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Conservation of Mechanical Energy states that in a system with only conservative forces (like gravity or springs), the total mechanical energy (kinetic + potential) stays constant. This is a cornerstone of AP Physics because it lets you solve problems without tracking every force or acceleration—just compare energy at two points. Real-world example: A roller coaster at the top of a hill has maximum gravitational potential energy (GPE). As it descends, GPE converts to kinetic energy (KE), but the total energy (GPE + KE) stays the same (ignoring friction). If the coaster starts at 50 m, it can’t go higher than 50 m later—energy can’t be created or destroyed, only transformed.
ME = KE + PE
Kinetic Energy (KE): Energy of motion.
KE = ½mv² (m = mass, v = velocity)
Gravitational Potential Energy (GPE): Energy due to an object’s height in a gravitational field.
GPE = mgh (m = mass, g = 9.8 m/s², h = height relative to a reference point)
Elastic Potential Energy (EPE): Energy stored in a stretched or compressed spring.
EPE = ½kx² (k = spring constant, x = displacement from equilibrium)
Conservative Force: A force where work done is independent of the path taken (e.g., gravity, springs). Work done by conservative forces only depends on initial and final positions.
Example: Lifting a book straight up vs. carrying it up stairs—work done by gravity is the same.
Non-Conservative Force: A force where work done depends on the path (e.g., friction, air resistance). These forces remove mechanical energy from a system (convert it to heat, sound, etc.).
Example: A sliding box slows down due to friction—ME decreases.
Work-Energy Theorem: Work done on an object equals its change in kinetic energy.
W = ?KE = KE_final – KE_initial
Conservation of Mechanical Energy (for conservative forces only):
KE_i + PE_i = KE_f + PE_f
Power: Rate of energy transfer or work done.
Units: Watts (W) = Joules/second (J/s)
Reference Level (for GPE): The arbitrary "zero" height where GPE = 0. Always define this in problems! (e.g., "Let h = 0 at the bottom of the ramp.")
Energy Bar Charts: Visual tool to track energy changes in a system (see Step-by-Step).
How to solve conservation of energy problems on the AP exam:
If non-conservative forces (friction, applied force) are present, use W_nc = ?ME (work done by non-conservative forces = change in ME).
Define the initial and final states:
Label knowns/unknowns (heights, velocities, spring displacements).
Choose a reference level for GPE:
Set h = 0 at the lowest point in the problem (simplifies calculations).
Write the conservation equation:
Plug in formulas (½mv² for KE, mgh for GPE, ½kx² for EPE).
Solve for the unknown:
Check units (e.g., height in meters, velocity in m/s).
Check for non-conservative forces (if applicable):
Example Problem: A 2 kg block slides down a frictionless ramp from a height of 5 m. What is its speed at the bottom? - Step 1: Only gravity (conservative) acts-ME conserved. - Step 2: Initial state = top (h = 5 m, v = 0); final state = bottom (h = 0, v = ?). - Step 3: Set h = 0 at the bottom. - Step 4: mgh_i + ½mv_i² = mgh_f + ½mv_f² -(2)(9.8)(5) + 0 = 0 + ½(2)v_f² - Step 5: Solve for v_f: v_f = ?(2gh) = ?(2 × 9.8 × 5)-9.9 m/s.
Correction: Always define h = 0 (e.g., "Let h = 0 at the ground"). GPE is relative, not absolute.
Mistake: Including non-conservative forces in the conservation equation.
Correction: If friction or applied forces are present, use W_nc = ?ME instead of ME_i = ME_f. Conservation only applies to systems with only conservative forces.
Mistake: Mixing up work and energy.
Correction: Work is energy transfer (Joules), while energy is a property of the system. Work done by conservative forces changes the form of energy (e.g., GPE-KE), but not the total ME.
Mistake: Ignoring rotational kinetic energy (for rolling objects).
Correction: For rolling objects (e.g., a ball down a ramp), include rotational KE (½I?²) in the conservation equation. AP often tests this in FRQs!
Mistake: Assuming energy is conserved when it’s not.
You’ll often be asked to draw a bar chart showing KE, GPE, and EPE at different points. Practice this! (See Quick Check Question #2.)
Tricky distinction: Conservative vs. non-conservative forces:
AP trap: A problem might say "frictionless" to hint that ME is conserved.
Common FRQ setup:
A block slides down a ramp, compresses a spring, or launches off a cliff. You’ll need to:
Multiple-choice traps:
A 0.5 kg ball is dropped from a height of 10 m. Ignoring air resistance, what is its speed when it hits the ground? (A) 5 m/s (B) 10 m/s (C) 14 m/s (D) 20 m/s
Answer: (C) 14 m/s Explanation: Use ME_i = ME_f: mgh = ½mv²-v = ?(2gh) = ?(2 × 9.8 × 10)-14 m/s.
A block slides down a frictionless ramp, compresses a spring at the bottom, and briefly comes to rest. Sketch an energy bar chart for the block at: - Point A: Top of the ramp (h = 4 m, v = 0). - Point B: Bottom of the ramp (h = 0, v = max). - Point C: Maximum spring compression (h = 0, v = 0).
Answer: - Point A: Only GPE (bar at max height, KE = 0, EPE = 0). - Point B: Only KE (GPE = 0, KE at max, EPE = 0). - Point C: Only EPE (GPE = 0, KE = 0, EPE at max).
A 1 kg block slides down a 5 m ramp with a coefficient of kinetic friction-= 0.2. What is the block’s speed at the bottom? (Assume g = 10 m/s²) (A) 5 m/s (B) 7 m/s (C) 9 m/s (D) 10 m/s
Answer: (B) 7 m/s Explanation: Friction does work: W_friction = ?mgd (d = ramp length). Use W_nc = ?ME: ?mgd = ½mv² – mgh-0.2 × 1 × 10 × 5 = ½ × 1 × v² – 1 × 10 × 5-v-7 m/s.
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