Analyze Energy Using Conservation Laws

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1

A 3.0 kg block is launched by a spring (spring constant $k=200\ \text{N/m}$) compressed by 0.30 m on a frictionless horizontal surface. What speed does the block have just after leaving the spring?

Use $PE_{spring}=\tfrac12 kx^2$ and $KE=\tfrac12 mv^2$.

1.4 m/s

2.4 m/s

2.0 m/s

3.5 m/s

Explanation

This question tests understanding of conservation of energy and the ability to analyze energy transformations in a spring-mass system. The law of conservation of energy states that the total energy in an isolated system remains constant—energy can transform between different forms (kinetic, potential, thermal, etc.) but cannot be created or destroyed, so E_initial = E_final when all energy forms are accounted for. In systems with only conservative forces like gravity and springs, mechanical energy (KE + PE) is conserved, but when non-conservative forces like friction act, mechanical energy decreases as it converts to thermal energy, though total energy including thermal is still conserved. When the spring is compressed by distance x=0.30 m, it stores elastic potential energy PE_spring = ½kx² = ½(200 N/m)(0.30 m)² = 9 J. When released on the frictionless surface, this potential energy converts to kinetic energy of the attached mass: just after leaving the spring (at equilibrium), KE = ½mv² = 9 J, which gives v = √(2 × 9 / 3) = √6 ≈ 2.45 m/s. Choice C is correct because it properly applies conservation of energy E_initial = E_final and correctly calculates using the formula v = x √(k/m) ≈ 2.4 m/s. Choice D forgets the ½ factor in the kinetic energy formula or misapplies the square root, calculating a higher speed that violates conservation by exceeding the initial spring energy. When solving conservation of energy problems: (1) identify all energy forms present initially and finally (KE, PE_g, PE_spring, thermal), (2) write E_initial = E_final explicitly: for conservative forces only, use KE_i + PE_i = KE_f + PE_f; for friction present, use KE_i + PE_i = KE_f + PE_f + E_thermal, (3) substitute formulas: KE = ½mv², PE_g = mgh, PE_spring = ½kx², (4) solve for the unknown, and (5) verify your answer makes physical sense (velocities reasonable, energies positive, etc.). Remember that mechanical energy (KE + PE) is only conserved when no non-conservative forces act—if friction, air resistance, or inelastic collisions occur, mechanical energy decreases as it converts to thermal energy, but total energy including thermal is always conserved: you can test this by calculating initial mechanical energy, final mechanical energy, and the work done by friction: E_mech-i = E_mech-f + W_friction should hold exactly, demonstrating that the 'lost' mechanical energy is accounted for as thermal energy.

2

A 2.0 kg ball is dropped from 10 m and bounces straight back up to 6.0 m. Take $g=10\ \text{m/s}^2$. How much energy was transformed into thermal/sound energy during the bounce?

Assume the ball’s kinetic energy just before impact is $mgh$ and just after leaving the ground is the energy needed to rise to 6.0 m.

120 J

80 J

8 J

40 J

Explanation

This question tests understanding of conservation of energy and the ability to analyze energy transformations during an inelastic bounce. The law of conservation of energy states that the total energy in an isolated system remains constant—energy can transform between different forms (kinetic, potential, thermal, etc.) but cannot be created or destroyed, so E_initial = E_final when all energy forms are accounted for. In systems with only conservative forces like gravity and springs, mechanical energy (KE + PE) is conserved, but when non-conservative forces like friction act, mechanical energy decreases as it converts to thermal energy, though total energy including thermal is still conserved. Starting at height h₁=10 m with PE₁ = mgh₁ = (2 kg)(10 m/s²)(10 m) = 200 J, the ball gains KE=200 J just before impact (PE→KE), then after the inelastic bounce, it climbs to h₂=6 m converting KE just after to PE₂ = mgh₂ = 120 J. The energy lost to thermal/sound during the bounce is E_lost = mg(h₁ - h₂) = (2)(10)(4) = 80 J, which is now thermal energy in the deformed materials. Choice C is correct because it accurately identifies the energy transformation sequence and correctly calculates the lost energy as the difference in potential energies, 80 J. Choice D only accounts for the initial or final energy without finding the difference, leading to an overestimate that ignores the transformation to non-mechanical forms. When solving conservation of energy problems: (1) identify all energy forms present initially and finally (KE, PE_g, PE_spring, thermal), (2) write E_initial = E_final explicitly: for conservative forces only, use KE_i + PE_i = KE_f + PE_f; for friction present, use KE_i + PE_i = KE_f + PE_f + E_thermal, (3) substitute formulas: KE = ½mv², PE_g = mgh, PE_spring = ½kx², (4) solve for the unknown, and (5) verify your answer makes physical sense (velocities reasonable, energies positive, etc.). Key energy transformation patterns to recognize: falling objects convert PE → KE, rising objects convert KE → PE, springs oscillate between elastic PE ↔ KE, friction always converts mechanical energy (KE + PE) → thermal energy, and in all cases total energy remains constant when all forms are included—the phrase 'missing energy' means energy that transformed from one form to another, not energy that disappeared.

3

A 4.0 kg pendulum bob is released from rest at a height of 2.5 m above its lowest point (take $PE_g=0$ at the lowest point). Ignoring air resistance, what is the bob’s speed at the lowest point?

Use $g=10\ \text{m/s}^2$, $PE_g=mgh$, and $KE=\tfrac12 mv^2$.

7.1 m/s

10 m/s

14 m/s

5.0 m/s

Explanation

This question tests understanding of conservation of energy and the ability to analyze energy transformations in a pendulum system. The law of conservation of energy states that the total energy in an isolated system remains constant—energy can transform between different forms (kinetic, potential, thermal, etc.) but cannot be created or destroyed, so E_initial = E_final when all energy forms are accounted for. In systems with only conservative forces like gravity and springs, mechanical energy (KE + PE) is conserved, but when non-conservative forces like friction act, mechanical energy decreases as it converts to thermal energy, though total energy including thermal is still conserved. At the highest point of the swing, the pendulum has maximum gravitational PE = mgh = (4.0 kg)(10 m/s²)(2.5 m) = 100 J and zero KE since released from rest, while at the lowest point it has minimum PE (zero) and maximum KE = ½mv². Energy conservation gives mgh_top = ½mv²_bottom, so v = √(2gh) = √(2 × 10 × 2.5) = √50 ≈ 7.07 m/s, and since ignoring air resistance, total mechanical energy remains constant. Choice B is correct because it properly applies conservation of energy E_initial = E_final and correctly calculates the speed using v = √(2gh) ≈ 7.1 m/s. Choice C confuses the calculation by omitting the ½ in KE or using v = √(gh), leading to √25 = 5 m/s which is too low, or possibly √(4gh) = 10 m/s which overestimates. When solving conservation of energy problems: (1) identify all energy forms present initially and finally (KE, PE_g, PE_spring, thermal), (2) write E_initial = E_final explicitly: for conservative forces only, use KE_i + PE_i = KE_f + PE_f; for friction present, use KE_i + PE_i = KE_f + PE_f + E_thermal, (3) substitute formulas: KE = ½mv², PE_g = mgh, PE_spring = ½kx², (4) solve for the unknown, and (5) verify your answer makes physical sense (velocities reasonable, energies positive, etc.). Remember that mechanical energy (KE + PE) is only conserved when no non-conservative forces act—if friction, air resistance, or inelastic collisions occur, mechanical energy decreases as it converts to thermal energy, but total energy including thermal is always conserved: you can test this by calculating initial mechanical energy, final mechanical energy, and the work done by friction: E_mech-i = E_mech-f + W_friction should hold exactly, demonstrating that the 'lost' mechanical energy is accounted for as thermal energy.

4

A 1.5 kg ball is dropped from rest from a height of 12 m above the ground ($g=10\ \text{m/s}^2$). Ignoring air resistance, what is the ball’s kinetic energy just before it hits the ground?

Use $PE_g=mgh$ and $KE=\tfrac12 mv^2$.

18 J

180 J

240 J

120 J

Explanation

This question tests understanding of conservation of energy and the ability to analyze energy transformations in a system involving a falling object. The law of conservation of energy states that the total energy in an isolated system remains constant—energy can transform between different forms (kinetic, potential, thermal, etc.) but cannot be created or destroyed, so E_initial = E_final when all energy forms are accounted for. In systems with only conservative forces like gravity and springs, mechanical energy (KE + PE) is conserved, but when non-conservative forces like friction act, mechanical energy decreases as it converts to thermal energy, though total energy including thermal is still conserved. In this scenario, the ball starts at height h=12 m with gravitational potential energy PE = mgh = (1.5 kg)(10 m/s²)(12 m) = 180 J and zero kinetic energy since it's dropped from rest. As it falls, ignoring air resistance, PE converts entirely to KE, so just before hitting the ground where h=0, KE = ½mv² = 180 J, demonstrating complete PE → KE transformation. Choice C is correct because it properly applies conservation of energy E_initial = E_final accounting for all forms and accurately identifies that the kinetic energy equals the initial potential energy of 180 J. Choice D forgets to use the correct potential energy or possibly doubles it, claiming 240 J, which violates conservation by suggesting more energy than initially present. When solving conservation of energy problems: (1) identify all energy forms present initially and finally (KE, PE_g, PE_spring, thermal), (2) write E_initial = E_final explicitly: for conservative forces only, use KE_i + PE_i = KE_f + PE_f; for friction present, use KE_i + PE_i = KE_f + PE_f + E_thermal, (3) substitute formulas: KE = ½mv², PE_g = mgh, PE_spring = ½kx², (4) solve for the unknown, and (5) verify your answer makes physical sense (velocities reasonable, energies positive, etc.). Remember that mechanical energy (KE + PE) is only conserved when no non-conservative forces act—if friction, air resistance, or inelastic collisions occur, mechanical energy decreases as it converts to thermal energy, but total energy including thermal is always conserved: you can test this by calculating initial mechanical energy, final mechanical energy, and the work done by friction: E_mech-i = E_mech-f + W_friction should hold exactly, demonstrating that the 'lost' mechanical energy is accounted for as thermal energy.

5

A 1.0 kg cart is at the top of a frictionless track at height 8 m (take the bottom as $h=0$). At a point halfway down, the cart is at height 4 m. Which statement correctly describes the energy changes from the top to the halfway point?

Ignore air resistance and use $PE_g=mgh$.

Gravitational potential energy decreases by 40 J and kinetic energy increases by 40 J.

Gravitational potential energy increases by 40 J and kinetic energy decreases by 40 J.

Both gravitational potential energy and kinetic energy decrease by 40 J.

Mechanical energy decreases by 40 J because energy is destroyed.

Explanation

This question tests understanding of conservation of energy and the ability to analyze energy transformations in a frictionless system. The law of conservation of energy states that the total energy in an isolated system remains constant—energy can transform between different forms (kinetic, potential, thermal, etc.) but cannot be created or destroyed, so E_initial = E_final when all energy forms are accounted for. In systems with only conservative forces like gravity and springs, mechanical energy (KE + PE) is conserved, but when non-conservative forces like friction act, mechanical energy decreases as it converts to thermal energy, though total energy including thermal is still conserved. From the top at h=8 m, PE_i = mgh = (1 kg)g(8 m), to halfway at h=4 m, PE_f = mg(4 m), so ΔPE = -mg(4 m) = -40 J (assuming g=10 m/s² for numerical value), and since frictionless, this decrease converts directly to KE increase of +40 J. Energy conservation ensures mechanical energy remains constant: PE decrease equals KE increase. Choice A is correct because it accurately identifies the energy transformation sequence, with PE decreasing and KE increasing by the same amount, maintaining conservation. Choice D violates conservation of energy by claiming energy is destroyed rather than transformed—energy never disappears, it only changes form from potential to kinetic here. When solving conservation of energy problems: (1) identify all energy forms present initially and finally (KE, PE_g, PE_spring, thermal), (2) write E_initial = E_final explicitly: for conservative forces only, use KE_i + PE_i = KE_f + PE_f; for friction present, use KE_i + PE_i = KE_f + PE_f + E_thermal, (3) substitute formulas: KE = ½mv², PE_g = mgh, PE_spring = ½kx², (4) solve for the unknown, and (5) verify your answer makes physical sense (velocities reasonable, energies positive, etc.). Remember that mechanical energy (KE + PE) is only conserved when no non-conservative forces act—if friction, air resistance, or inelastic collisions occur, mechanical energy decreases as it converts to thermal energy, but total energy including thermal is always conserved: you can test this by calculating initial mechanical energy, final mechanical energy, and the work done by friction: E_mech-i = E_mech-f + W_friction should hold exactly, demonstrating that the 'lost' mechanical energy is accounted for as thermal energy.

6

A pendulum bob of mass $1.0,\text{kg}$ is released from rest at a height of $0.80,\text{m}$ above its lowest point (take $g=10,\text{m/s}^2$). Neglect air resistance. What is the bob’s kinetic energy at the lowest point?

$8,\text{J}$

$16,\text{J}$

$4,\text{J}$

$0,\text{J}$

Explanation

This question tests understanding of conservation of energy and the ability to analyze energy transformations in a system. The law of conservation of energy states that the total energy in an isolated system remains constant—energy can transform between different forms (kinetic, potential, thermal, etc.) but cannot be created or destroyed, so E_initial = E_final when all energy forms are accounted for. In systems with only conservative forces like gravity and springs, mechanical energy (KE + PE) is conserved, but when non-conservative forces like friction act, mechanical energy decreases as it converts to thermal energy, though total energy including thermal is still conserved. For pendulum/oscillation: At the highest point of the swing, the pendulum has maximum gravitational PE = mgh = (1 kg)(10 m/s²)(0.8 m) = 8 J (where h is height above lowest point) and minimum KE (zero if momentarily at rest), while at the lowest point it has minimum PE (zero if we use lowest point as reference) and maximum KE = ½mv². Energy conservation gives mgh_top = ½mv²_bottom, and if no friction acts, this total mechanical energy remains constant throughout the swing: E_mech = mgh + ½mv² = constant at every point, so KE_bottom = 8 J. Choice C is correct because it properly applies conservation of energy E_initial = E_final accounting for all forms and accurately identifies the energy transformation sequence. Choice D violates conservation of energy by claiming energy is destroyed rather than transformed—energy never disappears, it only changes form from mechanical (KE and PE) to thermal energy when friction acts, or between KE and PE when only conservative forces act. When solving conservation of energy problems: (1) identify all energy forms present initially and finally (KE, PE_g, PE_spring, thermal), (2) write E_initial = E_final explicitly: for conservative forces only, use KE_i + PE_i = KE_f + PE_f; for friction present, use KE_i + PE_i = KE_f + PE_f + E_thermal, (3) substitute formulas: KE = ½mv², PE_g = mgh, PE_spring = ½kx², (4) solve for the unknown, and (5) verify your answer makes physical sense (velocities reasonable, energies positive, etc.).

7

A 3.0 kg block is launched by a compressed spring on a horizontal surface. The spring constant is $k=200\ \text{N/m}$ and the spring is compressed $x=0.30\ \text{m}$. Assume no friction and that the block starts from rest. What is the block’s speed just as it leaves the spring (when the spring returns to its natural length)?

3.0 m/s

2.4 m/s

6.0 m/s

4.2 m/s

Explanation

This question tests understanding of conservation of energy and the ability to analyze energy transformations in a system. The law of conservation of energy states that the total energy in an isolated system remains constant—energy can transform between different forms (kinetic, potential, thermal, etc.) but cannot be created or destroyed, so E_initial = E_final when all energy forms are accounted for. In systems with only conservative forces like gravity and springs, mechanical energy (KE + PE) is conserved, but when non-conservative forces like friction act, mechanical energy decreases as it converts to thermal energy, though total energy including thermal is still conserved. When the spring is compressed by distance x=0.30 m, it stores elastic potential energy PE_spring = ½kx² = ½(200 N/m)(0.30 m)² = 100×0.09 = 9 J. When released on the horizontal frictionless surface, this potential energy converts to kinetic energy of the attached block: at maximum speed (when the spring returns to natural length), KE = ½mv² equals the initial PE_spring, so ½(3.0)v² = 9, 1.5 v² = 9, v² = 6, v = √6 ≈ 2.4 m/s. Choice A is correct because it properly applies conservation of energy E_initial = E_final accounting for all forms and correctly calculates using the formula v = √(k/m) × x ≈ 2.4 m/s. Choice B forgets the ½ factor in the kinetic or potential energy formula, perhaps calculating v = x √(2k/m) or similar, leading to a higher speed like 3.0 m/s, which violates conservation. Key energy transformation patterns to recognize: falling objects convert PE → KE, rising objects convert KE → PE, springs oscillate between elastic PE ↔ KE, friction always converts mechanical energy (KE + PE) → thermal energy, and in all cases total energy remains constant when all forms are included—the phrase "missing energy" means energy that transformed from one form to another, not energy that disappeared.

8

A 5.0 kg pendulum bob is released from rest at a point 2.0 m above its lowest point (take the lowest point as $PE_g=0$ and $g=10\ \text{m/s}^2$). Ignoring air resistance, what is the bob’s kinetic energy at the lowest point?

50 J

20 J

100 J

0 J

Explanation

This question tests understanding of conservation of energy and the ability to analyze energy transformations in a system. The law of conservation of energy states that the total energy in an isolated system remains constant—energy can transform between different forms (kinetic, potential, thermal, etc.) but cannot be created or destroyed, so E_initial = E_final when all energy forms are accounted for. In systems with only conservative forces like gravity and springs, mechanical energy (KE + PE) is conserved, but when non-conservative forces like friction act, mechanical energy decreases as it converts to thermal energy, though total energy including thermal is still conserved. For the pendulum, at the highest point the bob has maximum gravitational PE = mgh = (5.0 kg)(10 m/s²)(2.0 m) = 100 J and minimum KE (zero since released from rest), while at the lowest point it has minimum PE (zero) and maximum KE = ½mv². Energy conservation gives mgh_top = ½mv²_bottom, and since no friction acts, this total mechanical energy remains constant: at the lowest point, KE = mgh = 100 J. Choice A is correct because it properly applies conservation of energy E_initial = E_final accounting for all forms and accurately identifies the energy transformation sequence from PE to KE. Choice D violates conservation of energy by claiming energy is destroyed rather than transformed—energy never disappears, it only changes form from potential to kinetic when only conservative forces act. When solving conservation of energy problems: (1) identify all energy forms present initially and finally (KE, PE_g, PE_spring, thermal), (2) write E_initial = E_final explicitly: for conservative forces only, use KE_i + PE_i = KE_f + PE_f; for friction present, use KE_i + PE_i = KE_f + PE_f + E_thermal, (3) substitute formulas: KE = ½mv², PE_g = mgh, PE_spring = ½kx², (4) solve for the unknown, and (5) verify your answer makes physical sense (velocities reasonable, energies positive, etc.).

9

A $4.0,\text{kg}$ sled starts from rest at the top of a $12,\text{m}$ hill (take $g=10,\text{m/s}^2$). It slides down a rough slope and reaches the bottom with speed $12,\text{m/s}$ (bottom is the $PE_g=0$ reference). During this motion, some mechanical energy is converted to thermal energy by friction. Using conservation of energy, how much thermal energy $E_{\text{thermal}}$ was produced?

Use: $PE_g=mgh$, $KE=\tfrac12 mv^2$.

$0,\text{J}$

$480,\text{J}$

$96,\text{J}$

$192,\text{J}$

Explanation

This question tests understanding of conservation of energy and the ability to analyze energy transformations in a system with friction. The law of conservation of energy states that the total energy in an isolated system remains constant—energy can transform between different forms (kinetic, potential, thermal, etc.) but cannot be created or destroyed, so E_initial = E_final when all energy forms are accounted for. In systems with only conservative forces like gravity and springs, mechanical energy (KE + PE) is conserved, but when non-conservative forces like friction act, mechanical energy decreases as it converts to thermal energy, though total energy including thermal is still conserved. Initially the sled has mechanical energy E_mech-i = PE_i + KE_i = mgh + 0 = (4 kg)(10 m/s²)(12 m) = 480 J, and finally it has E_mech-f = PE_f + KE_f = 0 + ½mv² = ½(4)(144) = 288 J. The decrease in mechanical energy ΔE_mech = 480 - 288 = 192 J equals the work done by friction, which converted this mechanical energy to thermal energy (heat) through the friction force acting over distance: the total energy is still conserved when we include thermal: E_mech-i = E_mech-f + E_thermal. Choice B is correct because it properly applies conservation of energy E_initial = E_final accounting for all forms and correctly calculates the thermal energy as the difference in mechanical energy. Choice C confuses the total initial potential energy with the thermal energy, claiming 480 J when actually only the portion not converted to kinetic energy becomes thermal: 480 J initial PE transforms to 288 J KE + 192 J thermal, not all to thermal. When solving conservation of energy problems: (1) identify all energy forms present initially and finally (KE, PE_g, PE_spring, thermal), (2) write E_initial = E_final explicitly: for conservative forces only, use KE_i + PE_i = KE_f + PE_f; for friction present, use KE_i + PE_i = KE_f + PE_f + E_thermal, (3) substitute formulas: KE = ½mv², PE_g = mgh, PE_spring = ½kx², (4) solve for the unknown, and (5) verify your answer makes physical sense (velocities reasonable, energies positive, etc.).

10

A $1.5,\text{kg}$ block is launched by a spring on a frictionless horizontal surface. The spring constant is $k=200,\text{N/m}$ and the spring is compressed $x=0.30,\text{m}$. After the block leaves the spring, what is its speed?

Use: $PE_{\text{spring}}=\tfrac12 kx^2$ and $KE=\tfrac12 mv^2$.

$2.0,\text{m/s}$

$3.5,\text{m/s}$

$12,\text{m/s}$

$6.0,\text{m/s}$

Explanation

This question tests understanding of conservation of energy and the ability to analyze energy transformations in a system. The law of conservation of energy states that the total energy in an isolated system remains constant—energy can transform between different forms (kinetic, potential, thermal, etc.) but cannot be created or destroyed, so E_initial = E_final when all energy forms are accounted for. In systems with only conservative forces like gravity and springs, mechanical energy (KE + PE) is conserved, but when non-conservative forces like friction act, mechanical energy decreases as it converts to thermal energy, though total energy including thermal is still conserved. When the spring is compressed by distance x = 0.30 m, it stores elastic potential energy PE_spring = ½kx² = ½(200 N/m)(0.30 m)² = 9 J. When released, this potential energy converts to kinetic energy of the attached mass: at maximum speed (passing through equilibrium), KE = ½mv² equals the initial PE_spring, so ½mv² = ½kx², which gives v = √(k/m) × x = √(200/1.5) × 0.3 ≈ 3.46 m/s, approximately 3.5 m/s. Choice B is correct because it properly applies conservation of energy E_initial = E_final accounting for all forms and correctly calculates using appropriate formula KE = ½mv² or PE_spring = ½kx². Choice C forgets to take the square root properly or doubles the value, perhaps calculating v = (k/m) x or similar error, leading to an overestimated speed that violates energy equivalence. When solving conservation of energy problems: (1) identify all energy forms present initially and finally (KE, PE_g, PE_spring, thermal), (2) write E_initial = E_final explicitly: for conservative forces only, use KE_i + PE_i = KE_f + PE_f; for friction present, use KE_i + PE_i = KE_f + PE_f + E_thermal, (3) substitute formulas: KE = ½mv², PE_g = mgh, PE_spring = ½kx², (4) solve for the unknown, and (5) verify your answer makes physical sense (velocities reasonable, energies positive, etc.).

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