| Derivation or Formula | Reasoning |
|---|---|
| \[U_g(x)=mg(-x)\tan\theta_0 \quad ( -D\le x\le 0)\] | Height above the horizontal surface is \((-x)\tan\theta_0\); choose zero gravitational energy at the base (\(x=0\)). Thus the potential energy on the ramp varies linearly with the horizontal coordinate. |
| \[K(x)=mgD\tan\theta_0-mg(-x)\tan\theta_0=mg\tan\theta_0(D+x) \quad ( -D\le x\le 0)\] | Mechanical energy is conserved on the friction-free ramp, so kinetic energy equals the difference between the initial potential energy \(mgD\tan\theta_0\) and the remaining potential energy \(U_g(x)\). |
| \[U_g(x)=0 \quad (0\le x\le 4D)\] | On the horizontal surface the height is zero; gravitational potential energy remains constant at the chosen zero reference. |
| \[K(x)=mgD\tan\theta_0-\mu_k mg\,x \quad (0\le x\le 4D)\] | Friction does work \(W_f=-\mu_k mg\,x\). Kinetic energy therefore decreases linearly from its value at the base to zero at \(x=4D\). |
| Derivation or Formula | Reasoning |
|---|---|
| \[\text{–}\] | Correct aspects: Doubling the ramp height doubles both the gravitational potential energy at the top and the kinetic energy at the base, so a greater distance is expected on the rough surface. The prediction of a final position at \(x=8D\) is therefore consistent.
Incorrect aspects: none. |
| Derivation or Formula | Reasoning |
|---|---|
| \[h=D\tan\theta_0\] | Initial ramp height in the first situation, expressed with base length \(D\). |
| \[mg h = \mu_k mg(4D)\] | Work–energy theorem: kinetic energy at the base equals the work done by friction over \(4D\), allowing \(\mu_k\) to be related to \(\theta_0\). |
| \[\mu_k = \frac{\tan\theta_0}{4}\] | Solve the previous relationship for \(\mu_k\). |
| \[h’ = 2D\tan\theta_0\] | The new ramp is twice as long horizontally, so its height is doubled. |
| \[mg h’ = \mu_k mg\,x_f\] | Set the new kinetic energy at the base equal to the work done by friction over the unknown stopping distance \(x_f\). |
| \[x_f = \frac{2D\tan\theta_0}{\mu_k} = \frac{2D\tan\theta_0}{\tan\theta_0/4}=8D\] | Substitute \(\mu_k\) from above to obtain the new final position. |
| \[\boxed{x_f = 8D}\] | Final algebraic result: the block stops at \(x=8D\) relative to the base of the ramp. |
| Derivation or Formula | Reasoning |
|---|---|
| \[K_{\text{base}}\propto h\] | The equations show that kinetic energy at the base is directly proportional to the ramp height; doubling \(h\) indeed doubles \(K_{\text{base}}\), validating that part of the student’s claim. |
| \[x_f = \frac{K_{\text{base}}}{\mu_k mg}\] | Since the friction force is unchanged, the stopping distance is proportional to \(K_{\text{base}}\). Because \(K_{\text{base}}\) doubles, the horizontal distance also doubles, fully supporting the student’s predicted position \(x=8D\). |
| \[\text{–}\] | No steps contradict the student’s logic, so there are no incorrect aspects to correct. |
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A uniform solid cylinder of mass \( M \) and radius \( R \) is initially at rest on a frictionless horizontal surface. A massless string is attached to the cylinder and is wrapped around it. The string is then pulled with a constant force \( F \) , causing the cylinder to rotate about its center of mass. After the cylinder has rotated through an angle \( \theta \), what is the kinetic energy of the cylinder in terms of \( F \) and \( \theta \)?
A projectile of mass 0.750 kg is shot straight up with an initial speed of 18.0 m/s.

Refer to the diagram above and solve all equations in terms of \(R\), \(M\), \(k\), and constants.
A box having a mass of \( 1.5 \) \( \text{kg} \) is accelerated across a table at \( 1.5 \) \( \text{m/s}^2 \). The coefficient of kinetic friction on the box is \( 0.3 \).
In which one of the following circumstances does the principle of conservation of mechanical energy apply, even though a nonconservative force acts on the moving object?
A 75.0kg log floats downstream with a speed of 1.80 m/s. Eight frogs hop onto the log in a series of perfectly inelastic collisions. If each frog has a mass of 0.30 kg and an upstream speed of 1.3 m/s, what is the change in kinetic energy for this system?

Using only work and energy, find the velocity of the masses after they have traveled \(0.8 \, \text{m}\). Refer to the image above.
According to Newton’s third law, each team in a tug of war pulls with equal force on the other team. What, then, determines which team will win?
A block of mass \( m \) is moving on a horizontal frictionless surface with a speed \( v_0 \) as it approaches a block of mass \( 2m \) which is at rest and has an ideal spring attached to one side.
When the two blocks collide, the spring is completely compressed and the two blocks momentarily move at the same speed, and then separate again, each continuing to move.
Two masses \(m_1\) and \(4m_1\) are on an incline. Both surfaces have the same coefficient of kinetic friction. Both objects start from rest at the same height. Which mass has the largest speed at the bottom?
\(x_f=8D\)
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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] |
Metric Prefixes
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] | 0.000000000001 |
Nano- | n | [katex]10^{-9}[/katex] | 0.000000001 |
Micro- | µ | [katex]10^{-6}[/katex] | 0.000001 |
Milli- | m | [katex]10^{-3}[/katex] | 0.001 |
Centi- | c | [katex]10^{-2}[/katex] | 0.01 |
Deci- | d | [katex]10^{-1}[/katex] | 0.1 |
(Base unit) | – | [katex]10^{0}[/katex] | 1 |
Deca- or Deka- | da | [katex]10^{1}[/katex] | 10 |
Hecto- | h | [katex]10^{2}[/katex] | 100 |
Kilo- | k | [katex]10^{3}[/katex] | 1,000 |
Mega- | M | [katex]10^{6}[/katex] | 1,000,000 |
Giga- | G | [katex]10^{9}[/katex] | 1,000,000,000 |
Tera- | T | [katex]10^{12}[/katex] | 1,000,000,000,000 |
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