{-9}J

c. ΔK=12mv2\Delta K=\frac12mv^2

7.5×10-9 J = 12(0.004kg)v2\frac12\left(0.004kg\right)v^2

7.5⋅10−9J0.002kg⁡=0.002kgv2⁡0.002kg⁡\sqrt{\frac{7.5\cdot10^{-9}J}{0.002\operatorname{kg}}}=\frac{0.002\operatorname{kg\sqrt{v^2}}}{0.002\operatorname{kg}}

v = 1.94×10-3 m/s


Sample 2

w = ?

E = 450 N/C

q = 3.4×10-6 C

d = 0.1 m


W = (450 N/C)(3.4×10-6)(0.10m) = 1.53×10-4 J


Sample 3

m = 3.25×10-3 kg

d = 0.12 m

vi = 0 m/s

vf = 25 m/s


a. W = ΔKE=12mvf2−12mvi2\Delta KE=\frac12mv_{f}^2-\frac12mv_{i^{}}^2

W = 12(3.25⋅10−3)(24ms)2−12(3.25⋅10−3kg⁡)(0)2\frac12\left(3.25\cdot10^{-3}\right)\left(24\frac{m}{s}\right)^2-\frac12\left(3.25\cdot10^{-3}\operatorname{kg}\right)\left(0\right)^2

W = 12(3.25⋅10−3kg⁡)(25ms)2=1.01J\frac12\left(3.25\cdot10^{-3}\operatorname{kg}\right)\left(25\frac{m}{s}\right)^2=1.01J


b. W = -ΔU\Delta U

ΔU=−W\Delta U=-W

ΔU=−1.01J\Delta U=-1.01J


c. W =qEd → E = Wqd\frac{W}{qd}

E = 1.01J(2.5⋅10−9C)(0.12m)\frac{1.01J}{\left(2.5\cdot10^{-9}C\right)\left(0.12m\right)}

E = 1.01J3.0⋅10−10\frac{1.01J}{3.0\cdot10^{-10}}

E = 3.36×109 N/C

Capacitors and Capacitance


Capacitors are devices for storing charges. In its most basic form, it consists of two metals plates and a dielectric inbetween.


Capacitance

  • Ratio of charge to voltage

    C=QVC=\frac{Q}{V}

    SI Unit is Farad.

    1 Farad = 1 C/ 1 V


Example:

If a 22 μF\mu F capacitor is connected to a 10 V source, the charge is 220 μC\mu C. 220×10-4 C


22μF\mu F = Q10V\frac{Q}{10V}

(10V)(22×10-6) = Q

220×10-4 C


Capacitance depends on three physical characteristics:


C is directly proportional to the distance (d) between the plates.


C is inversely proportional to the distance (d) between the plates.

C =∈Ad\frac{\in A}{d}


Find the capacitance of a 4 cm diameter sensor immersed in oil if the plates are 0.25mm.

(∈\inoil = 3.54×10-11 C2/N2m)

c = (3.54x10−11C2Nm2)(1.26⋅10−3m2)0.25⋅10−3m\frac{\left(3.54x10^{-11}C^2Nm^2\right)\left(1.26\cdot10^{-3}m^2\right)}{0.25\cdot10^{-3}m}

c = 1.78×10-10 F


2.

a. A = 0.0025 m2

∈\in $ = 4.8×10-11 C2/Nm2

d = 0.0001 m


C = (4.6x10−11C2Nm2)(0.0025m2)0.0001m\frac{\left(4.6x10^{-11}C^2Nm^2\right)\left(0.0025m^2\right)}{0.0001m}

C = 1.2×10-9 F


b. V = qc=2⋅10−8C1.2⋅10−9F=16.7V\frac{q}{c}=\frac{2\cdot10^{-8}C}{1.2\cdot10^{-9}F}=16.7V

E = Vd=16.7V0.0001m\frac{V}{d}=\frac{16.7V}{0.0001m}

= 1.67×105 V/m


A = 8.0×10-4 m2

∈\in mica= 4.8×10-11 C2/Nm2

∈\in glass = 7.0×10-11 C2/Nm2

d = 5 mm/0.005 m


The plate area is half of 8×10-4=4×10-4, since half of the space is filled with glass and mica.


C = Cglass + Cmica

=(7⋅10−11)(4⋅10−4)5⋅10−3m+(4.8⋅10−11)(4⋅10−4)5⋅10−3m\frac{\left(7\cdot10^{-11}\right)\left(4\cdot10^{-4}\right)}{5\cdot10^{-3}m}+\frac{\left(4.8\cdot10^{-11}\right)\left(4\cdot10^{-4}\right)}{5\cdot10^{-3}m}

= 9.44×10-12 Farad


Series Capacitor Rules


Capacitance

a. CT = 11C1+1C2+1C3…\frac{1}{\frac{1}{C_1}+\frac{1}{C_2}+\frac{1}{C_3}\ldots}


Charge

b. qT = q1 = q2 = q3…


Voltage

VT = V1 + V2 + V3…


Parallel Capacitor Rules


Capacitance

CT = C1 + C2 + C3…


Charge

qT = q1 + q2 + q3…


Voltage

VT = V1 = V2 = V3…

Series Problems


If a 0.001μF\mu F capacitor is connected in series with an 800 pF capacitor and subject to potential difference of 50 V. Find a. total capacitance, b. charge stored in each capacitor, and c. potential difference across each capacitor.


a. CT = 110.001μF+1800pF=4.44⋅1010F\frac{1}{\frac{1}{0.001\mu F}+\frac{1}{800pF}}=4.44\cdot10^{10}F


b. qT = CV

= (4.44×10 F)(50 V) = 2.22×10-8C


c. V1 = qc\frac{q}{c}

= 2.22⋅10−8C0.001⋅10−6F=22.2V\frac{2.22\cdot10^{-8}C}{0.001\cdot10^{-6}F}=22.2V


V2 = qc\frac{q}{c}

= 2.22⋅10−8C800⋅10−12F=27.8V\frac{2.22\cdot10^{-8}C}{800\cdot10^{-12}F}=27.8V


To capacitors with 2.0 F and 3.0 F capacitance are connected in series and subjected to a potential difference of 120 V. Find a) total capacitance, b) charge stored in each capacitor, and c) potential difference across each capacitor.


a. CT = 112+13=1.2F\frac{1}{\frac12+\frac13}=1.2F

b. qT = CV = (1.2 F)(120 V) = 144 C

q1 = q2 = 144 C

c. V1 = 144C2F=72V\frac{144C}{2F}=72V

V2 = 144C3F=48V\frac{144C}{3F}=48V


Parallel Problems


A 10 F capacitor is connected in parallel with a 5 F capacitor and 4 F, and is subjected to a potential difference of 120 V. What is the total capacitance of the system? Find the individual charge and potential difference in each capacitor.


a. CT = 10 F + 5 F + 4 F = 19 F

b. qT = CTVT = (19 F)(120 V) = 2280 C

c. V1 = V2 = V3 = 120 V


Find

a. Total Capacitance

b. Individual Charge

c. Potential Difference in each capacitor


a. C1-2 = 1110F+15F=3.33F\frac{1}{\frac{1}{10F}+\frac{1}{5F}}=3.33F


CT = C1-2 + C3 = 4 F + 3.33 F = 7.33 F


b. qT = (7.33 F)(120 V) = 879.6 C


q1-2 = (3.33 F)(120 V) = 399.6 C

q3 = (4 F)(120 V) = 480 C


V1 = 399.6C10F=39.96V\frac{399.6C}{10F}=39.96V

V2 = 399.6C5F=79.92V\frac{399.6C}{5F}=79.92V

V3 = 480C4F=120V\frac{480C}{4F}=120V


W = U = 12qV=12cv2=q22c\frac12qV=\frac12cv^2=\frac{q^2}{2c}


How much energy is stored by a 35 μF\mu F capacitor when the charge on each plate is 2500 μC\mu C? What is the potential difference the plates of the capacitor?


C = 35×10-6F

q = 2500×10-6C

U = (2500⋅10−6)22(35⋅10−6)=0.09J\frac{\left(2500\cdot10^{-6}\right)^2}{2\left(35\cdot10^{-6}\right)}=0.09J


U = 12qV→V=2Uq\frac12qV\to V=\frac{2U}{q}

V = 2(0.09J)2500⋅10−6C=72V\frac{2\left(0.09J\right)}{2500\cdot10^{-6}C}=72V

Electric Current

Static Electricity vs. Electric Current


Static Electricity is a one-time event.


While Electric Currents are constantly flowing


Electric Current (I) is the rate at which charge passes a given point in an electric circuits.


SI - Ampere Formula I = Δqt\frac{\Delta q}{t}

Andre Marie Ampere I = C/s Ampere (A)


An ammeter is a device used to measure current. It is always connected in series with the circuit.


Examples


A cross section of wire is isolated

20 C = Δ\Deltaq I = 20C40s\frac{20C}{40s}

40 s = t I = 0.5 A


Alternating Current vs Direct Current

AC - Electron flow in alternating directions. It is produced by proven plants.


DC - Electrons flow in one direction. It is caused by batteries.


Electrical Resistance

(R) Resistance is the opposition of a material to the flow of electric current .


The resistance is the ratio of the potential difference (v) and the current (I)


R = VI\frac{V}{I}


Resistance are devices that limit current flow.


Factors that affect the resistance of a wire:


  1. Length (L): Increasing the length (L) of the wire will increase the resistance. Decreasing the length will decrease the resistance.


R = L


  1. Area (A): Increasing the cross-sectional area (A) of a wire will decrease the wires resistance.


R = 1A\frac{1}{A}


A = πr2\pi r^2


  1. Resistivity (ρ)\left(\rho\right): This is a characteristic of a material that depends on it’s electronic structure. The higher the resistivity, the higher resistance and vice versa.


R = ρ\rho


  1. Temperature - as temperature increases, resistance and resistivity increases for conductors, and decreases for insulators.


Full Equation

R = ρLA\frac{\rho L}{A}


Short, thick, & cold wires = low resistance.


Long, thin, & hot wires = high resistance.


  1. Determine the resistance of a 4m copper wire with a diameter of 2 mm. Assume temperature is 20 Co

    ρ\rho copper = 1.72×10-8Ω⋅m\Omega\cdot m


    A = π(1⋅10−6m2)\pi\left(1\cdot10_{}^{-6}m^2\right)

    = 3.14×10-6m2


    R = (1.72⋅10−8Ω⋅m)(4m)3.14⋅10−6m2\frac{\left(1.72\cdot10^{-8}\Omega\cdot m\right)\left(4m\right)}{3.14\cdot10^{-6}m^2}


R = 0.022Ω\Omega


  1. An insulated wire 1.5 m long and made of copper with a diameter of 2.3 mm.


a. What is the resistance of the extension cord?

b. If an aluminum wire of the same length will be used instead of copper, what should be the diameter of the aluminum wire for the cord to have the same resistance.


a.


RI=ρLπr2=(1.72⋅10−8m)(1.5m)π(1.15⋅10−3m)\frac{R}{I}=\frac{\rho L}{\pi r^2}=\frac{\left(1.72\cdot10^{-8}m\right)\left(1.5m\right)}{\pi\left(1.15\cdot10^{-3}m\right)}

= 0.0062Ω\Omega


b.

ρlRπ=(2.62⋅10−8m)(1.5m)(0.0062Ω)π=0.0015m\sqrt{\frac{\rho l}{R\pi}}=\sqrt{\frac{\left(2.62\cdot10^{-8}m\right)\left(1.5m\right)}{\left(0.0062\Omega\right)\pi}}=0.0015m


  1. Determine the length of a copper wire that has a resistance of .172Ω\Omega and area of 1×10-4m2, The resistivity of copper is 1.72×10-8Ωm\Omega m


R = ρLAA\frac{\rho LA}{A}

ARρ=ρLρ\frac{AR}{\rho}=\frac{\rho L}{\rho}

L=ARρL=\frac{AR}{\rho}


L=(0.001m2)(0.172Ω)1.72⋅10−8ΩmL=\frac{\left(0.001m^2\right)\left(0.172\Omega\right)}{1.72\cdot10^{-8}\Omega m}

L = 10000 m

Ohm’s Law


R =VI\frac{V}{I}


I = VR\frac{V}{R} ; V = IR


  1. V = 12 V

    I = 0.10 A


R = 12V0.10A\frac{12V}{0.10A}

R = 120Ω\Omega


  1. V = (0.5 A)(20 A)


  1. V = 110 V

    I = 15 A


R = 110V15A\frac{110V}{15A}

= 7.3Ω\Omega

Electromotive Force (ϵ\epsilon) is the potential difference across the terminals of a cell when no current is flowing. It is the voltage indicated on a battery.


Terminal Voltage (TV) is the potential difference across the terminals of a cell when current flows.


TV = ϵ\epsilon - IR


  1. ϵ=1.5V\epsilon=1.5V

    TV = 1.5 V - 0.5 A

    0.5r = 1.5 V - 1.35 V

    0.45r0.45=0.15V0.45\frac{0.45r}{0.45}=\frac{0.15V}{0.45}

    r = 0.33 Ω\Omega


  1. A cell has a terminal voltage of 50 V for a current of 10 A, and 54 V for a current of 6 A. Find the electromotive force and internal resistance of the cell.


TV =ϵ\epsilon- IR


50 =ϵ−10r\epsilon-10r 50 = ϵ−10r\epsilon-10r

-54 =ϵ+6r\epsilon+6r 50 = ϵ−10(1)\epsilon-10\left(1\right)

−4−4=−4r−4\frac{-4}{-4}=\frac{-4r}{-4}

r = 1Ω\Omega


50 = ϵ−10r\epsilon-10r

50 = ϵ−10(1)\epsilon-10\left(1\right)

50 = ϵ−10\epsilon-10

50 + 10 = ϵ\epsilon

60 V = ϵ\epsilon



Capacitor Rules


Series


Capacitance

CT = 11C1+1C2+1C3…\frac{1}{\frac{1}{C_1}+\frac{1}{C_2}+\frac{1}{C_3}\ldots}


Charge

qT = q1 = q2 = q3 …


Voltage

VT = V1 + V2 + V3 …


Parallel


Capacitance

CT = C1 + C2 + C3 …


Charge

qT = q1 = q2 = q3 …


Voltage

VT = V1 = V2 = V3 …


Resistors


Series


Resistance

RT = R1 + R2 + R3 …


Current

IT = I1 = I2 = I3…


Voltage

VT = V1 + V2 + V3…


Parallel


Resistance

RT = 11R1+1R2+1R3…\frac{1}{\frac{1}{R_1}+\frac{1}{R_2}+\frac{1}{R_3}\ldots}


Current

IT = I1 + I2 + I3


Voltage

VT = V1 = V2 = V3


Sample 1:


a.

R2-3 = 3.5Ω+2.5Ω=6Ω3.5\Omega+2.5\Omega=6\Omega

R2-4 = 116Ω+124Ω=4.8Ω\frac{1}{\frac{1}{6\Omega}+\frac{1}{24\Omega}}=4.8\Omega

R1-5 = 5Ω+4.8Ω+9.2Ω=9.2Ω5\Omega+4.8\Omega+9.2\Omega=9.2\Omega


b.

IT = 30V19Ω\frac{30V}{19\Omega} = 1.58A

I1 = 1.58 A

I2-4 = 1.58 A

I5 = 1.58 A


I4 = 7.58V24Ω=0.32A\frac{7.58V}{24\Omega}=0.32A

I2-3 = 7.58V6Ω=1.26A\frac{7.58V}{6\Omega}=1.26A


V = IR

V1 = (1.58A)(3Ω)=7.9V\left(1.58A\right)\left(3\Omega\right)=7.9V

V2-4 = (1.58A)(4.8Ω)=7.58V\left(1.58A\right)\left(4.8\Omega\right)=7.58V

V5 = (1.58A)(9.2Ω)=14.54V\left(1.58A\right)\left(9.2\Omega\right)=14.54V


V4 = 7.58 V

V2 = (1.26A)(3.5Ω)=4.41V\left(1.26A\right)\left(3.5\Omega\right)=4.41V

V3 = (1.26A)(2.5Ω)=3.15V\left(1.26A\right)\left(2.5\Omega\right)=3.15V