Energy and Conservation | IB - Wyatt's Notes

Forms of Energy

Energy is a scalar quantity measured in joules ($\mathrm J$). It exists in many forms and can be Transformed from one form to another, but the total energy in a closed system is conserved.

Form	Description
Kinetic	Energy of motion
Gravitational potential	Energy due to position in a gravitational field
Elastic potential	Energy stored in a deformed object
Thermal	Energy associated with temperature
Chemical	Energy stored in chemical bonds
Nuclear	Energy stored in atomic nuclei
Electrical	Energy of moving charges
Radiant (electromagnetic)	Energy of electromagnetic waves

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Kinetic Energy

Translational Kinetic Energy

For an object of mass $m$ moving with speed $v$:

$$E_k = \frac\{1\}\{2\}mv^2$$

Key Points

• Kinetic energy is always non-negative ($E_k \ge 0$).
• on speed squared, so doubling speed quadruples kinetic energy.
• It is a scalar (no direction).

Work-Energy Theorem

The net work done on an object equals the change in its kinetic energy:

$$W_\{\mathrm\{net\}\} = \Delta E_k = \frac\{1\}\{2\}mv_f^2 - \frac\{1\}\{2\}mv_i^2$$

:::note Example A $1500\mathrm{ kg}$ car travelling at $20\mathrm{ m/s}$ brakes to a stop. Find the work done by the Brakes.

$$W = \Delta E_k = 0 - \frac\{1\}\{2\}(1500)(400) = -300000\mathrm\{ J\} = -300\mathrm\{ kJ\}$$

The negative sign indicates the brakes do negative work (remove energy from the car).

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Gravitational Potential Energy

Near Earth’s Surface

For small height changes (where $g$ is approximately constant):

$$E_p = mgh$$

Where $h$ is the height above a chosen reference level (datum).

Universal Gravitational Potential Energy

For any two masses separated by distance $r$:

E_p = -\frac`\{GMm}`\{r\}

Where $G = 6.674 \times 10^{-11}\mathrm{ N}\cdot\mathrm m^2/\mathrm{kg}^2$.

Key Differences

Property	Near Surface ($mgh$)	Universal ($-GMm/r$)
Reference level	Arbitrary ( ground)	Zero at infinity
Sign	Positive above reference	Negative (bound state)
Validity	$h \ll R_{\mathrm{Earth}}$	Any distance
Gradient	$-\dfrac{dE_p}{dh} = -mg$	$-\dfrac{dE_p}{dr} = -\dfrac{GMm}{r^2}$
:::
:::note
Example
Find the gravitational potential energy of a $70\mathrm{ kg}$ person at the top of a $50\mathrm{ m}$
Building (using $mgh$).

$$E_p = 70 \times 9.81 \times 50 = 34335\mathrm\{ J\} \approx 34.3\mathrm\{ kJ\}$$

::: :::note Example A satellite of mass $500\mathrm{ kg}$ orbits at a height of $300\mathrm{ km}$ above Earth’s surface. Find its gravitational potential energy. ($M_E = 5.97 \times 10^{24}\mathrm{ kg}$ $R_E = 6.37 \times 10^6\mathrm{ m}$)

$$R = 6.37 \times 10^6 + 3.0 \times 10^5 = 6.67 \times 10^6\mathrm\{ m\}$$ $$E_p = -\frac\{6.674 \times 10^\{-11\} \times 5.97 \times 10^\{24\} \times 500\}\{6.67 \times 10^6\}$$ $$= -\frac\{1.992 \times 10^\{17\}\}\{6.67 \times 10^6\} = -2.987 \times 10^\{10\}\mathrm\{ J\}$$

Escape Velocity

The minimum speed needed to escape a gravitational field:

$$V_\{\mathrm\{esc\}\} = \sqrt\{\frac\{2GM\}\{r\}\}$$

For Earth: $v_{\mathrm{esc}} \approx 11200\mathrm{ m/s} \approx 11.2\mathrm{ km/s}$.

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Elastic Potential Energy

Hooke’s Law

For a spring obeying Hooke’s law (within the elastic limit):

$$F = -kx$$

Where $k$ is the spring constant (stiffness) and $x$ is the displacement from equilibrium.

Elastic Potential Energy

$$E_e = \frac\{1\}\{2\}kx^2$$

This is also the work done in compressing or extending the spring by $x$:

$$W = \int_0^x kx'\,dx' = \frac\{1\}\{2\}kx^2$$

::: :::note Example A spring with $k = 200\mathrm{ N/m}$ is compressed by $0.1\mathrm{ m}$. Find the elastic potential Energy stored.

$$E_e = \frac\{1\}\{2\}(200)(0.01) = 1.0\mathrm\{ J\}$$

Force-Extension Graphs

For a spring obeying Hooke’s law, the force-extension graph is a straight line through the origin. The area under the graph equals the elastic potential energy.

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Conservation of Mechanical Energy

Observe how kinetic energy and gravitational potential energy interchange as a skater moves along a Track. Try changing the skater’s mass and the track shape to see how energy is conserved.

Principle

In a system with only conservative forces (gravity, elastic forces), the total mechanical energy is Conserved:

$$E_k + E_p + E_e = \mathrm\{constant\}$$ $$\frac\{1\}\{2\}mv_1^2 + mgh_1 + \frac\{1\}\{2\}kx_1^2 = \frac\{1\}\{2\}mv_2^2 + mgh_2 + \frac\{1\}\{2\}kx_2^2$$

Conservative vs Non-Conservative Forces

Conservative Forces	Non-Conservative Forces
Gravity	Friction
Elastic (spring)	Air resistance
Electrostatic	Applied pushes/pulls
Work is path-independent	Work is path-dependent

Applications

::: :::note Example A $2\mathrm{ kg}$ ball is dropped from a height of $10\mathrm{ m}$. Find its speed just before it Hits the ground (ignoring air resistance).

$$E_k(\mathrm\{top\}) + E_p(\mathrm\{top\}) = E_k(\mathrm\{bottom\}) + E_p(\mathrm\{bottom\})$$ $$0 + 2(9.81)(10) = \frac\{1\}\{2\}(2)v^2 + 0$$ $$196.2 = v^2$$ $$V = 14.0\mathrm\{ m/s\}$$

::: :::note Example A pendulum of length $1.5\mathrm{ m}$ is released from horizontal. Find its speed at the lowest Point.

Taking the lowest point as reference ($E_p = 0$):

$$E_p(\mathrm\{top\}) = mgL = m(9.81)(1.5)$$ $$E_k(\mathrm\{bottom\}) = \frac\{1\}\{2\}mv^2$$

By conservation: $mgL = \dfrac{1}{2}mv^2$.

$$V = \sqrt\{2gL\} = \sqrt\{2(9.81)(1.5)\} = \sqrt\{29.43\} = 5.42\mathrm\{ m/s\}$$

::: :::note Example A block of mass $0.5\mathrm{ kg}$ slides from rest down a frictionless curved ramp of height $3\mathrm{ m}$ onto a horizontal surface with friction ($\mu_k = 0.4$). How far does it slide before Stopping?

At the bottom of the ramp, all $E_p$ converts to $E_k$:

$$\frac\{1\}\{2\}(0.5)v^2 = 0.5(9.81)(3) \implies v^2 = 58.86 \implies v = 7.67\mathrm\{ m/s\}$$

Friction does work to stop the block:

$$\mu_k mg \cdot d = \frac\{1\}\{2\}mv^2$$ $$0.4(0.5)(9.81)d = \frac\{1\}\{2\}(0.5)(58.86)$$ $$1.962d = 14.72 \implies d = 7.50\mathrm\{ m\}$$

Alternatively, using energy directly: $mgh = \mu_k mg d \implies d = \dfrac{h}{\mu_k} = \dfrac{3}{0.4} = 7.5\mathrm{ m}$.

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Work Done by Non-Conservative Forces

When non-conservative forces (like friction) are present:

$$W_\{\mathrm\{nc\}\} = \Delta E_k + \Delta E_p$$

Or equivalently:

$$E_\{k,i\} + E_\{p,i\} + W_\{\mathrm\{nc\}\} = E_\{k,f\} + E_\{p,f\}$$

Where $W_{\mathrm{nc}}$ is the work done by non-conservative forces (negative for friction). ::: :::note Example A $3\mathrm{ kg}$ block slides down a $5\mathrm{ m}$ ramp inclined at $30\degree$ with $\mu_k = 0.2$. Find the speed at the bottom if it starts from rest.

$$Mgh - \mu_k mg\cos\theta \cdot d = \frac\{1\}\{2\}mv^2$$ $$3(9.81)(5\sin 30\degree) - 0.2(3)(9.81)\cos 30\degree \times \frac\{5\}\{\sin 30\degree\} = \frac\{1\}\{2\}(3)v^2$$

Wait, $d = \dfrac{h}{\sin\theta} = \dfrac{5\sin 30\degree}{\sin 30\degree} = 5\mathrm{ m}$ (since $h = 5\sin 30\degree = 2.5\mathrm{ m}$).

$$3(9.81)(2.5) - 0.2(3)(9.81)(0.866)(10) = \frac\{1\}\{2\}(3)v^2$$ $$73.58 - 50.97 = 1.5v^2$$ $$22.61 = 1.5v^2 \implies v = 3.88\mathrm\{ m/s\}$$

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Power

Definition

Power is the rate at which work is done or energy is transferred:

$$P = \frac\{W\}\{t\} = \frac\{\Delta E\}\{t\}$$

For a constant force:

$$P = Fv$$

Units

• SI unit: watt ($\mathrm W$), where $1\mathrm{ W} = 1\mathrm{ J/s}$.
• Other units: kilowatt ($1\mathrm{ kW} = 1000\mathrm{ W}$), horsepower ($1\mathrm{ hp} \approx 746\mathrm{ W}$).

Power and Inclined Planes

For an object moving up an incline at constant speed $v$:

$$P = Fv = (mg\sin\theta + f)v$$

Power and Vehicles

For a car on a level road at maximum speed (driving force equals drag):

$$P = Fv = f_\{\mathrm\{drag\}\} \cdot v$$

Since drag increases with speed, there is a maximum speed where $P = f_{\mathrm{drag}} \cdot v_{\max}$. ::: :::note Example A car engine produces $80\mathrm{ kW}$ of power. The total resistive force is $800\mathrm{ N}$ at The car’s maximum speed. Find the maximum speed.

$$P = Fv \implies 80000 = 800v \implies v = 100\mathrm\{ m/s\}$$

This is $360\mathrm{ km/h}$Which is unrealistic for a car with $80\mathrm{ kW}$ — in practice, Drag increases with $v^2$ so the maximum speed would be lower.

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Efficiency of Energy Transfers

Definition

\mathrm\{Efficiency\} = \frac\{\mathrm\{useful energy output\}\}\{\mathrm\{total energy input\}\} \times 100\%

Energy Degradation

In all real energy transfers, some energy is dissipated ( as thermal energy due to friction). This means:

• Efficiency is always less than 100%.
• Total energy is always conserved, but useful energy decreases.
• The “lost” energy is not destroyed — it is transferred to the surroundings as heat.

Sankey Diagrams

Sankey diagrams visually represent energy flows:

• The width of each arrow is proportional to the amount of energy.
• The input energy splits into useful output and wasted energy. ::: :::note Example A light bulb converts $100\mathrm{ J}$ of electrical energy into $10\mathrm{ J}$ of light energy and $90\mathrm{ J}$ of thermal energy per second.

$$\mathrm\{Efficiency\} = \frac\{10\}\{100\} \times 100\% = 10\%$$

Power input $= 100\mathrm{ W}$Useful power output $= 10\mathrm{ W}$.

Common Efficiencies

Device	Typical Efficiency
Incandescent light bulb	5—10%
LED light bulb	30—40%
Electric motor	70—95%
Car engine (petrol)	20—30%
Diesel engine	30—40%
Steam turbine	35—45%
Solar cell	15—25%
Human body	20—25%

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Energy in Simple Harmonic Motion

Total Energy in SHM

In simple harmonic motion, energy continuously converts between kinetic and potential:

$$E_\{\mathrm\{total\}\} = E_k + E_p = \frac\{1\}\{2\}kA^2 = \frac\{1\}\{2\}m\omega^2 A^2$$

Where $A$ is the amplitude.

Energy as a Function of Position

$$E_k(x) = \frac\{1\}\{2\}k(A^2 - x^2)$$ $$E_p(x) = \frac\{1\}\{2\}kx^2$$

Energy as a Function of Time

$$E_k(t) = \frac\{1\}\{2\}kA^2\cos^2(\omega t)$$ $$E_p(t) = \frac\{1\}\{2\}kA^2\sin^2(\omega t)$$

The total energy remains constant at all times.

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IB Exam-Style Questions

Question 1 (Paper 1 style)

A roller coaster car of mass $500\mathrm{ kg}$ starts from rest at point A which is $30\mathrm{ m}$ above the ground. It travels along the track to point B which is $10\mathrm{ m}$ Above the ground. Neglecting friction, find its speed at B.

$$Mgh_A = mgh_B + \frac\{1\}\{2\}mv_B^2$$ $$9.81(30) = 9.81(10) + \frac\{1\}\{2\}v_B^2$$ $$294.3 = 98.1 + 0.5v_B^2$$ $$V_B^2 = 392.4 \implies v_B = 19.8\mathrm\{ m/s\}$$

Question 2 (Paper 2 style)

A spring-loaded launcher has spring constant $k = 500\mathrm{ N/m}$ and is compressed by $0.15\mathrm{ m}$. It launches a $0.2\mathrm{ kg}$ ball vertically upward.

(a) Find the speed of the ball as it leaves the launcher.

$$\frac\{1\}\{2\}kx^2 = \frac\{1\}\{2\}mv^2$$ $$V = x\sqrt\{\frac\{k\}\{m\}\} = 0.15\sqrt\{\frac\{500\}\{0.2\}\} = 0.15\sqrt\{2500\} = 0.15 \times 50 = 7.5\mathrm\{ m/s\}$$

(b) Find the maximum height reached (from the launch point).

$$\frac\{1\}\{2\}mv^2 = mgh$$ $$H = \frac\{v^2\}\{2g\} = \frac\{56.25\}\{19.62\} = 2.87\mathrm\{ m\}$$

Question 3 (Paper 2 style)

A pump lifts $500\mathrm{ kg}$ of water per minute from a well $15\mathrm{ m}$ deep. The pump has an Efficiency of 65%. Find the power input to the pump.

P_\{\mathrm\{useful\}\} = \frac`\{mgh}`\{t\} = \frac\{500 \times 9.81 \times 15\}\{60\} = 1226\mathrm\{ W\} $$P_\{\mathrm\{input\}\} = \frac\{P_\{\mathrm\{useful\}\}\}\{\eta\} = \frac\{1226\}\{0.65\} = 1887\mathrm\{ W\} \approx 1.89\mathrm\{ kW\}$$

Question 4 (Paper 1 style)

A satellite of mass $200\mathrm{ kg}$ is in a circular orbit at altitude $500\mathrm{ km}$. ($M_E = 5.97 \times 10^{24}\mathrm{ kg}$, $R_E = 6.37 \times 10^6\mathrm{ m}$)

(a) Find the orbital speed.

$$R = 6.87 \times 10^6\mathrm\{ m\}$$ \frac`\{GMm}`\{r^2\} = \frac\{mv^2\}\{r\} \implies v = \sqrt\{\frac`\{GM}`\{r\}\} = \sqrt\{\frac\{6.674 \times 10^\{-11\} \times 5.97 \times 10^\{24\}\}\{6.87 \times 10^6\}\} $$V = \sqrt\{5.80 \times 10^7\} = 7616\mathrm\{ m/s\}$$

(b) Find the total mechanical energy.

E_\{\mathrm\{total\}\} = E_k + E_p = \frac\{1\}\{2\}mv^2 - \frac`\{GMm}`\{r\} = \frac\{1\}\{2\}m\frac`\{GM}`\{r\} - \frac`\{GMm}`\{r\} = -\frac`\{GMm}`\{2r\} $$E = -\frac\{6.674 \times 10^\{-11\} \times 5.97 \times 10^\{24\} \times 200\}\{2 \times 6.87 \times 10^6\}$$ $$= -\frac\{7.97 \times 10^\{16\}\}\{1.374 \times 10^7\} = -5.80 \times 10^9\mathrm\{ J\}$$

Question 5 (Paper 2 style)

A $60\mathrm{ kg}$ person jumps from a platform $5\mathrm{ m}$ above a trampoline. The trampoline Sags $0.5\mathrm{ m}$ at the lowest point. Find the spring constant of the trampoline.

At the lowest point, all energy is elastic potential energy:

$$Mg(h + x) = \frac\{1\}\{2\}kx^2$$ $$60(9.81)(5.5) = \frac\{1\}\{2\}k(0.25)$$ $$3237.3 = 0.125k \implies k = 25898\mathrm\{ N/m\} \approx 26000\mathrm\{ N/m\}$$

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Intuition

Energy is the universe’s currency, and conservation is its accounting principle. A ball sitting on a shelf has stored credit in gravitational potential energy; when it falls, that credit converts to kinetic energy at a rate determined by gravity. Friction is the taxman who always takes a cut, converting useful mechanical energy into thermal energy that dissipates into the surroundings. The work-energy theorem reveals that the net work done on an object is directly the deposit or withdrawal from its kinetic energy account. Power measures how quickly you spend energy, which is why a powerful engine can accelerate a car faster even though both engines ultimately convert the same amount of fuel.

flowchart TD
    A[3_Energyx] --> B[Key Concepts]
    A --> C[Core Principles]
    A --> D[Practical Applications]
    B --> E[Fundamental definitions]
    C --> F[Design patterns]
    D --> G[Real-world usage]

Summary

Energy Type	Formula
Kinetic	$E_k = \dfrac{1}{2}mv^2$
Gravitational PE (near surface)	$E_p = mgh$
Gravitational PE (universal)	$E_p = -\dfrac{GMm}{r}$
Elastic PE	$E_e = \dfrac{1}{2}kx^2$
Conservation	$E_k + E_p + E_e = \mathrm{constant}$
Work-energy theorem	$W_{\mathrm{net}} = \Delta E_k$
Power	$P = \dfrac{W}{t} = Fv$
Efficiency	$\eta = \dfrac{E_{\mathrm{out}}}{E_{\mathrm{in}}} \times 100\%$
:::
:::tip
Exam Strategy
For energy conservation problems, always define your reference level for gravitational PE. Show the
Energy at two chosen points ( start and end). When friction is present, subtract the Work done by
friction from the total mechanical energy.

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Energy in Gravitational Fields (Extended)

Gravitational Potential Energy Curves

For two masses $M$ and $m$ separated by distance $r$The total energy determines the type of orbit:

| Total Energy $E$ | Orbit Type | | ---------------- | ----------------------------- | --- | --- | --- | ------------------ | | $E \lt 0$ (and $| E | \lt | E_p |$) | Bound (elliptical) | | $E = 0$ | Parabolic (escape trajectory) | | | | | | $E \gt 0$ | Hyperbolic (unbound) | | | | |

For a circular orbit:

E_\{\mathrm\{total\}\} = E_k + E_p = \frac\{1\}\{2\}mv^2 - \frac`\{GMm}`\{r\} = \frac`\{GMm}`\{2r\} - \frac`\{GMm}`\{r\} = -\frac`\{GMm}`\{2r\}

Energy to Change Orbits

To move from one circular orbit to another, energy must be supplied. The minimum energy required is The difference in total orbital energies. ::: :::note Example Find the energy required to move a $1000\mathrm{ kg}$ satellite from a circular orbit at $300\mathrm{ km}$ altitude to one at $600\mathrm{ km}$ altitude.

($M_E = 5.97 \times 10^{24}\mathrm{ kg}$, $R_E = 6.37 \times 10^6\mathrm{ m}$)

$$R_1 = 6.67 \times 10^6\mathrm\{ m\}, \quad r_2 = 6.97 \times 10^6\mathrm\{ m\}$$ E_1 = -\frac`\{GMm}`\{2r_1\} = -\frac\{6.674 \times 10^\{-11\} \times 5.97 \times 10^\{24\} \times 1000\}\{2 \times 6.67 \times 10^6\} $$= -\frac\{3.985 \times 10^\{17\}\}\{1.334 \times 10^7\} = -2.988 \times 10^\{10\}\mathrm\{ J\}$$ E_2 = -\frac`\{GMm}`\{2r_2\} = -\frac\{3.985 \times 10^\{17\}\}\{1.394 \times 10^7\} = -2.858 \times 10^\{10\}\mathrm\{ J\} $$\Delta E = E_2 - E_1 = -2.858 \times 10^\{10\} - (-2.988 \times 10^\{10\}) = 1.30 \times 10^9\mathrm\{ J\}$$

The energy required is $1.30 \times 10^9\mathrm{ J}$ (about $1.30\mathrm{ GJ}$).

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Work Done by a Variable Force

When the force varies with position, the work done is the area under the force-displacement graph:

$$W = \int_\{x_1\}^\{x_2\} F(x)\,dx$$

::: :::note Example A spring obeys Hooke’s law: $F = -kx$. Find the work done in compressing the spring from $x = 0$ to $x = -d$.

$$W = \int_0^\{-d\} (-kx)\,dx = \left[-\frac\{kx^2\}\{2\}\right]_0^\{-d\} = -\frac\{k(-d)^2\}\{2\} = -\frac\{kd^2\}\{2\}$$

The negative sign indicates work is done on the spring (energy stored). The elastic potential energy Is $\dfrac{1}{2}kd^2$.

Force-Extension Graphs for Non-Hookean Materials

For materials that do not obey Hooke’s law, the area under the force-extension graph still equals The elastic potential energy, but it must be found by integration or by counting squares.

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Power in Rotational Systems

For rotational systems:

$$P = \tau\omega$$

Where $\tau$ is the torque and $\omega$ is the angular velocity. ::: :::note Example A motor delivers a torque of $50\mathrm{ N}\cdot\mathrm m$ at $3000\mathrm{ rpm}$. Find the power Output.

$$\omega = 3000 \times \frac\{2\pi\}\{60\} = 314.2\mathrm\{ rad/s\}$$ $$P = 50 \times 314.2 = 15708\mathrm\{ W\} \approx 15.7\mathrm\{ kW\}$$

:::

Energy Dissipation and Thermal Effects

Friction and Heat

When friction does work $W_f$The energy is converted to thermal energy:

$$Q = W_f = \mu_k Nd$$

Air Resistance

Air resistance converts kinetic energy to thermal energy:

$$\Delta E_k = W_\{\mathrm\{drag\}\} = \int F_\{\mathrm\{drag\}\}\,dx$$

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Additional IB Exam-Style Questions

Question 6 (Paper 2 style)

A $0.5\mathrm{ kg}$ ball is attached to a string of length $1.0\mathrm{ m}$ and swings as a simple Pendulum. It is released from horizontal.

(a) Find the tension in the string at the lowest point.

At the lowest point, all $E_p$ has converted to $E_k$:

$$\frac\{1\}\{2\}(0.5)v^2 = 0.5(9.81)(1.0) \implies v^2 = 19.62 \implies v = 4.43\mathrm\{ m/s\}$$

For circular motion at the lowest point:

$$T - mg = \frac\{mv^2\}\{r\}$$ $$T = mg + \frac\{mv^2\}\{r\} = 0.5(9.81) + \frac\{0.5(19.62)\}\{1.0\} = 4.905 + 9.81 = 14.72\mathrm\{ N\}$$

(b) Find the speed when the string makes an angle of $45\degree$ with the vertical.

Height above lowest point: $h = L - L\cos 45\degree = 1.0 - 0.707 = 0.293\mathrm{ m}$.

$$Mgh = \frac\{1\}\{2\}mv^2$$ $$V = \sqrt\{2gh\} = \sqrt\{2(9.81)(0.293)\} = \sqrt\{5.75\} = 2.40\mathrm\{ m/s\}$$

Question 7 (Paper 2 style)

A car of mass $1500\mathrm{ kg}$ travels up a hill of incline $5\degree$ at constant speed of $20\mathrm{ m/s}$. The total resistive force (friction + air resistance) is $400\mathrm{ N}$.

(a) Calculate the driving force required.

$$F = mg\sin\theta + f = 1500(9.81)\sin 5\degree + 400 = 1283 + 400 = 1683\mathrm\{ N\}$$

(b) Calculate the power output of the engine.

$$P = Fv = 1683 \times 20 = 33660\mathrm\{ W\} \approx 33.7\mathrm\{ kW\}$$

(c) If the engine efficiency is $25\%$What is the rate of fuel energy consumption?

$$P_\{\mathrm\{input\}\} = \frac\{33660\}\{0.25\} = 134640\mathrm\{ W\} = 134.6\mathrm\{ kW\}$$

Question 8 (Paper 1 style)

A spring with $k = 500\mathrm{ N/m}$ is used to launch a $0.1\mathrm{ kg}$ projectile vertically. The spring is compressed $0.08\mathrm{ m}$. What is the maximum height reached above the launch Point?

$$\frac\{1\}\{2\}kx^2 = mgh$$ $$H = \frac\{kx^2\}\{2mg\} = \frac\{500(0.0064)\}\{2(0.1)(9.81)\} = \frac\{3.2\}\{1.962\} = 1.63\mathrm\{ m\}$$

For the A-Level treatment of this topic, see Work, Energy and Power.

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:::tip Diagnostic Test Ready to test your understanding of Energy and Conservation? The contains the hardest questions within

the IB specification for this topic, each with a full worked solution.

Unit tests probe edge cases and common misconceptions. Integration tests combine Energy and Conservation with other physics topics to test synthesis under exam conditions.

See for instructions on self-marking and building a personal test matrix.

Common Pitfalls

1. Rounding intermediate answers too early, which compounds errors in multi-step calculations.

2. Confusing scalar and vector quantities. Always check whether direction matters for the quantity in question.

3. Forgetting to include units in final answers, especially when working with derived units like $\text{N}\,\text{kg}^{-1}\,\text{m}^2$.

4. Misidentifying the system boundary when applying conservation laws. Define what is included before writing equations.

Cross-References

Topic	Site	Link
[Energy and Work]	A-Level	View
[Energy and Work]	IB	View
[Energy and Work]	DSE	View

Worked Examples

Worked examples demonstrating the application of key concepts are covered in the detailed sub-pages linked above. :::

See Also

• Space Time And Motion
• Kinematics
• Rotational Motion