Notes - Fisika - Finals
I should take a walk for a bit
Alternating Current
ƒ=1/T
y=A*sin(ω*t)
E=(E_m)*sin(ω*t)=N⋅B⋅A⋅ω⋅sin(ω*t)
ƒ is frequency
T is period of the current
A is amplitude
ω is angular frequency
(V_effective)=(V_max)/√(,2)
(I_effective)=(I_max)/√(,2)
Oscilloscopes measure maximum voltage (V_max), voltmeters measure effective voltage (V_E). Effective voltage is basically the amount of DC voltage needed to match the AC voltage.
How do you read an oscilloscope?
(V_max)=(s_y)⋅A
T=(s_x)⋅λ
The vertical axis uses a scale based on volts per centimeter.
The horizontal axis uses a scale based on miliseconds per centimeter.
R-L-C
(X_L)=ω*L=2*π*ƒ*L
(X_C)=1/(ω*C)=1/(2*π*ƒ*C)
V=√(,(V_R)^2+((V_L)-(V_C))^2)
I⋅Z=√(,(I*R)^2+(I*(X_L)-I*(X_C))^2)
Z=√(,R^2+((X_L)-(X_C))^2)
I=V/Z=(V_L)/(X_L)=(V_R)/R=(V_C)/(X_C)
tan(θ)=((X_L)-(X_C))/R
(X_L)>(X_C) → Circuit is inductive
(X_C)>(X_L) → Circuit is capacitive
(X_L)=(X_C) → Resonance with ƒ
ƒ=1/(2*π√(,L*C))
I(t)=(I_max)*sin(ω*t)
V(t)=(V_max)*sin(ω*t+θ)
P=I^2*R
Z is impedance, basically the total opposing resistance.
R is resistance from a resistor
(X_L) is inductive resistance
(X_C) is capacitive resistance
(V_L) is voltage across the inductor
(V_C) is voltage across the capacitor
P is dissipation, only taking into account R
In a phasor diagram, (V_R) and I have an angle of 0° (right). (V_L) has an angle of 90° (up) and (V_C) has an angle of 270° (down). This means that (V_L) and (V_C) have opposing directions.
Highlighted Problems
Problem 1
∴(V_max)=3⋅80=240volts
T=8⋅2.5=20ms
∴ƒ=1/(20⋅10^(-3))=1000/20=50Hz
(B)
Problem 2
Voltmeters measure effective voltage.
(V_max)=4⋅10=40volts
∴(V_effective)=40/√(,2)=20√(,2)
T=2⋅8=16ms
∴ƒ=1/(16⋅10^(-3))=1000/16=125/2=62.5Hz
Drawing is easy, so I won't showcase it. The vertical scale is basically how many squares a peak or a valley takes up, and the horizontal scale is how many squares 1 wave takes up.
Problem 3
(V_R)=80volts
(V_max)=100volts
80=(I_max)⋅160
(I_max)=0.5A
(V_RL)=100=√(,80^2+(V_L)^2)
(V_L)=√(,100^2-80^2)=60=(X_L)⋅I
(X_L)=60/0.5=120Ω
Z=100=√(,80^2+(Δ(V))^2)
100^2-80^2=(Δ(V))^2
Δ(V)=√(,100^2-80^2)=60
Δ(V)=(V_C)-(V_L)=60
You can swap the order of (V_C) and (V_L) to find a nonzero solution.
(V_C)=60+60=120
120=0.5⋅(X_C)
(X_C)=240Ω
Problem 4
Well, let's just get right to it.
V(t)=100√(,2)*sin(100*t)
(X_L)=2⋅100=200Ω
(X_C)=1/(10⋅100⋅10^(-6))=1000Ω (it's supposed to be micro faradays)
tan(θ)=(200-1000)/600=-4/3
∴θ=-53° (a)
Rangkaian bersifat kapasitif karena (X_C)>(X_L) (b)
Z=√(,600^2+(200-1000)^2)=1000Ω
100√(,2)=1000⋅(I_max)
(I_max)=0.1√(,2)
I(t)=0.1√(,2)*sin(100*t+53°) (c)
(V_R)=600⋅0.1=60volts
(V_L)=200⋅0.1=20volts
(V_C)=1000⋅0.1=100volts
(d)
P=1/10^2⋅600=6W (e)
Black Body Radiation
Use a calculator.
P=e⋅σ⋅A⋅T^4
I=P/(4*π*r^2)
P is radiation, joules per second, aka watts.
e is coefficient of emissivity
σ is the Stefan Boltzmann constant, 5.67⋅10^(-8)
A is the area
T is temperature in Kelvin
I is intensity, with r being distance
Highlighted Problems
Problem 1
A=(10⋅10^(-2))^2=1⋅10^(-2)⋅2
P=5.67⋅10^(-8)⋅8/10⋅1⋅10^(-2)⋅2⋅(727+273)^4=2⋅453.6W
Problem 2
The given variables are R, r, I
I=P/(4*π*r^2)
P=4*I*π*r^2=σ*A*T^4
4*I*π*r^2=σ⋅(4*π*R^2)⋅T^4
I*r^2=σ*R^2*T^4
T^4=(I*r^2)/(σ*R^2)
=(1400⋅(1.5⋅10^11)^2)/(5.67⋅10^(-8)⋅(7⋅10^8)^2)
≈1.13⋅10^15
T≈5800K
Photoelectric Effect
E=h⋅ƒ=(h⋅c)/λ
(KE_max)=e⋅(V_s)
(KE_max)=E-(W_s)
(W_s)=h⋅(ƒ_s)=(h⋅c)/(λ_s)
E is energy from photon, joule or eV
h is 6.62⋅10^(-34)
ƒ is light frequency
(KE_max) is maximum kinetic energy
e is 1.6⋅10^(-19)
(V_s) is stopping potential
(W_s) is work function / energi ambang
(ƒ_s) is work frequency / frekuensi minimum / frekuensi ambang
c is the speed of light
1 eV is 1.6⋅10^(-19) joule
Highlighted Problems
Problem 1
(ƒ_s)=2.30eV
2.30⋅1.6⋅10^(-19)=(6.62⋅10^(-34)⋅3⋅10^8)/(λ_s)
(λ_s)≈5.39⋅10^(-7) (a)
E=(6.62⋅10^(-34)⋅3⋅10^8)/(150⋅10^(-9))=1.324⋅10^(-18)
(KE_max)=1.324⋅10^(-18)-2.30⋅1.6⋅10^(-19)=9.56⋅10^(-19) (joules) (b)
9.56⋅10^(-19)=1.6⋅10^(-19)⋅(V_s)
(V_s)=5.975volt (c)
Problem 2
(W_s)=1.6eV=2.56⋅10^(-19) (a)
2.56⋅10^(-19)=(6.6⋅10^(-34)⋅3⋅10^8)/(λ_s)
(λ_s)=7.73⋅10^(-7)=773nm (b)
(0.4⋅1.6⋅10^(-19))+(2.56⋅10^(-19))=6.6⋅10^(-34)⋅ƒ
ƒ=4.84⋅10^14 (c)
Compton Effect
Photons scatter off electrons.
Δ(λ)=(λ^′)-λ=h/(m⋅c)⋅(1-cos(θ))
E=(h⋅c)/λ
(E_k)=E-(E^′)
At this point the symbols should be obvious, but here they are.
Δ(λ) is change in wavelength
h is 6.6⋅10^(-34)
c is the speed of light
m is mass of an electron, 9.1⋅10^(-31)
λ and (λ^′) are the wavelengths before and after scattering
θ is the angle of scattering
E is an energy of a photon
(E_k) is the amount of kinetic energy given to the electron
Highlighted Problems
Problem 1
λ=3.5⋅10^(-2)⋅10^(-9)=3.5⋅10^(-11)
cos(37°)≈4/5
Δ(λ)=(6.6⋅10^(-34))/(9.1⋅10^(-31)⋅3⋅10^8)⋅(1-4/5)=4.83⋅10^(-13)
(λ^′)=4.83⋅10^(-13)+3.5⋅10^(-11)=3.54⋅10^(-11)=0.0354nm (a)
(E^′)=(3⋅10^8⋅6.6⋅10^(-34))/(3.54⋅10^(-11))=5.59⋅10^(-15) (b)
E=(3⋅10^8⋅6.6⋅10^(-34))/(3.5⋅10^(-11))=5.65⋅10^(-15)
(E_k)=5.65⋅10^(-15)-5.59⋅10^(-15)=0.06⋅10^(-15) (c)
Problem 2
λ=1.000⋅10^(-10)
Δ(λ)=(6.6⋅10^(-34))/(9.1⋅10^(-31)⋅3⋅10^8)⋅1=2.41⋅10^(-12)=0.00241nm (a)
(λ^′)=1⋅10^(-10)+2.41⋅10^(-12)=1.024⋅10^(-10)
(E_k)=3⋅10^8⋅6.6⋅10^(-34)⋅(1/(1.000⋅10^(-10))-1/(1.024⋅10^(-18)))
=4.640⋅10^(-17)
4.64⋅10^(-17)=(m⋅v^2)/2
=1/2⋅9.1⋅10^(-31)⋅v^2
v=10099096=1.0099096⋅10^7