Examen de Física II URV 2024 · Exámenes de : Teoría y Laboratorio (Mayo 2024)

Examen de Física II de la URV (Grado en Química) 2024, Exámenes de : Teoría y Laboratorio (Mayo 2024): 15 problemas con solución. Con corrección al momento.

Temas del examen: Oscillations: simple harmonic, damped and forced · Work, mechanical energy and potential energy curves · Electrostatics: Coulomb, electric field, Gauss's law and potential · Direct current circuits · Laboratory: measurement, errors, elasticity and fluids

Ejercicio Lab 1 · Laboratory: measurement, errors, elasticity and fluids

Lab 1. Calculation of errors

Explain how the volume resolution error would change if all length dimensions were determined solely by using a caliper instead of other instruments. Compute the quantitative magnitude of this change using your experimental laboratory data. Would the random error be affected as well? Justify your answer.

Ejercicio Lab 2 · Oscillations: simple harmonic, damped and forced

Lab 2. Elasticity of a spring and Hooke's law

A force of 20 N20\text{ N} is applied to a system of two springs coupled in series, causing the assembly to stretch by 10 cm10\text{ cm}.

a)

Determine the equivalent elastic constant of this spring system.

b)

Assuming the spring constant of the first spring is half that of the second spring, find the individual elastic constant of each spring.

Ejercicio Lab 3 · Oscillations: simple harmonic, damped and forced

Lab 3. Mechanical resonance in elongation

In the laboratory experiment on mechanical resonance, two contact forces act directly upon the oscillating mass: the elastic restoring force of the spring and the viscous damping force of the immersion fluid. The driving motor does not act directly on the suspended mass. How does the action of the motor turn into a driving resonant force governing the motion of the mass?

Ejercicio Exercise 1 · Oscillations: simple harmonic, damped and forced

Exercise 1 (10 points). Bungee jumper oscillation

An individual of mass m=60 kgm = 60\text{ kg} leaps from a bridge situated at a height h=100 mh = 100\text{ m} above the ground, secured to an elastic rope of natural length L0=20 mL_0 = 20\text{ m} and spring constant kk. The jumper experiences free fall until the rope reaches its unstretched length. Beyond this point, the cord stretches and applies an upward force that decelerates the jumper until he momentarily halts and rebounds into oscillatory motion. Assume air resistance and the mass of the rope are negligible (g=9.8 m/s2g = 9.8\text{ m/s}^2).

a.

Calculate the spring constant kk required so that the jumper stops (v=0v = 0) just before reaching the ground. [2 points]

b.

Determine the maximum elongation of this same rope if a second jumper of mass m2=90 kgm_2 = 90\text{ kg} performs the jump. [2 points]

c.

Compute the speed of this second jumper when reaching the ground level. [2 points]

d.

Establish the differential equation and solve for the equation of motion x(t)x(t) of this second jumper once the rope begins to stretch, setting x(0)=0x(0) = 0 at the moment the rope starts extending. [4 points]

Ejercicio Exercise 2 · Direct current circuits

Exercise 2 (10 points). DC circuit analysis

Consider three identical DC generators, each having an electromotive force E=9 V\mathcal{E} = 9\text{ V} and an internal resistance r=1 Ωr = 1\ \Omega.

a.

Calculate the equivalent electromotive force and internal resistance if all three generators are connected: (i) in series, and (ii) in parallel. [3 points]

b.

If the three generators are interconnected in the circuit shown in the diagram, compute the intensity of current flowing through each element in the steady state (taking R1,R2,R3R_1, R_2, R_3 as the branch resistances). [3.5 points]

c.

Assuming the capacitor in the middle branch has a capacitance of C=2 μFC = 2\ \mu\text{F}, determine the electric charge accumulated on its plates in terms of the voltage ∣VC∣|V_C| across it. [3.5 points]

Question 1 · Work, mechanical energy and potential energy curves

Question 1 (5 points). Morse potential

A widely used model for describing the vibrational motion of diatomic molecules is the Morse potential. In a specific dimensionless one-dimensional formulation, the potential energy is given by:

V(x)=e−2x−2e−xV(x) = e^{-2x} - 2e^{-x}

Analyze and discuss the dynamics of a particle moving in this potential field if its total mechanical energy is E=−0.5 JE = -0.5\text{ J}.

1.

Position xmin⁡x_{\min} and value Vmin⁡V_{\min} of the potential energy minimum:

2.

For E=−0.5 JE = -0.5\text{ J}, calculate the inner (x1x_1) and outer (x2x_2) classical turning points, and the maximum kinetic energy Kmax⁡K_{\max}:

3.

Characterize the nature of the motion for E=−0.5 JE = -0.5\text{ J} (e.g. bounded vs unbounded, type of motion):

Question 2 · Electrostatics: Coulomb, electric field, Gauss's law and potential

Question 2 (5 points). Electrostatic work

A point charge Q=+5 nCQ = +5\text{ nC} is located at the origin of coordinates (0,0)(0, 0).

a.

Determine the energy required to bring a test charge q=+1 nCq = +1\text{ nC} from infinity to point A(3 m,4 m)A(3\text{ m}, 4\text{ m}).

b.

If the charge qq is subsequently displaced from point A(3 m,4 m)A(3\text{ m}, 4\text{ m}) to point B(4 m,3 m)B(4\text{ m}, 3\text{ m}), what is the amount of work required to perform this second displacement?

Ejercicio Simulation 1 · Electrostatics: Coulomb, electric field, Gauss's law and potential

Simulation 1. Electric field and potential of a +1 μC charge

In the electrostatic field simulation, clear the workspace and place a single point charge q=+1 μCq = +1\,\mu\text{C} at the origin (0,0)(0, 0). Activate the display of electric field vectors and equipotential lines.

a.

Record the potential VV, field magnitude EE, components Ex,EyE_x, E_y, and angle α\alpha measured at position (100 m,100 m)(100\text{ m}, 100\text{ m}).

V

N/C

N/C

N/C

°

b.

Record the same quantities at position (100 m,−100 m)(100\text{ m}, -100\text{ m}).

V

N/C

N/C

N/C

°

c.

Verify these experimental simulation values against theoretical calculations applying the formulas for a point charge:

E⃗=14πε0qr2u^r,V=14πε0qr\vec{E} = \frac{1}{4\pi\varepsilon_0} \frac{q}{r^2}\hat{u}_r, \quad V = \frac{1}{4\pi\varepsilon_0} \frac{q}{r}

Ejercicio Simulation 2 · Electrostatics: Coulomb, electric field, Gauss's law and potential

Simulation 2. Electric field and potential of a -1 μC charge

Place a charge q=−1 μCq = -1\,\mu\text{C} at the origin (0,0)(0, 0) and repeat the measurements of point 1 at (100 m,100 m)(100\text{ m}, 100\text{ m}) and (100 m,−100 m)(100\text{ m}, -100\text{ m}). Compare the outcomes with the positive charge case: what differences are observed?

1.

Measurements at position (100 m,100 m)(100\text{ m}, 100\text{ m}):

V

N/C

N/C

N/C

°

2.

Measurements at position (100 m,−100 m)(100\text{ m}, -100\text{ m}):

V

N/C

N/C

N/C

°

3.

Compare the outcomes with the positive charge case: what differences are observed?

Ejercicio Simulation 3 · Electrostatics: Coulomb, electric field, Gauss's law and potential

Simulation 3. Electric field and potential of a charge dipole (+2 μC and -2 μC)

Clear the workspace and place a charge q1=+2 μCq_1 = +2\,\mu\text{C} at (−100 m,0)(-100\text{ m}, 0) and a charge q2=−2 μCq_2 = -2\,\mu\text{C} at (100 m,0)(100\text{ m}, 0). Observe the field vectors, field lines, and equipotential curves. Record the electric potential VV, field module EE, vector components Ex,EyE_x, E_y, and angle α\alpha at the following positions:

a.

(−100 m,0)(-100\text{ m}, 0) (near the positive charge, e.g. at (−100 m,−1 m)(-100\text{ m}, -1\text{ m})):

V

N/C

N/C

N/C

°

b.

(0,0)(0, 0):

V

N/C

N/C

N/C

°

c.

(−150 m,0)(-150\text{ m}, 0):

V

N/C

N/C

N/C

°

d.

(0,150 m)(0, 150\text{ m}):

V

N/C

N/C

N/C

°

e.

(−150 m,150 m)(-150\text{ m}, 150\text{ m}):

V

N/C

N/C

N/C

°

Ejercicio Simulation 4 · Electrostatics: Coulomb, electric field, Gauss's law and potential

Lab 6. Numerical simulation of central forces

A point charge q1=−4 μCq_1 = -4\ \mu\text{C} is located at the origin (0,0)(0, 0), and a second point charge q2=+2 μCq_2 = +2\ \mu\text{C} is located at (200 m,200 m)(200\text{ m}, 200\text{ m}).

Simulation 4. Electric field and potential of a three-charge configuration

Reset the simulation screen and configure three point charges: q1=+4 μCq_1 = +4\ \mu\text{C} at (0,0)(0, 0), q2=−2 μCq_2 = -2\ \mu\text{C} at (0,−100 m)(0, -100\text{ m}), and q3=−2 μCq_3 = -2\ \mu\text{C} at (0,100 m)(0, 100\text{ m}). Inspect the field lines and equipotential patterns, and record the potential and electric field vector at:

a)

At (150 m,0)(150\text{ m}, 0):

V

N/C

b)

At (0,150 m)(0, 150\text{ m}):

V

N/C

c)

At (−150 m,150 m)(-150\text{ m}, 150\text{ m}):

V

N/C

d)

At (200 m,0)(200\text{ m}, 0):

V

N/C

Ejercicio Lab 4 · Laboratory: measurement, errors, elasticity and fluids

Lab 6. Numerical simulation of central forces

A point charge q1=−4 μCq_1 = -4\ \mu\text{C} is located at the origin (0,0)(0, 0), and a second point charge q2=+2 μCq_2 = +2\ \mu\text{C} is located at (200 m,200 m)(200\text{ m}, 200\text{ m}).

Lab 4. Determination of the center of gravity

Theoretically evaluate the coordinates of the center of gravity of the flat, homogeneous plate shown in the figure below. Take the origin of coordinates at point A(0,0)A(0, 0).

The outer dimensions are 10 cm×10 cm10\text{ cm} \times 10\text{ cm}. A square central section is cut out from the top edge, leaving two vertical side arms of width 3 cm3\text{ cm} each, and a bottom horizontal bar of height 3 cm3\text{ cm}.

a)

cm

b)

cm

Ejercicio Lab 5 · Laboratory: measurement, errors, elasticity and fluids

Lab 5. Measuring the density of liquids

To determine the density of an unknown liquid, a spherical metallic mass of diameter d=2.12 cmd = 2.12\text{ cm} is utilized. The measured mass of the sphere in air is mair=126.75 gm_{\text{air}} = 126.75\text{ g}, and its apparent mass when fully immersed in the liquid is mapp=122.18 gm_{\text{app}} = 122.18\text{ g}.

a)

What is the buoyant force exerted by the liquid on the immersed sphere?

b)

Calculate the density of the liquid.

Ejercicio Lab 6 · Electrostatics: Coulomb, electric field, Gauss's law and potential

Lab 6. Numerical simulation of central forces

A point charge q1=−4 μCq_1 = -4\ \mu\text{C} is located at the origin (0,0)(0, 0), and a second point charge q2=+2 μCq_2 = +2\ \mu\text{C} is located at (200 m,200 m)(200\text{ m}, 200\text{ m}).

a)

Calculate the magnitude and direction of the net electric field vector at point A(100 m,100 m)A(100\text{ m}, 100\text{ m}).

N/C

°

b)

Plot or sketch the resulting electric field vector at point AA.

Ejercicio Lab 7 · Direct current circuits

15. Lab 7. Association of resistances and Kirchhoff's laws

What was the experimental value of the galvanometer current IGI_G measured in your laboratory session? Under what circumstances can the condition IG=0 AI_G = 0\text{ A} occur? If this condition can be achieved, explain what circuit modifications or parameter settings must be made.

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