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PDF</button><button class="ds2-5-button ds2-5-button--secondary js-swp-download-button" data-signup-modal="{"location":"download-pdf-button--work-card","attachmentId":44974664,"attachmentType":"pdf","workUrl":"https://www.academia.edu/24647465/EQUILIBRIO_DE_FUERZAS_CONCURRENTES"}"><span class="material-symbols-outlined" style="font-size: 20px" translate="no">download</span>Download PDF</button></div></div></div></div><div data-auto_select="false" data-client_id="331998490334-rsn3chp12mbkiqhl6e7lu2q0mlbu0f1b" data-doc_id="44974664" data-landing_url="https://www.academia.edu/24647465/EQUILIBRIO_DE_FUERZAS_CONCURRENTES" data-login_uri="https://www.academia.edu/registrations/google_one_tap" data-moment_callback="onGoogleOneTapEvent" id="g_id_onload"></div><div class="ds-top-related-works--grid-container"><div class="ds-related-content--container ds-top-related-works--container"><h2 class="ds-related-content--heading">Related papers</h2><div class="ds-related-work--container js-wsj-grid-card" data-collection-position="0" data-entity-id="40692470" data-sort-order="default"><a class="ds-related-work--title js-wsj-grid-card-title ds2-5-body-md ds2-5-body-link" href="https://www.academia.edu/40692470/FUERZAS_CONCURRENTES">FUERZAS CONCURRENTES</a><div class="ds-related-work--metadata"><a class="js-wsj-grid-card-author ds2-5-body-sm ds2-5-body-link" data-author-id="132039748" href="https://uniatlantico.academia.edu/JULIOCESARCANCIOPADILLA">JULIO CESAR CANCIO PADILLA</a></div><p class="ds-related-work--abstract ds2-5-body-sm">Resumen En el presente laboratorio se pudo estudiar la fuerza, donde se conoce como la mag-nitud vectorial de cualquier acción que pueda alterar el estado de reposo de cualquier cuerpo. Ahora bien, en un sistema de fuerzas concurrentes es donde existe un punto en común para todas las rectas de las fuerzas que compone el sistema. Para esto, to-das las fuerzas se pueden descomponer en un plano xy, donde el punto de origen será el punto donde las fuerzas se intersecan y así conocer las fuerza resultante o vicever-sa, conocemos la resultante y podemos hallar sus componentes en x y en y. Este sis-tema al encontrarse en equilibrios, la sumatoria de las fuerzas debe ser igual a 0. Abstract In this laboratory the force can be studied, where it is known as the vectorial magnitude of any action that may alter the state of rest of any body. Now, in a system of concurrent forces there is a common point for all the straight lines of forces that make up the system. For this, all forces can be decomposed into a xy plane, where the point of origin will be the point where the forces intersect and so know the resulting force or vice versa, We know the resulting and we can find its components in x and y. This system when found in balances, the sum of forces must be equal to 0. Introducción: Dentro de las magnitudes más importantes que encontramos en física se encuentra el vector. Un vector es un segmento de recta con origen en un punto del espacio y que sirve para representar magnitudes que tie-nen una dirección y un sentido (por lo cual se llaman magnitudes vectoriales). La ve-locidad y la fuerza son dos ejemplos de magnitudes vectoriales; como hablamos de magnitud, significa que tiene un tama-ño, el cual llamaremos módulo, entonces un vector tiene módulo (su tamaño), di-rección y sentido. Es común que un cuer-po esté siempre sometido a la acción de dos o más fuerzas. Decimos que dos o más</p><div class="ds-related-work--ctas"><button class="ds2-5-text-link ds2-5-text-link--inline js-swp-download-button" data-signup-modal="{"location":"wsj-grid-card-download-pdf-modal","work_title":"FUERZAS CONCURRENTES","attachmentId":60976344,"attachmentType":"pdf","work_url":"https://www.academia.edu/40692470/FUERZAS_CONCURRENTES","alternativeTracking":true}"><span class="material-symbols-outlined" style="font-size: 18px" translate="no">download</span><span class="ds2-5-text-link__content">Download free PDF</span></button><a class="ds2-5-text-link ds2-5-text-link--inline js-wsj-grid-card-view-pdf" href="https://www.academia.edu/40692470/FUERZAS_CONCURRENTES"><span class="ds2-5-text-link__content">View PDF</span><span class="material-symbols-outlined" style="font-size: 18px" translate="no">chevron_right</span></a></div></div><div class="ds-related-work--container js-wsj-grid-card" data-collection-position="1" data-entity-id="29808812" data-sort-order="default"><a class="ds-related-work--title js-wsj-grid-card-title ds2-5-body-md ds2-5-body-link" href="https://www.academia.edu/29808812/FUERZAS_EN_EQUILIBRIO">FUERZAS EN EQUILIBRIO</a><div class="ds-related-work--metadata"><a class="js-wsj-grid-card-author ds2-5-body-sm ds2-5-body-link" data-author-id="56526245" href="https://independent.academia.edu/OliviaEstrada3">Olivia Estrada</a></div><p class="ds-related-work--abstract ds2-5-body-sm">Determinar las condiciones del equilibrio estático de las fuerzas.</p><div class="ds-related-work--ctas"><button class="ds2-5-text-link ds2-5-text-link--inline js-swp-download-button" data-signup-modal="{"location":"wsj-grid-card-download-pdf-modal","work_title":"FUERZAS EN EQUILIBRIO","attachmentId":50271189,"attachmentType":"doc","work_url":"https://www.academia.edu/29808812/FUERZAS_EN_EQUILIBRIO","alternativeTracking":true}"><span class="material-symbols-outlined" style="font-size: 18px" translate="no">download</span><span class="ds2-5-text-link__content">Download free PDF</span></button><a class="ds2-5-text-link ds2-5-text-link--inline js-wsj-grid-card-view-pdf" href="https://www.academia.edu/29808812/FUERZAS_EN_EQUILIBRIO"><span class="ds2-5-text-link__content">View PDF</span><span class="material-symbols-outlined" style="font-size: 18px" translate="no">chevron_right</span></a></div></div><div class="ds-related-work--container js-wsj-grid-card" data-collection-position="2" data-entity-id="29242489" data-sort-order="default"><a class="ds-related-work--title js-wsj-grid-card-title ds2-5-body-md ds2-5-body-link" href="https://www.academia.edu/29242489/L2_FUERZAS_CONCURRENTES">L2 FUERZAS CONCURRENTES</a><div class="ds-related-work--metadata"><a class="js-wsj-grid-card-author ds2-5-body-sm ds2-5-body-link" data-author-id="55220329" href="https://independent.academia.edu/JoegeRivas">Joege Rivas</a></div><p class="ds-related-work--abstract ds2-5-body-sm">INTRODUCCIÓN: Por todos es sabido, acerca de la gran importancia que tienen los vectores dentro de la física no solo como modelo matemático sino también como una herramienta que permitió cuantificar muchos fenómenos físicos. Las fuerzas concurrentes son dos o más fuerzas aplicadas sobre un mismo objeto. Si el resultado de todas ellas es cero, el sistema está equilibrado y no le afectará la presencia de otras fuerzas. La representación será a base de vectores que son dibujados mediante flechas. OBJETIVOS • Determinar experimentalmente el vector resultante en la suma de varias fuerzas coplanares cuyas líneas de acción pasan por un mismo punto. • Analizar algunos métodos gráficos para la adición de vectores. • Interpretar la precisión de una " mesa de fuerzas " EQUIPO • Mesa de fuerzas. • 4 poleas, 4 Portapesas, Hilo fino • 4 Juego de pesas de 10,2 0,50 y 100 gramos • Argolla, Nivel, Lanilla. • 3 hojas de papel milimetrado (No es suministrado por el laboratorio) MARCO TEÓRICO Concepto de dirección vectorial Los ejes de coordenadas, X, Y, se utilizan como sistema de referencia para trazar gráficas, como se muestra en la Figura 1. Una recta orientada o eje define una dirección y un sentido. Las rectas paralelas orientadas en el mismo sentido definen la misma dirección, pero si poseen orientaciones opuestas, definen direcciones opuestas, Figura 2. En un plano, una dirección está determinada por el ángulo que se forma entre una dirección y un sentido de referencia (o eje) y la dirección que se desea indicar, medido en sentido levógiro (positivo), o contrario al movimiento de las manecillas de un reloj. Las direcciones opuestas están determinadas por los ángulos θ y π + θ (o 180° + θ), Figura 3. Escalares y vectores Muchas magnitudes físicas están determinadas completamente por un número real, su valor numérico, expresado en unidades adecuadas. A estas magnitudes se les llama escalares. Volumen, temperatura, tiempo, masa, carga y energía son magnitudes escalares. Otras magnitudes requieren para su completa determinación, además de su valor numérico, una dirección. Éstas se conocen como vectores. El vector más evidente es el desplazamiento. El desplazamiento de un cuerpo está determinado por la distancia que se ha movido en línea recta y la dirección en que lo hace, esto es, por el vector AB (Figura 4). Velocidad, aceleración y fuerza son magnitudes vectoriales. Los vectores se representan gráficamente mediante segmentos de recta que tienen la misma dirección que el vector (indicada con una flecha) cuya longitud es proporcional a su módulo. Se les denota como V v , mientras que el módulo se denota con la letra en cursivas solamente, V. Un vector unitario es aquel cuyo módulo es la unidad. El vector V v paralelo al vector unitario u ˆ se puede expresar en la forma V u V ˆ = r (1) Un vector negativo tiene el mismo módulo que su contraparte positiva y dirección opuesta. Figura 1 Figura 2 Figura 3 Figrua 4 Equilibrio de una partícula Cuando la fuerza resultante, suma de todas las fuerzas que actúan sobre una partícula (fuerzas concurrentes), es cero, la aceleración de la partícula también es cero. La partícula está es reposo o en movimiento uniforme, en este caso se dice que está en equilibrio. En general: ∑ = = + + + i i F F F 0 o 0 3 2 1 F r L r r r En términos de componentes rectangulares de las fuerzas, las condiciones de equilibrio se pueden expresar como ∑ ∑ ∑ = = = i iz i iy i ix 0 y 0 , 0 F F F</p><div class="ds-related-work--ctas"><button class="ds2-5-text-link ds2-5-text-link--inline js-swp-download-button" data-signup-modal="{"location":"wsj-grid-card-download-pdf-modal","work_title":"L2 FUERZAS CONCURRENTES","attachmentId":49692324,"attachmentType":"pdf","work_url":"https://www.academia.edu/29242489/L2_FUERZAS_CONCURRENTES","alternativeTracking":true}"><span class="material-symbols-outlined" style="font-size: 18px" translate="no">download</span><span class="ds2-5-text-link__content">Download free PDF</span></button><a class="ds2-5-text-link ds2-5-text-link--inline js-wsj-grid-card-view-pdf" href="https://www.academia.edu/29242489/L2_FUERZAS_CONCURRENTES"><span class="ds2-5-text-link__content">View PDF</span><span class="material-symbols-outlined" style="font-size: 18px" translate="no">chevron_right</span></a></div></div><div class="ds-related-work--container js-wsj-grid-card" data-collection-position="3" data-entity-id="31850370" data-sort-order="default"><a class="ds-related-work--title js-wsj-grid-card-title ds2-5-body-md ds2-5-body-link" href="https://www.academia.edu/31850370/FUERZAS_CONCURRENTES_CONCURRENT_FORCES">FUERZAS CONCURRENTES CONCURRENT FORCES</a><div class="ds-related-work--metadata"><a class="js-wsj-grid-card-author ds2-5-body-sm ds2-5-body-link" data-author-id="61466986" href="https://independent.academia.edu/JhonMarioRam%C3%ADrez">Jhon Mario Ramírez</a></div><p class="ds-related-work--abstract ds2-5-body-sm">RESUMEN El objetivo de este informe es demostrar que la fuerza resultante entre dos o más fuerzas de diferente magnitud, puede expresarse como una suma vectorial; dada por las componentes rectangulares de dichas fuerzas, con un ángulo de inclinación determinado, es decir, y. Partiendo de la teoría de que las fuerzas aplicadas a la mesa de fuerza, deben estar en equilibrio respecto al anillo que se encuentra en el centro de la mesa; pueden obtenerse los datos necesarios para obtener la fuerza resultante analíticamente. Gráficamente, usando papel milimetrado, se representaron cada una de las fuerzas obtenidas con en ángulo de inclinación obtenido. Ahora, el valor de dichas fuerzas, presentó ciertos errores de medición, propios de toda práctica de laboratorio; teniendo que cuenta que el error en el cálculo de las fuerzas no puede sobrepasar el 5%; se halló el error para cada una de las componentes de las fuerzas estudiadas, obteniendo 1.5% en promedio del error en las y el promedio del error en fue 1.39%. Palabras Clave. Fuerza Resultante, Componentes Rectangulares de una Fuerza. Error de medición. ABSTRACT The objective of this report is to demostrate that the resultant force between two or more forces of different scale can be expressed as a vector sum; given by the rectangular components of such forces, with a particular inclination angle, that is, and. On the basis of the theory that the forces applied to the table of force, must be in balance with respect to the ring in the center of the table; the data necessary to obtain the resultant force analytically can obtain. Graphically, using graph paper, depicted each obtained forces with retrieved inclination angle. Now, the value of such forces, presented certain errors of measurement, all laboratory practice; Bearing in mind that the error in the calculation of the forces may not exceed 5%; We found the error for each of the components of the forces studied, gaining 1.5% on average of the error in the and the average of the error in It was 1.39%.</p><div class="ds-related-work--ctas"><button class="ds2-5-text-link ds2-5-text-link--inline js-swp-download-button" data-signup-modal="{"location":"wsj-grid-card-download-pdf-modal","work_title":"FUERZAS CONCURRENTES CONCURRENT FORCES","attachmentId":52141368,"attachmentType":"doc","work_url":"https://www.academia.edu/31850370/FUERZAS_CONCURRENTES_CONCURRENT_FORCES","alternativeTracking":true}"><span class="material-symbols-outlined" style="font-size: 18px" translate="no">download</span><span class="ds2-5-text-link__content">Download free PDF</span></button><a class="ds2-5-text-link ds2-5-text-link--inline js-wsj-grid-card-view-pdf" href="https://www.academia.edu/31850370/FUERZAS_CONCURRENTES_CONCURRENT_FORCES"><span class="ds2-5-text-link__content">View PDF</span><span class="material-symbols-outlined" style="font-size: 18px" translate="no">chevron_right</span></a></div></div><div class="ds-related-work--container js-wsj-grid-card" data-collection-position="4" data-entity-id="14388893" data-sort-order="default"><a class="ds-related-work--title js-wsj-grid-card-title ds2-5-body-md ds2-5-body-link" href="https://www.academia.edu/14388893/EQUIPOS_DE_ARCO_SUMERGIDO">EQUIPOS DE ARCO SUMERGIDO</a><div class="ds-related-work--metadata"><a class="js-wsj-grid-card-author ds2-5-body-sm ds2-5-body-link" data-author-id="33332159" href="https://independent.academia.edu/luiscuba1">luis cuba</a></div><div class="ds-related-work--ctas"><button class="ds2-5-text-link ds2-5-text-link--inline js-swp-download-button" data-signup-modal="{"location":"wsj-grid-card-download-pdf-modal","work_title":"EQUIPOS DE ARCO SUMERGIDO","attachmentId":38291706,"attachmentType":"pdf","work_url":"https://www.academia.edu/14388893/EQUIPOS_DE_ARCO_SUMERGIDO","alternativeTracking":true}"><span class="material-symbols-outlined" style="font-size: 18px" translate="no">download</span><span class="ds2-5-text-link__content">Download free PDF</span></button><a class="ds2-5-text-link ds2-5-text-link--inline js-wsj-grid-card-view-pdf" href="https://www.academia.edu/14388893/EQUIPOS_DE_ARCO_SUMERGIDO"><span class="ds2-5-text-link__content">View PDF</span><span class="material-symbols-outlined" style="font-size: 18px" translate="no">chevron_right</span></a></div></div><div class="ds-related-work--container js-wsj-grid-card" data-collection-position="5" data-entity-id="25535866" data-sort-order="default"><a class="ds-related-work--title js-wsj-grid-card-title ds2-5-body-md ds2-5-body-link" href="https://www.academia.edu/25535866/LABORATORIO_N_4_FUERZAS_EN_EQUILIBRIO">LABORATORIO N° 4 FUERZAS EN EQUILIBRIO</a><div class="ds-related-work--metadata"><a class="js-wsj-grid-card-author ds2-5-body-sm ds2-5-body-link" data-author-id="49095656" href="https://independent.academia.edu/Seb%C3%A1stianValero">Sebástian Valero</a></div><div class="ds-related-work--ctas"><button class="ds2-5-text-link ds2-5-text-link--inline js-swp-download-button" data-signup-modal="{"location":"wsj-grid-card-download-pdf-modal","work_title":"LABORATORIO N° 4 FUERZAS EN EQUILIBRIO","attachmentId":45865989,"attachmentType":"docx","work_url":"https://www.academia.edu/25535866/LABORATORIO_N_4_FUERZAS_EN_EQUILIBRIO","alternativeTracking":true}"><span class="material-symbols-outlined" style="font-size: 18px" translate="no">download</span><span class="ds2-5-text-link__content">Download free PDF</span></button><a class="ds2-5-text-link ds2-5-text-link--inline js-wsj-grid-card-view-pdf" href="https://www.academia.edu/25535866/LABORATORIO_N_4_FUERZAS_EN_EQUILIBRIO"><span class="ds2-5-text-link__content">View PDF</span><span class="material-symbols-outlined" style="font-size: 18px" translate="no">chevron_right</span></a></div></div><div class="ds-related-work--container js-wsj-grid-card" data-collection-position="6" data-entity-id="22769698" data-sort-order="default"><a class="ds-related-work--title js-wsj-grid-card-title ds2-5-body-md ds2-5-body-link" href="https://www.academia.edu/22769698/L%C3%8DNEAS_DE_FUERZA_Y_L%C3%8DNEAS_EQUIPOTENCIALES">LÍNEAS DE FUERZA Y LÍNEAS EQUIPOTENCIALES</a><div class="ds-related-work--metadata"><a class="js-wsj-grid-card-author ds2-5-body-sm ds2-5-body-link" data-author-id="44406609" href="https://independent.academia.edu/JUANDIEGOGomez">JUAN DIEGO Gomez</a></div><p class="ds-related-work--abstract ds2-5-body-sm">Objetivos 1. Describir el concepto de campo, 2. Describir el concepto de líneas de fuerza, 3. Describir el concepto de líneas equipotenciales, 4. Dibujar las líneas equipotenciales y las líneas de fuerza de dos placas paralelas, y 5. Dibujar las líneas equipotenciales y las líneas de fuerza de dos cargas puntiformes Teoría Un campo es cualquier región del espacio cuyos puntos están caracterizados por el valor de una variable física. Supongamos un salón de clases. En cada punto del espacio dentro del salón hay una temperatura. Entonces, el interior del salón de clases es un campo térmico. También es un campo de presión, un campo gravitatorio y uno magnético, entre otros, porque en cada punto del salón la presión atmosférica tiene un cierto valor, lo mismo la aceleración de la gravedad y la intensidad del campo magnético terrestre. Los campos pueden ser escalares, como el térmico, y el de presión, o vectoriales, como el gravitatorio y el magnético. La existencia del campo eléctrico vectorial se propone para explicar la atracción entre cargas eléctricas de signos distintos, o el rechazo entre cargas del mismo signo, aún cuando no hay contacto físico entre ellas. Este fenómeno se conoce como acción a distancia y nos resulta familiar en la interacción entre imanes. La atracción gravitatoria también es un fenómeno de acción a distancia ya que afecta a los cuerpos celestes aun cuando estos no están en contacto. En el caso electrostático, se asume que la carga positiva es una fuente de campo eléctrico, es decir, la carga positiva es el origen del campo eléctrico mientras que la carga negativa es el " desagüe " de campo eléctrico, o el sitio en el cual terminan las líneas de fuerza que empezaron en alguna carga positiva. Para definir el campo eléctrico, E, necesitamos una carga de prueba q 0 , suficientemente pequeña. La colocamos en cualquier punto alrededor de la carga cuyo campo eléctrico deseamos medir. Como la carga de prueba es muy pequeña, su propio campo eléctrico se considera insignificante frente al que vamos a medir. La carga de prueba debe ser positiva. Al ser colocada en la vecindad de otra carga va a sufrir una fuerza, F, cuya dirección es la misma que la del campo en ese punto. La magnitud del campo eléctrico es el resultado de dividir la fuerza entre q 0 , es decir, q o F E = Aunque el concepto de campo eléctrico, como lo conocemos ahora, no fue establecido originalmente en su forma actual, su existencia y propiedades básicas fueron propuestas por el físico y químico inglés Michael Faraday (1791-1867), a trabes de lo que llamó líneas de fuerza. 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