Herramienta pedag?gica para la ense?anza de las ciencias naturales

48 P?ginasRecurso Electr?nicoEl presente proyecto est? basado en la implementaci?n de una Herramienta Pedag?gica en el ?rea de las Ciencias Naturales en el grado s?ptimo (A, B y C) de la Instituci?n Escuela Normal Superior Santa Teresita. Esta instituci?n no cuenta con proyectos sobre las herramientas pedag?gicas, pero es de resaltar que la instituci?n es netamente pedag?gica y que se fundamenta en el pedagogo Celestin Freinet, el cual plantea el texto libre y la UAI. Teniendo en cuenta los Lineamientos curriculares, los cuales proponen ejes fundamentales como son los procesos de pensamiento y acci?n y conocimiento cient?fico b?sico, se realiza la Cartilla ?EXPLOREMOS 7?? ?La C?lula?, con el fin de que los estudiantes participen de un aprendizaje activo y significativo. Para la realizaci?n de este proyecto, las investigadoras se centraron en varios autores como Koock, Ville, Helena Curt?s, Sneider y Chowan, quienes dieron aportes significativos a esta tesis de grado. Con esta Herramienta Pedag?gica se busca mejorar los procesos de aprendizaje de los estudiantes, mejorando la actividad educativa evidenciando mediante la pr?ctica resultados positivos de aprendizaje.ABSTRACT. This project is based on the implementation of a Pedagogical Tool in the area of natural science in seventh grade (A, B and C) of the Superior Normal School Institution Theresa. This institution has no projects on educational tools, but it is noteworthy that the institution is purely educational and is based on the pedagogue Celestin Freinet, which raises the free text and IAU. Given the curriculum guidelines, which are proposed as the cornerstones of thought and action processes and basic scientific knowledge, the Primer is done "EXPLORATIONS 7th" "The Cell" in order to engage students in learning active and meaningful. For this project, the researchers focused on several authors as Koock, Ville, Helena Curtis, Sneider and Chowan, who gave significant contributions to this thesis. This pedagogical tool is to improve the learning processes of students, improving the educational activity showing positive results through practical learning.INTRODUCCI?N 11 1. MARCO CONTEXTUAL 12 2. ANTECEDENTES 13 3. FORMULACI?N DEL PROBLEMA 15 4. PREGUNTA PROBLEMATIZADORA 16 5. JUSTIFICACI?N 17 6. OBJETIVOS 18 6.1 OBJETIVO GENERAL 18 6.2 OBJETIVOS ESPEC?FICOS 18 7. MARCO TE?RICO 19 7.1 LEY GENERAL DE EDUCACI?N 19 7.2 LINEAMIENTOS Y EST?NDARES CURRICULARES 19 7.2.1 Procesos de pensamiento y acci?n grado s?ptimo 20 7.2.2 Conocimiento de procesos biol?gicos 20 7.3 CONSTRUCTIVISMO 21 7.4 DID?CTICA 21 7.5 ESTRATEGIA 22 7.6 ESTRATEGIAS DID?CTICAS 23 7.7 APRENDIZAJE SIGNIFICATIVO 23 7.8 ENSE?ANZA 26 7.9 PEDAGOG?AS ACTIVAS 26 7.10 CELESTIN FREINET 27 7.11 HELENA CURTIS 29 7.12 N. SUE BARNES 30 7.13 ADRIANA SCHNEK 30 8. DISE?O METODOL?GICO 31 8.1 TIPO DE INVESTIGACI?N 31 8.2 FASES DE LA INVESTIGACI?N 32 8.3 POBLACI?N 33 8.4 MUESTRA 33 8.5 CATEGOR?AS 33 8.6 INSTRUMENTOS PARA LA RECOLECCI?N DE INFORMACI?N 33 8.6.1 Observaci?n participativa 34 8.6.2 Taller 34 9. CRONOGRAMA DE ACTIVIDADES 35 10. AN?LISIS DE RESULTADOS 36 10.1 PRE-T?S TALLER DE DIAGN?STICO 36 10.2 POST-TEST. PRUEBA FINAL 37 10.3 AN?LISIS COMPARATIVO 39 10.3.1 Diferencias de la c?lula animal y la c?lula vegetal 39 10.3.2 Funciones de la c?lula animal y vegetal 39 11. CONCLUSIONES 41 RECOMENDACIONES 42 REFERENCIAS 43 ANEXOS 4

Herramienta pedag?gica para la ense?anza de las ciencias naturales

48 p. Recurso Electr?nicoEl presente proyecto est? basado en la implementaci?n de una Herramienta Pedag?gica en el ?rea de las Ciencias Naturales en el grado s?ptimo (A, B y C) de la Instituci?n Escuela Normal Superior Santa Teresita. Esta instituci?n no cuenta con proyectos sobre las herramientas pedag?gicas, pero es de resaltar que la instituci?n es netamente pedag?gica y que se fundamenta en el pedagogo Celestin Freinet, el cual plantea el texto libre y la UAI. Teniendo en cuenta los Lineamientos curriculares, los cuales proponen ejes fundamentales como son los procesos de pensamiento y acci?n y conocimiento cient?fico b?sico, se realiza la Cartilla ?EXPLOREMOS 7?? ?La C?lula?, con el fin de que los estudiantes participen de un aprendizaje activo y significativo. Para la realizaci?n de este proyecto, las investigadoras se centraron en varios autores como Koock, Ville, Helena Curt?s, Sneider y Chowan, quienes dieron aportes significativos a esta tesis de grado. Con esta Herramienta Pedag?gica se busca mejorar los procesos de aprendizaje de los estudiantes, mejorando la actividad educativa evidenciando mediante la pr?ctica resultados positivos de aprendizaje. Palabras claves: Procesos, herramientas, pedagogos, ense?anza-aprendizaje, estudiantes, tesis, pedagog?a activa, instituci?n educativa, cartilla, formaci?n.This project is based on the implementation of a Pedagogical Tool in the area of natural science in seventh grade (A, B and C) of the Superior Normal School Institution Theresa. This institution has no projects on educational tools, but it is noteworthy that the institution is purely educational and is based on the pedagogue Celestin Freinet, which raises the free text and IAU. Given the curriculum guidelines, which are proposed as the cornerstones of thought and action processes and basic scientific knowledge, the Primer is done "EXPLORATIONS 7th" "The Cell" in order to engage students in learning active and meaningful. For this project, the researchers focused on several authors as Koock, Ville, Helena Curtis, Sneider and Chowan, who gave significant contributions to this thesis. This pedagogical tool is to improve the learning processes of students, improving the educational activity showing positive results through practical learning. Keywords: Processes, tools, teachers, teaching and learning, students, thesis, active pedagogy, educational institution, primer, training

Development of the CMS detector for the CERN LHC Run 3

International audienceSince the initial data taking of the CERN LHC, the CMS experiment has undergone substantial upgrades and improvements. This paper discusses the CMS detector as it is configured for the third data-taking period of the CERN LHC, Run 3, which started in 2022. The entire silicon pixel tracking detector was replaced. A new powering system for the superconducting solenoid was installed. The electronics of the hadron calorimeter was upgraded. All the muon electronic systems were upgraded, and new muon detector stations were added, including a gas electron multiplier detector. The precision proton spectrometer was upgraded. The dedicated luminosity detectors and the beam loss monitor were refurbished. Substantial improvements to the trigger, data acquisition, software, and computing systems were also implemented, including a new hybrid CPU/GPU farm for the high-level trigger

Development of the CMS detector for the CERN LHC Run 3

International audienceSince the initial data taking of the CERN LHC, the CMS experiment has undergone substantial upgrades and improvements. This paper discusses the CMS detector as it is configured for the third data-taking period of the CERN LHC, Run 3, which started in 2022. The entire silicon pixel tracking detector was replaced. A new powering system for the superconducting solenoid was installed. The electronics of the hadron calorimeter was upgraded. All the muon electronic systems were upgraded, and new muon detector stations were added, including a gas electron multiplier detector. The precision proton spectrometer was upgraded. The dedicated luminosity detectors and the beam loss monitor were refurbished. Substantial improvements to the trigger, data acquisition, software, and computing systems were also implemented, including a new hybrid CPU/GPU farm for the high-level trigger

Development of the CMS detector for the CERN LHC Run 3

International audienceSince the initial data taking of the CERN LHC, the CMS experiment has undergone substantial upgrades and improvements. This paper discusses the CMS detector as it is configured for the third data-taking period of the CERN LHC, Run 3, which started in 2022. The entire silicon pixel tracking detector was replaced. A new powering system for the superconducting solenoid was installed. The electronics of the hadron calorimeter was upgraded. All the muon electronic systems were upgraded, and new muon detector stations were added, including a gas electron multiplier detector. The precision proton spectrometer was upgraded. The dedicated luminosity detectors and the beam loss monitor were refurbished. Substantial improvements to the trigger, data acquisition, software, and computing systems were also implemented, including a new hybrid CPU/GPU farm for the high-level trigger

Development of the CMS detector for the CERN LHC Run 3

Since the initial data taking of the CERN LHC, the CMS experiment has undergone substantial upgrades and improvements. This paper discusses the CMS detector as it is configured for the third data-taking period of the CERN LHC, Run 3, which started in 2022. The entire silicon pixel tracking detector was replaced. A new powering system for the superconducting solenoid was installed. The electronics of the hadron calorimeter was upgraded. All the muon electronic systems were upgraded, and new muon detector stations were added, including a gas electron multiplier detector. The precision proton spectrometer was upgraded. The dedicated luminosity detectors and the beam loss monitor were refurbished. Substantial improvements to the trigger, data acquisition, software, and computing systems were also implemented, including a new hybrid CPU/GPU farm for the high-level trigger.Since the initial data taking of the CERN LHC, the CMS experiment has undergone substantial upgrades and improvements. This paper discusses the CMS detector as it is configured for the third data-taking period of the CERN LHC, Run 3, which started in 2022. The entire silicon pixel tracking detector was replaced. A new powering system for the superconducting solenoid was installed. The electronics of the hadron calorimeter was upgraded. All the muon electronic systems were upgraded, and new muon detector stations were added, including a gas electron multiplier detector. The precision proton spectrometer was upgraded. The dedicated luminosity detectors and the beam loss monitor were refurbished. Substantial improvements to the trigger, data acquisition, software, and computing systems were also implemented, including a new hybrid CPU/GPU farm for the high-level trigger

Development of the CMS detector for the CERN LHC Run 3

International audienceSince the initial data taking of the CERN LHC, the CMS experiment has undergone substantial upgrades and improvements. This paper discusses the CMS detector as it is configured for the third data-taking period of the CERN LHC, Run 3, which started in 2022. The entire silicon pixel tracking detector was replaced. A new powering system for the superconducting solenoid was installed. The electronics of the hadron calorimeter was upgraded. All the muon electronic systems were upgraded, and new muon detector stations were added, including a gas electron multiplier detector. The precision proton spectrometer was upgraded. The dedicated luminosity detectors and the beam loss monitor were refurbished. Substantial improvements to the trigger, data acquisition, software, and computing systems were also implemented, including a new hybrid CPU/GPU farm for the high-level trigger

Development of the CMS detector for the CERN LHC Run 3

Since the initial data taking of the CERN LHC, the CMS experiment has undergone substantial upgrades and improvements. This paper discusses the CMS detector as it is configured for the third data-taking period of the CERN LHC, Run 3, which started in 2022. The entire silicon pixel tracking detector was replaced. A new powering system for the superconducting solenoid was installed. The electronics of the hadron calorimeter was upgraded. All the muon electronic systems were upgraded, and new muon detector stations were added, including a gas electron multiplier detector. The precision proton spectrometer was upgraded. The dedicated luminosity detectors and the beam loss monitor were refurbished. Substantial improvements to the trigger, data acquisition, software, and computing systems were also implemented, including a new hybrid CPU/GPU farm for the high-level trigger

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s= \sqrt{s} = 5.02 TeV

The inclusive jet cross section is measured as a function of jet transverse momentum $p_{\mathrm{T}}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} =$ 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4$\,\text{pb}^{-1}$. The jets are reconstructed with the anti-$k_{\mathrm{T}}$ algorithm using a distance parameter of $R=$ 0.4, within the rapidity interval $|y| <$ 2, and across the kinematic range 0.06 $< p_{\mathrm{T}} <$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$.The inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$