A comprehensive 3-block high school physics lesson deconstructing macroscopic contact forces including elastic deformation, normal force, friction, and buoyancy through empirical inquiry and mathematical modeling.
GUESS Takeaway: Horizontal push produces vertical friction to support weight!
GUESS guarantees you never miss a step in multi-force vector problems! TEKS 5D
Block 5 Modeling • TE p. 42
The Pinball Launcher: Stored Energy to Speed
Spring Gun Model
How the Spring Launches the Ball
\Delta x (How far you pull back)
More Pull (\(\Delta x\)) = Way More Speed (\(v\))!
Common Student Trap Busted!
Does the spring push with the same force the whole way out? NO! When fully squished, it kicks with maximum force. As it uncoils, the push dies down until it drops to zero right as the ball flies away!
Energy Trade: Squeeze to Speed
You do mechanical work to squish the spring coils. That stored potential energy instantly converts into the kinetic energy of the speeding steel ball!
Assess on the Spot Look-For: Make sure students draw shrinking arrows as the spring stretches back out! TEKS 5F / 5D
Block 6 Wrap-Up • The Grand Connection
The Big Reveal: Everything Is Made of Springs!
Unit Mastery
1. The Secret of Matter
All matter (wood, rubber, steel, bones) is held together by electric atomic bonds that act exactly like microscopic coils.
When you push a wall, you compress those atomic springs. That is all "Normal Force" has ever been!
The Tennis Ball Solved!
2. Friction & Buoyancy
Friction: Microscopic mountain peaks interlocking like Velcro.
Buoyancy: Water shoved aside by an intruder pushing back with the exact weight of the puddle displaced.
Macroscopic Contact Forces
3. Newton's 2nd Law
\[ a = \frac{F_{net}}{m} \]
Add up all the pushes and pulls using GUESS. The leftover net force determines whether an object speeds up, slows down, or stays frozen!
Ready for the Unit Quiz!
You now understand how the physical world pushes back! TEKS 5F & 5D Mastered
TEKS 5D
A book of mass \(m = 1.50\text{ kg}\) is held against a wall. The static coefficient is \(\mu_s = 0.40\). Calculate the minimum horizontal push force (\(F_{push}\)) needed to stop it slipping downward.
Given (G)
Unknown (U)
Equation (E)
Substitute (S)
Solve (S)
Physics Dynamics • Types of Forces Worksheet
Page 2 of 3 • GUESS Calculations (12pt Edition)
Block 6 Evaluation & Model Synthesis
Student Name:
Part 3
Conceptual Mastery Checkpoints
7. A heavy wooden crate sits motionless on a rough floor. What describes the contact forces?
A. The floor cannot push upward because inanimate objects are passive.
B. The normal force balances gravity, while static friction is zero until pushed.
C. Static friction pushes upward on the crate to counteract Earth's gravity.
D. Kinetic friction prevents the crate from accelerating into the ground.
8. A spring compressed by distance \(\Delta x\) is released. What describes the force as it uncoils?
A. The force remains perfectly constant until the ball leaves the coil.
B. The force increases steadily as the spring expands toward equilibrium.
C. The force decreases linearly down to zero at the equilibrium position.
D. The force abruptly switches direction and pulls the ball backward.
Part 4
Math Skill: Absolute Value & Engineering Tolerance (TE p. 44)
TEKS 5D
In physics and engineering, force tolerance measures the maximum allowed difference from a target force regardless of direction: \(|F_{\text{actual}} - F_{\text{target}}| \le \text{Tolerance}\).
A pinball launcher spring must exert a target force of \(50.0\text{ N}\) with a tolerance of \(\pm 4.0\text{ N}\). Write the absolute value inequality and find the acceptable range of forces.
Part 5
Model Synthesis: Pinball Launcher Acceleration (TE p. 42 & 45)
Newtonian Synthesis
When the pinball plunger is pulled back \(3.0\text{ cm}\) and released, does the steel pinball experience constant acceleration or changing acceleration during launch? Use Newton's Second Law (\(a = F_{net}/m\)) and Hooke's Law (\(F_s = k\Delta x\)) to explain your answer.
Physics Dynamics • Types of Forces Worksheet
Page 3 of 3 • Checkpoints & Synthesis (12pt Edition)
"The normal force balances gravity, while static friction is zero until pushed." Passive objects exert normal forces by atomic compression. Static friction only appears when a tangential applied force is present.
Question 8: Correct Answer C
"The force decreases linearly down to zero at the equilibrium position." By Hooke's Law (\(F_s = k\Delta x\)), as the spring returns to its natural uncompressed length (\(\Delta x \to 0\)), the push force drops to zero.
Exemplar Answer: The pinball experiences changing (non-constant) acceleration. By Hooke's Law, the spring force is \(F_s = k\Delta x\). As the plunger pushes the ball forward, the compression distance \(\Delta x\) continuously decreases toward zero. According to Newton's Second Law:
Because the restoring force drops continuously as the spring expands, the acceleration of the pinball starts at a maximum and steadily decreases to zero when the ball disconnects from the plunger.
Physics Dynamics • Force Fundamentals Answer Key
Page 3 of 3 • Evaluation & Synthesis (12pt Edition)
Surface Type
Trial 1 \(h_1\) (m)
Trial 2 \(h_1\) (m)
Average Bounce (m)
Visible Squish? (Ball vs Surface)
Impact Sound
Hard Tabletop / Tile
Ball squishes
Loud snap
Soft Foam / Cushion
Foam squishes
Muffled thud
Station 1 Question: Why does the foam pad make the bounce quieter and lower than the hard table?
Station 2
Hooke's Law: Spring Stretch (\(F_s = k\Delta x\))
\(F_g = mg\)
Hang increasing masses on the spring. Measure initial position \(x_0\) and stretched position \(x\) to find stretch \(\Delta x = x - x_0\).
Trial
Hanging Mass \(m\) (kg)
Weight Force \(mg\) (N)
Stretch Distance \(\Delta x\) (m)
Spring Constant \(k = F/\Delta x\) (N/m)
1
0.100 kg
0.98 N
2
0.200 kg
1.96 N
3
0.300 kg
2.94 N
Station 2 Question: When you doubled the hanging weight from \(0.100\text{ kg}\) to \(0.200\text{ kg}\), did the stretch also double? What does this tell you about the spring?
Physics Dynamics • Contact Forces Lab Guide
Page 2 of 4 • Stations 1 & 2 (12pt Edition)
Page 3 Station 3 & Station 4 Data Collection
Student Name:
Station 3
Surface Friction: Starting vs. Sliding
Spring scale pull
Pull the wooden block across different surfaces. Record the peak force needed to start moving (Static Friction \(f_s\)) and the steady force to keep it sliding (Kinetic Friction \(f_k\)).
Surface
Normal Force \(F_N\) (N)
Force to Start Moving \(f_s\) (N)
Force to Keep Sliding \(f_k\) (N)
Is \(f_s > f_k\)?
Wood on Desk
YES / NO
Wood on Sandpaper
YES / NO
Wood on Wax Paper
YES / NO
Station 3 Question: Why does it take more force to break the object free from a standstill than to keep it sliding?
Station 4
Buoyancy: The Water Push (Archimedes)
\(F_B = F_{\text{air}} - F_{\text{sub}}\)
Weigh the metal block in air with a spring scale. Submerge it into an overflow cup of water, measure the new scale reading, and weigh the overflow water that spilled out.
Object
Weight in Air (N)
Weight Underwater (N)
Water's Upward Push \(F_B\) (N)
Weight of Spilled Water (N)
Heavy Metal Block
Station 4 Question: How does the upward push of the water (\(F_B\)) compare to the weight of the water that spilled out?
Physics Dynamics • Contact Forces Lab Guide
Page 3 of 4 • Stations 3 & 4 (12pt Edition)
Page 4 Real-World Engineering Synthesis
Student Name:
Synthesis
Connecting Lab Results to Real-World Designs
1. Car Crash Crumple Zones: Old vintage cars had rock-hard steel bumpers, while modern cars have front ends designed to crumple and accordion during a crash. Based on what you observed at Station 1 with hard vs. soft surfaces, why are crumple zones much safer for the passengers inside?
2. Athletic Running Shoes: Basketball and running shoes have thick, squishy foam soles. Using the concept of normal force and contact time, explain how squishy shoe soles protect a runner's knees and bones when landing from a jump.
3. Pinball Launch Springs: In a pinball machine, you pull back a spring plunger to launch a heavy steel ball. Using Hooke's Law from Station 2, explain what happens to the launch force and the ball's acceleration if you pull the plunger back \(4\text{ cm}\) instead of \(2\text{ cm}\).
Big Physics Takeaway
All contact forces (normal force, friction, springs, and collisions) arise from atoms pushing, pulling, or sliding against each other. When an interaction allows for more squish or deformation, the contact time increases and the peak impact force drops!
Physics Dynamics • Contact Forces Lab Guide
Page 4 of 4 • Synthesis (12pt Edition)
Hard Table
0.55 m
0.53 m
0.54 m
Ball squishes
Sharp crack
Foam Pad
0.18 m
0.16 m
0.17 m
Foam dents
Dull thud
Station 1 Exemplar Answer:
The foam pad deforms macroscopically and absorbs a significant portion of the ball's kinetic energy, converting it into internal friction and thermal energy within the open-cell foam. Because less elastic potential energy is stored and returned to the ball, the rebound height is much lower and the sound is muffled.
Station 2 Data Hooke's Law: Spring Stretch (8 pts)
\(k \approx 24.5\text{ N/m}\)
Trial
Mass \(m\)
Weight \(F_g\)
Stretch \(\Delta x\)
\(k = F/\Delta x\)
1
0.100 kg
0.98 N
0.040 m
24.5 N/m
2
0.200 kg
1.96 N
0.080 m
24.5 N/m
3
0.300 kg
2.94 N
0.121 m
24.3 N/m
Station 2 Exemplar Answer:
Yes, doubling the hanging weight from \(0.98\text{ N}\) to \(1.96\text{ N}\) doubles the stretch from \(0.040\text{ m}\) to \(0.080\text{ m}\). This confirms Hooke's Law: restoring force is directly proportional to displacement (\(F \propto \Delta x\)) with a constant spring stiffness \(k\).
Teacher Edition Stations 3 & 4 Sample Data & Solutions
Expected Values
Station 3 Data Friction: Starting vs. Sliding (8 pts)
\(f_s > f_k\) Always
Surface
Normal Force \(F_N\)
Start Moving \(f_s\)
Keep Sliding \(f_k\)
Is \(f_s > f_k\)?
Wood on Desk
2.00 N
0.70 N
0.50 N
YES
Wood on Sandpaper
2.00 N
1.40 N
1.10 N
YES
Wood on Wax Paper
2.00 N
0.45 N
0.30 N
YES
Station 3 Exemplar Answer:
When stationary, surface microscopic ridges interlock deeply and form temporary electrostatic bonds. Breaking these interlocking ridges requires a large initial force (\(f_s\)). Once in motion, the surfaces skate across the tops of the ridges before settling, creating less resistance (\(f_k\)).
Station 4 Data Buoyancy & Displaced Water (8 pts)
Archimedes Principle
Object
Weight in Air
Submerged Weight
Buoyant Push \(F_B\)
Spilled Water Weight
Metal Block
1.00 N
0.72 N
0.28 N
0.28 N
Station 4 Exemplar Answer:
The upward buoyant force (\(F_B = 1.00\text{ N} - 0.72\text{ N} = 0.28\text{ N}\)) exactly equals the weight of the spilled water (\(0.28\text{ N}\)). This confirms Archimedes' principle: any submerged body experiences an upward buoyant push equal to the weight of the fluid it displaces.
Exemplar Answer: Old rigid steel cars acted like the hard tabletop: stopping immediately in milliseconds, resulting in massive, lethal peak impact forces transferred to passengers. Modern crumple zones act like the soft foam pad: they accordion and crush over several feet. This extends the collision duration (\(\Delta t\)), spreading out the change in momentum and dramatically reducing the peak impact force on the cabin.
2. Running Shoes & Knee Protection (6 pts)
Exemplar Answer: The foam midsole compresses macroscopically during foot strike. This extends the deceleration contact time from \(\approx 0.01\text{ s}\) to \(\approx 0.03\text{ s}\). By \(F_{avg} = \Delta p / \Delta t\), tripling the stopping time cuts the peak normal impact force transmitted up the tibia and knee joints by two-thirds.
3. Pinball Plunger Hooke's Law Launch (6 pts)
Exemplar Answer: By Hooke's Law (\(F_s = k\Delta x\)), pulling the plunger \(4\text{ cm}\) instead of \(2\text{ cm}\) doubles the compression distance, thereby doubling the launch restoring force. By Newton's Second Law (\(a = F/m\)), doubling the net force doubles the initial acceleration of the steel ball.
Grading Rubric Summary (50 Points Total)
Pre-Lab CFUs
10 pts
2 questions @ 5 pts
Station 1 Data
8 pts
Drops & sound notes
Station 2 Data
8 pts
Hooke's \(k\) calculation
Stations 3 & 4
16 pts
Friction & Buoyancy
Synthesis
8 pts
Safety engineering
Physics Dynamics • Contact Forces Lab Answer Key
Page 4 of 4 • Synthesis Solutions (12pt Edition)
Tipo de Superficie
Prueba 1 \(h_1\) (m)
Prueba 2 \(h_1\) (m)
Rebote Promedio (m)
¿Deformación Visible?
Sonido de Impacto
Mesa Dura / Baldosa
Pelota se aplasta
Seco y fuerte
Espuma Suave / Toalla
Espuma se hunde
Apagado y suave
Pregunta de la Estación 1: ¿Por qué la espuma hace que el rebote sea más bajo y silencioso que en la mesa dura?
Estación 2
Ley de Hooke: Estiramiento de Resorte (\(F_s = k\Delta x\))
\(g = 9.8\text{ m/s}^2\)
Cuelga masas crecientes del resorte. Mide la posición inicial \(x_0\) y estirada \(x\) para calcular la elongación \(\Delta x = x - x_0\).
Prueba
Masa Colgada \(m\) (kg)
Fuerza de Peso \(mg\) (N)
Estiramiento \(\Delta x\) (m)
Constante \(k = F/\Delta x\) (N/m)
1
0.100 kg
0.98 N
2
0.200 kg
1.96 N
3
0.300 kg
2.94 N
Pregunta de la Estación 2: Al duplicar el peso colgado de \(0.100\text{ kg}\) a \(0.200\text{ kg}\), ¿se duplicó también el estiramiento? ¿Qué nos indica esto sobre el resorte?
Física Dinámica • Laboratorio de Fuerzas de Contacto
Página 2 de 4 • Estaciones 1 y 2 (12pt)
Página 3 Datos: Estación 3 y Estación 4
Nombre del Estudiante:
Estación 3
Fricción: Iniciar el Movimiento vs. Deslizar
Tirón con dinamómetro
Tira del bloque de madera en distintas superficies. Registra la fuerza máxima para empezar a moverlo (fricción estática \(f_s\)) y la fuerza constante para mantenerlo deslizándose (\(f_k\)).
Superficie
Fuerza Normal \(F_N\) (N)
Fuerza para Iniciar \(f_s\) (N)
Fuerza para Deslizar \(f_k\) (N)
¿Es \(f_s > f_k\)?
Madera sobre Mesa
SÍ / NO
Madera sobre Lija
SÍ / NO
Madera sobre Papel Encerado
SÍ / NO
Pregunta de la Estación 3: ¿Por qué se requiere más fuerza para poner el bloque en movimiento que para mantenerlo deslizándose?
Estación 4
Flotabilidad: El Empuje del Agua (Arquímedes)
\(F_B = F_{\text{aire}} - F_{\text{sum}}\)
Pesa el bloque de metal en el aire. Sumérgelo en el vaso de desbordamiento, anota el nuevo peso en el agua y pesa el agua desbordada que cae en el vaso receptor.
Objeto Sumergido
Peso en el Aire (N)
Peso en el Agua (N)
Empuje del Agua \(F_B\) (N)
Peso del Agua Desbordada (N)
Bloque Metálico Pesado
Pregunta de la Estación 4: ¿Cómo se compara el empuje hacia arriba del agua (\(F_B\)) con el peso del agua que se desbordó?
Física Dinámica • Laboratorio de Fuerzas de Contacto
Página 3 de 4 • Estaciones 3 y 4 (12pt)
Página 4 Síntesis y Aplicaciones en el Mundo Real
Nombre del Estudiante:
Síntesis
Conexión de los Resultados con el Mundo Real
1. Zonas de Deformación en Autos: Los autos antiguos tenían parachoques de acero rígido, mientras que los modernos tienen frentes que se arrugan y colapsan en un choque. Con base en lo observado en la Estación 1 (superficies duras vs. blandas), ¿por qué las zonas de deformación protegen mucho mejor a los pasajeros?
2. Zapatillas Deportivas y Rodillas: Las zapatillas de correr tienen suelas gruesas de espuma flexible. Usando los conceptos de fuerza normal y tiempo de contacto, explica cómo la suela protege las articulaciones y los huesos al saltar o correr sobre pavimento.
3. Lanzador de Pinball: En una máquina de pinball se jala un resorte para lanzar una bola de acero. Usando la Ley de Hooke de la Estación 2, explica qué sucede con la fuerza de empuje y la aceleración de la bola si jalas el resorte \(4\text{ cm}\) en lugar de \(2\text{ cm}\).
Gran Conclusión de la Física
Todas las fuerzas de contacto (fuerza normal, fricción, resortes y choques) provienen de átomos que se empujan, jalan o deslizan entre sí. Cuando una superficie puede deformarse o amortiguar, el tiempo de contacto aumenta y la fuerza máxima de impacto disminuye notablemente.
Física Dinámica • Laboratorio de Fuerzas de Contacto
Página 4 de 4 • Síntesis (12pt)
Datos (G)
Incógnita (U)
Ecuación (E)
Sustituir (S)
Resolver (S)
Problema 6 Equilibrio con Fricción Estática Vertical
TEKS 5D
Un libro de física con masa \(m = 1.50\text{ kg}\) se sostiene contra una pared vertical. El coeficiente estático es \(\mu_s = 0.40\). Calcula la fuerza de empuje horizontal mínima (\(F_{empuje}\)) para evitar que resbale hacia abajo.
Datos (G)
Incógnita (U)
Ecuación (E)
Sustituir (S)
Resolver (S)
Física Dinámica • Hoja de Trabajo de Fuerzas Fundamentales
Página 2 de 3 • Cálculos con GUESS (12pt)
Bloque 6 Evaluación y Síntesis de Modelos
Nombre del Estudiante:
Parte 3
Puntos de Verificación Conceptual
7. Una caja de madera descansa sin moverse en el suelo. ¿Qué describe las fuerzas de contacto?
A. El suelo no puede empujar hacia arriba porque es inanimado.
B. La fuerza normal equilibra el peso; la fricción estática es cero hasta empujar.
C. La fricción estática empuja hacia arriba contra la gravedad.
D. La fricción cinética evita que la caja se hunda en el suelo.
8. Se suelta un resorte comprimido una distancia \(\Delta x\). ¿Qué describe la fuerza mientras se expande?
A. La fuerza permanece constante hasta que la bola se separa.
B. La fuerza aumenta continuamente conforme se descomprime.
C. La fuerza disminuye linealmente hasta cero en el equilibrio.
D. La fuerza invierte su sentido y hala la bola hacia atrás.
Parte 4
Matemáticas: Valor Absoluto y Tolerancia de Fuerza
TEKS 5D
En ingeniería, la tolerancia mide la desviación máxima permitida respecto a una fuerza objetivo: \(|F_{\text{real}} - F_{\text{objetivo}}| \le \text{Tolerancia}\).
Un resorte de pinball debe ejercer una fuerza de \(50.0\text{ N}\) con una tolerancia de \(\pm 4.0\text{ N}\). Escribe la desigualdad con valor absoluto y calcula el rango aceptable de fuerzas.
Parte 5
Síntesis: Aceleración en el Lanzador de Pinball
Síntesis Newtoniana
Cuando el émbolo del pinball se comprime \(3.0\text{ cm}\) y se suelta, ¿experimenta la bola una aceleración constante o aceleración cambiante durante el lanzamiento? Usa la Segunda Ley de Newton (\(a = F_{net}/m\)) y la Ley de Hooke (\(F_s = k\Delta x\)) para fundamentar tu respuesta.
Física Dinámica • Hoja de Trabajo de Fuerzas Fundamentales