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Part A – Explanation of forces on FBD
| Step | Derivation/Formula | Reasoning |
|---|---|---|
| a) | \(B\) | This is the buoyant force acting upward on the balloon, equal to the weight of the displaced air. |
| a) | \(W_{\text{balloon}} = (0.0050\,\text{kg})\,g\) | This is the weight of the balloon (including helium) acting downward. |
| a) | \(T\) | This is the tension in the string, which transmits the downward pull from the attached \(0.015\,\text{kg}\) object. (Only the balloon is considered here so its forces include the upward buoyant force and the two downward forces: its own weight and the tension from the string.) |
Part B – Buoyant force on the balloon
| Step | Derivation/Formula | Reasoning |
|---|---|---|
| b) 1 | \(B = W_{\text{balloon}} + W_{\text{object}} = (0.0050\,\text{kg} + 0.015\,\text{kg})\,g = 0.0200\,g\) | The balloon is just prevented from rising, so its upward buoyant force exactly balances the combined weight of the balloon and the attached object. (The buoyant force on the object is negligible.) |
| b) 2 | \(B = 0.0200 \times 9.8 \; (\text{m/s}^2) = \boxed{0.196\,\text{N}}\) | Substitute \(g \approx 9.8\,\text{m/s}^2\) to calculate the buoyant force in newtons. |
Part C – Volume of the balloon
| Step | Derivation/Formula | Reasoning |
|---|---|---|
| c) 1 | \(B = \rho_{\text{air}} \; g \; V\) | This is Archimedes’ principle stating that the buoyant force is equal to the weight of the displaced air. Here \(\rho_{\text{air}} = 1.29\,\text{kg/m}^3\), and \(g = 9.8\,\text{m/s}^2\). |
| c) 2 | \(V = \displaystyle \frac{B}{\rho_{\text{air}} \; g} = \frac{0.196}{1.29 \times 9.8}\) | Rearrange the equation to solve for the volume \(V\) of the balloon. |
| c) 3 | \(V \approx \frac{0.196}{12.642} \approx \boxed{0.0155\,\text{m}^3}\) | Calculate the denominator (\(1.29 \times 9.8 \approx 12.642\)) and then evaluate \(V\). The volume of the balloon is approximately \(0.0155\,\text{m}^3\). |
Part D – Position of ballon in the car
| Step | Derivation/Formula | Reasoning |
|---|---|---|
| d) 1 | Effective gravity: \(\vec{g}_{\text{eff}} = \vec{g} – \vec{a}\) | When the car accelerates forward with acceleration \(a\), the effective gravitational field in the car’s frame tilts backward. This is a standard result for non-inertial frames. |
| d) 2 | For a mass not affected by buoyancy, the equilibrium direction of the string makes an angle \(\theta\) where \(\tan(\theta)=\frac{a}{g}\). | The heavy \(0.015\,\text{kg}\) object behaves as a normal pendulum, aligning along the effective gravitational field. This causes it to deflect opposite to the car’s acceleration (i.e., towards the rear of the car). |
| d) 3 | Result: The \(0.015\,\text{kg}\) object \(\rightarrow\) moves backward relative to the car. | Thus, when the car accelerates forward, the object swings toward the back of the car, while the buoyant balloon (not shown here) would deflect forward. Since the child holds the string midway, the object is pulled into its equilibrium position defined by \(\vec{g}_{\text{eff}}\). |
Just ask: "Help me solve this problem."
Three identical reservoirs, \(A\), \(B\), and \(C\), are represented above, each with a small pipe where water exits horizontally. The pipes are set at the same height above a pool of water. The water in the reservoirs is kept at the levels shown. Which of the following correctly ranks the horizontal distances \( d \) that the streams of water travel before hitting the surface of the pool?
A solid plastic cube with uniform density (side length = \(0.5\) \(\text{m}\)) of mass \(100\) \(\text{kg}\) is placed in a vat of fluid whose density is \(1200\) \(\text{kg/m}^3\). What fraction of the cube’s volume floats above the surface of the fluid?
A drinking fountain projects water at an initial angle of \( 50^ \circ \) above the horizontal, and the water reaches a maximum height of \( 0.150 \) \( \text{m} \) above the point of exit. Assume air resistance is negligible.
A sample of an unknown material appears to weigh \( 285 \) \( \text{N} \) in air and \( 195 \) \( \text{N} \) when immersed in alcohol of specific gravity \( 0.700 \).
A horizontal tube with two vertical T-branches (A and B) is partially submerged in a liquid, with the open ends of the branches exposed to the air. However, the section of the tube above point B is hidden from view and may either be wider or narrower than the section above A.
Air is blown through the horizontal tube, causing the liquid levels in the vertical branches to rise as shown. Based on the observed water levels, which of the following best describes the characteristics of the hidden section of the tube above B?
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| Kinematics | Forces |
|---|---|
| \(\Delta x = v_i t + \frac{1}{2} at^2\) | \(F = ma\) |
| \(v = v_i + at\) | \(F_g = \frac{G m_1 m_2}{r^2}\) |
| \(v^2 = v_i^2 + 2a \Delta x\) | \(f = \mu N\) |
| \(\Delta x = \frac{v_i + v}{2} t\) | \(F_s =-kx\) |
| \(v^2 = v_f^2 \,-\, 2a \Delta x\) |
| Circular Motion | Energy |
|---|---|
| \(F_c = \frac{mv^2}{r}\) | \(KE = \frac{1}{2} mv^2\) |
| \(a_c = \frac{v^2}{r}\) | \(PE = mgh\) |
| \(T = 2\pi \sqrt{\frac{r}{g}}\) | \(KE_i + PE_i = KE_f + PE_f\) |
| \(W = Fd \cos\theta\) |
| Momentum | Torque 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 Motion | Fluids |
|---|---|
| \(F = -kx\) | \(P = \frac{F}{A}\) |
| \(T = 2\pi \sqrt{\frac{l}{g}}\) | \(P_{\text{total}} = P_{\text{atm}} + \rho gh\) |
| \(T = 2\pi \sqrt{\frac{m}{k}}\) | \(Q = Av\) |
| \(x(t) = A \cos(\omega t + \phi)\) | \(F_b = \rho V g\) |
| \(a = -\omega^2 x\) | \(A_1v_1 = A_2v_2\) |
| Constant | Description |
|---|---|
| [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 |
| Variable | SI 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] |
| Variable | Derived 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] |
General Metric Conversion Chart
Example of using unit analysis: Convert 5 kilometers to millimeters.
Start with the given measurement: [katex]\text{5 km}[/katex]
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]
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]
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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