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  2. MCAT Chemical and Physical Foundations of Biological Systems
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MCAT Chemical and Physical Foundations of Biological Systems Flashcards: 4a Energy Conservation Mechanical Advantage

Study 4a Energy Conservation Mechanical Advantage in MCAT Chemical and Physical Foundations of Biological Systems with focused flashcards that help you recognize the idea, recall the key rule, and apply it in practice-style prompts.

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What this deck covers

This deck focuses on 4a Energy Conservation Mechanical Advantage, giving you a quick way to review the definitions, rules, and examples that matter most for MCAT Chemical and Physical Foundations of Biological Systems.

How to use these flashcards

Work through these flashcards in short sessions. Try to answer each prompt before flipping the card, then revisit any cards you miss until the explanation feels automatic.

MCAT Chemical and Physical Foundations of Biological Systems Flashcards: 4a Energy Conservation Mechanical Advantage

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QUESTION

What is the definition of mechanical advantage (MA) for a simple machine using forces?

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ANSWER

MA=FoutFinMA = \frac{F_{out}}{F_{in}}MA=Fin​Fout​​. Mechanical advantage measures force amplification, defined as the ratio of output to input force in simple machines.

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Flashcard 1: What is the definition of mechanical advantage (MA) for a simple machine using forces?

Answer: MA=FoutFinMA = \frac{F_{out}}{F_{in}}MA=Fin​Fout​​. Mechanical advantage measures force amplification, defined as the ratio of output to input force in simple machines.

Flashcard 2: Identify the ideal MA for an ideal fixed pulley (single pulley attached to the ceiling).

Answer: MA=1MA = 1MA=1. A fixed pulley changes force direction but not magnitude, resulting in no net force amplification ideally.

Flashcard 3: State the ideal simple-machine energy relation between input and output work.

Answer: Win=WoutW_{in} = W_{out}Win​=Wout​. In ideal machines without friction, energy conservation implies equal input and output work despite force-distance trade-offs.

Flashcard 4: State the work–energy theorem relating net work WnetW_{net}Wnet​ to kinetic energy change.

Answer: Wnet=ΔKW_{net} = \Delta KWnet​=ΔK. The theorem states that net work on an object equals its change in kinetic energy, derived from Newton's second law integrated over displacement.

Flashcard 5: State the formula for work done by a constant force FFF over displacement ddd at angle θ\thetaθ.

Answer: W=Fdcos⁡θW = Fd\cos\thetaW=Fdcosθ. Work measures energy transfer by force along displacement, with cos⁡θ\cos\thetacosθ accounting for the component parallel to motion.

Flashcard 6: State the formula for power in terms of work WWW done over time interval Δt\Delta tΔt.

Answer: P=WΔtP = \frac{W}{\Delta t}P=ΔtW​. Power represents the rate of work done, averaging energy transfer over time for non-instantaneous processes.

Flashcard 7: State the instantaneous power formula for a force F⃗\vec{F}F acting on a moving object with velocity v⃗\vec{v}v.

Answer: P=F⃗⋅v⃗P = \vec{F}\cdot\vec{v}P=F⋅v. Instantaneous power is the dot product capturing the rate of energy transfer at a specific moment for varying forces or velocities.

Flashcard 8: What is the sign of work done by kinetic friction on a sliding object moving forward?

Answer: Negative work. Kinetic friction opposes motion, so the angle between force and displacement is 180°, yielding a negative cosine and energy dissipation.

Flashcard 9: State the magnitude of kinetic friction force in terms of μk\mu_kμk​ and normal force NNN.

Answer: fk=μkNf_k = \mu_k Nfk​=μk​N. Kinetic friction is proportional to the normal force, with μk\mu_kμk​ as the coefficient depending on surface properties.

Flashcard 10: State the relationship between nonconservative work WncW_{nc}Wnc​ and mechanical energy change ΔEmech\Delta E_{mech}ΔEmech​.

Answer: Wnc=ΔEmechW_{nc} = \Delta E_{mech}Wnc​=ΔEmech​. Nonconservative forces like friction change mechanical energy through path-dependent work, equaling the net gain or loss in EmechE_{mech}Emech​.

Flashcard 11: Identify the energy conservation equation for a system including nonconservative work WncW_{nc}Wnc​.

Answer: Ki+Ui+Wnc=Kf+UfK_i + U_i + W_{nc} = K_f + U_fKi​+Ui​+Wnc​=Kf​+Uf​. This equation accounts for energy input or dissipation by nonconservative forces, balancing initial and final mechanical energies.

Flashcard 12: State the formula for elastic potential energy stored in an ideal spring compressed or stretched by xxx.

Answer: Us=12kx2U_s = \frac{1}{2}kx^2Us​=21​kx2. Elastic potential energy derives from Hooke's law, integrating force over displacement to store energy quadratically with deformation.

Flashcard 13: What is the definition of ideal mechanical advantage (IMA) using distances moved?

Answer: IMA=dindoutIMA = \frac{d_{in}}{d_{out}}IMA=dout​din​​. Ideal mechanical advantage assumes no energy losses, equating to the ratio of input to output distances based on geometry.

Flashcard 14: Identify the condition under which mechanical energy is conserved in a system.

Answer: Only conservative forces do work (no nonconservative work). Conservation holds when work is path-independent, as conservative forces like gravity store energy as potential without dissipation.

Flashcard 15: State the formula for gravitational potential energy near Earth for a mass at height hhh.

Answer: Ug=mghU_g = mghUg​=mgh. This formula quantifies the energy stored due to an object's position in a gravitational field, derived from the work done against gravity over height hhh.

Flashcard 16: State the formula for kinetic energy of a mass mmm moving at speed vvv.

Answer: K=12mv2K = \frac{1}{2}mv^2K=21​mv2. This equation calculates the energy of motion, arising from integrating force over distance for constant acceleration.

Flashcard 17: What is the definition of mechanical energy EmechE_{mech}Emech​ in terms of KKK and UUU?

Answer: Emech=K+UE_{mech} = K + UEmech​=K+U. Mechanical energy sums kinetic and potential energies, representing the total energy convertible between motion and position without losses.

Flashcard 18: State the efficiency formula for a machine in terms of output and input work.

Answer: η=WoutWin\eta = \frac{W_{out}}{W_{in}}η=Win​Wout​​. Efficiency quantifies the fraction of input work converted to useful output, less than 1 due to losses like friction.

Flashcard 19: State the efficiency formula in terms of actual mechanical advantage (AMA) and IMA.

Answer: η=AMAIMA\eta = \frac{AMA}{IMA}η=IMAAMA​. This relates actual performance (AMA) to theoretical maximum (IMA), highlighting losses in real machines.

Flashcard 20: Identify the ideal MA for an ideal movable pulley with one pulley supporting the load by two rope segments.

Answer: MA=2MA = 2MA=2. The movable pulley halves the required input force by distributing the load across two rope segments ideally.

Flashcard 21: What is the ideal MA of an ideal block-and-tackle equal to, in terms of supporting rope segments nnn?

Answer: MA=nMA = nMA=n. In a block-and-tackle system, mechanical advantage equals the number of load-supporting ropes, amplifying force proportionally.

Flashcard 22: Find the speed at the bottom after dropping from rest through height hhh with no friction.

Answer: v=2ghv = \sqrt{2gh}v=2gh​. Conservation of energy converts gravitational potential to kinetic, yielding speed independent of mass for free fall near Earth.

Flashcard 23: Find the work done by kinetic friction over distance ddd on a level surface with coefficient μk\mu_kμk​.

Answer: Wf=−μkmgdW_f = -\mu_k mgdWf​=−μk​mgd. Friction work is negative as it opposes motion, dissipating energy proportional to coefficient, weight, and distance on a flat surface.

Flashcard 24: Identify the input force needed to lift a load FoutF_{out}Fout​ with an ideal machine having MA=4MA = 4MA=4.

Answer: Fin=Fout4F_{in} = \frac{F_{out}}{4}Fin​=4Fout​​. For ideal machines, mechanical advantage inversely relates input and output forces, requiring one-fourth force to lift with MA=4.

Flashcard 25: Find the compression xxx of a spring that stops a mass mmm moving at speed vvv on a frictionless surface.

Answer: x=vmkx = v\sqrt{\frac{m}{k}}x=vkm​​. Equating initial kinetic energy to stored elastic potential gives the deformation where the spring constant balances mass and velocity.