AP Physics

Unit 1 - Vectors and Kinematics

MCQ
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Step Reasoning
Relate the flux through the open hemispherical surface to the flux through the flat circular disk using Gauss’s law.
\[\Phi_{\text{hemisphere}} = \Phi_{\text{disk}} = \int \vec{E} \cdot d\vec{A}\]
The hemisphere and the disk together form a closed surface enclosing zero net charge. Therefore, the net electric flux through the closed surface is zero, meaning the magnitude of the flux through the open hemisphere equals the flux through the flat disk.
Set up the surface integral for the flux through the flat disk in polar coordinates.
\[\Phi_E = \int_0^R E \cos\theta (2\pi r \, dr) = \int_0^R \dfrac{q}{4\pi\varepsilon_0 (r^2 + d^2)} \left(\dfrac{d}{\sqrt{r^2 + d^2}}\right) (2\pi r \, dr)\]
At a distance \(r\) from the center of the disk, the electric field from the point charge \(q\) has magnitude \(E = \dfrac{q}{4\pi\varepsilon_0 (r^2 + d^2)}\) and the angle with the normal to the disk satisfies \(\cos\theta = \dfrac{d}{\sqrt{r^2 + d^2}}\).
Evaluate the integral to derive the final expression for electric flux.
\[\Phi_E = \dfrac{q d}{2\varepsilon_0} \int_0^R \dfrac{r}{(r^2 + d^2)^{3/2}} \, dr = \dfrac{q d}{2\varepsilon_0} \left[ -\dfrac{1}{\sqrt{r^2 + d^2}} \right]_0^R = \dfrac{q}{2\varepsilon_0} \left(1 – \dfrac{d}{\sqrt{R^2 + d^2}}\right)\]
Performing the single substitution \(u = r^2 + d^2\) yields the integrated flux value.

Why each choice is correct or incorrect:

(A) Omits the factor of \(2\) in the denominator by using \(4\pi\) from the full-sphere equation without accounting for the factor of \(2\pi\) from polar area integration.

(B) Uses \(\cos\theta\) directly instead of \(1 – \cos\theta\), which calculates the fraction corresponding to the complementary exterior cone rather than the disk’s subtended angle.

(C) This is the correct answer. Gauss’s law equates the flux through the open surface to the flux through the bounding disk, evaluating to \(\dfrac{q}{2\varepsilon_0}\left(1 – \dfrac{d}{\sqrt{R^2 + d^2}}\right)\).

(D) Omits the square root when writing \(\cos\theta = \dfrac{d}{\sqrt{R^2 + d^2}}\), leaving an unphysical squared ratio.

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KinematicsForces
\(\Delta x = v_i t + \frac{1}{2} at^2\)\(F = ma\)
\(v = v_i + at\)\(F_g = \frac{G m_1 m_2}{r^2}\)
\(v^2 = v_i^2 + 2a \Delta x\)\(f = \mu N\)
\(\Delta x = \frac{v_i + v}{2} t\)\(F_s =-kx\)
\(v^2 = v_f^2 \,-\, 2a \Delta x\) 
Circular MotionEnergy
\(F_c = \frac{mv^2}{r}\)\(KE = \frac{1}{2} mv^2\)
\(a_c = \frac{v^2}{r}\)\(PE = mgh\)
\(T = 2\pi \sqrt{\frac{r}{g}}\)\(KE_i + PE_i = KE_f + PE_f\)
 \(W = Fd \cos\theta\)
MomentumTorque and Rotations
\(p = mv\)\(\tau = r \cdot F \cdot \sin(\theta)\)
\(J = \Delta p\)\(I = \sum mr^2\)
\(p_i = p_f\)\(L = I \cdot \omega\)
Simple Harmonic MotionFluids
\(F = -kx\)\(P = \frac{F}{A}\)
\(T = 2\pi \sqrt{\frac{l}{g}}\)\(P_{\text{total}} = P_{\text{atm}} + \rho gh\)
\(T = 2\pi \sqrt{\frac{m}{k}}\)\(Q = Av\)
\(x(t) = A \cos(\omega t + \phi)\)\(F_b = \rho V g\)
\(a = -\omega^2 x\)\(A_1v_1 = A_2v_2\)
ConstantDescription
[katex]g[/katex]Acceleration due to gravity, typically [katex]9.8 , \text{m/s}^2[/katex] on Earth’s surface
[katex]G[/katex]Universal Gravitational Constant, [katex]6.674 \times 10^{-11} , \text{N} \cdot \text{m}^2/\text{kg}^2[/katex]
[katex]\mu_k[/katex] and [katex]\mu_s[/katex]Coefficients of kinetic ([katex]\mu_k[/katex]) and static ([katex]\mu_s[/katex]) friction, dimensionless. Static friction ([katex]\mu_s[/katex]) is usually greater than kinetic friction ([katex]\mu_k[/katex]) as it resists the start of motion.
[katex]k[/katex]Spring constant, in [katex]\text{N/m}[/katex]
[katex] M_E = 5.972 \times 10^{24} , \text{kg} [/katex]Mass of the Earth
[katex] M_M = 7.348 \times 10^{22} , \text{kg} [/katex]Mass of the Moon
[katex] M_M = 1.989 \times 10^{30} , \text{kg} [/katex]Mass of the Sun
VariableSI Unit
[katex]s[/katex] (Displacement)[katex]\text{meters (m)}[/katex]
[katex]v[/katex] (Velocity)[katex]\text{meters per second (m/s)}[/katex]
[katex]a[/katex] (Acceleration)[katex]\text{meters per second squared (m/s}^2\text{)}[/katex]
[katex]t[/katex] (Time)[katex]\text{seconds (s)}[/katex]
[katex]m[/katex] (Mass)[katex]\text{kilograms (kg)}[/katex]
VariableDerived SI Unit
[katex]F[/katex] (Force)[katex]\text{newtons (N)}[/katex]
[katex]E[/katex], [katex]PE[/katex], [katex]KE[/katex] (Energy, Potential Energy, Kinetic Energy)[katex]\text{joules (J)}[/katex]
[katex]P[/katex] (Power)[katex]\text{watts (W)}[/katex]
[katex]p[/katex] (Momentum)[katex]\text{kilogram meters per second (kgm/s)}[/katex]
[katex]\omega[/katex] (Angular Velocity)[katex]\text{radians per second (rad/s)}[/katex]
[katex]\tau[/katex] (Torque)[katex]\text{newton meters (Nm)}[/katex]
[katex]I[/katex] (Moment of Inertia)[katex]\text{kilogram meter squared (kgm}^2\text{)}[/katex]
[katex]f[/katex] (Frequency)[katex]\text{hertz (Hz)}[/katex]

Metric Prefixes

Example of using unit analysis: Convert 5 kilometers to millimeters. 

  1. Start with the given measurement: [katex]\text{5 km}[/katex]

  2. Use the conversion factors for kilometers to meters and meters to millimeters: [katex]\text{5 km} \times \frac{10^3 \, \text{m}}{1 \, \text{km}} \times \frac{10^3 \, \text{mm}}{1 \, \text{m}}[/katex]

  3. Perform the multiplication: [katex]\text{5 km} \times \frac{10^3 \, \text{m}}{1 \, \text{km}} \times \frac{10^3 \, \text{mm}}{1 \, \text{m}} = 5 \times 10^3 \times 10^3 \, \text{mm}[/katex]

  4. Simplify to get the final answer: [katex]\boxed{5 \times 10^6 \, \text{mm}}[/katex]

Prefix

Symbol

Power of Ten

Equivalent

Pico-

p

[katex]10^{-12}[/katex]

Nano-

n

[katex]10^{-9}[/katex]

Micro-

µ

[katex]10^{-6}[/katex]

Milli-

m

[katex]10^{-3}[/katex]

Centi-

c

[katex]10^{-2}[/katex]

Deci-

d

[katex]10^{-1}[/katex]

(Base unit)

[katex]10^{0}[/katex]

Deca- or Deka-

da

[katex]10^{1}[/katex]

Hecto-

h

[katex]10^{2}[/katex]

Kilo-

k

[katex]10^{3}[/katex]

Mega-

M

[katex]10^{6}[/katex]

Giga-

G

[katex]10^{9}[/katex]

Tera-

T

[katex]10^{12}[/katex]

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