// Numbas version: finer_feedback_settings {"name": "John's copy of Resolve forces on particle in equilibrium", "extensions": [], "custom_part_types": [], "resources": [["question-resources/statics1.png", "/srv/numbas/media/question-resources/statics1.png"]], "navigation": {"allowregen": true, "showfrontpage": false, "preventleave": false, "typeendtoleave": false}, "question_groups": [{"pickingStrategy": "all-ordered", "questions": [{"functions": {}, "ungrouped_variables": ["F1", "theta1", "F2", "theta2", "F3", "theta3", "check", "check2"], "name": "John's copy of Resolve forces on particle in equilibrium", "tags": [], "preamble": {"css": "", "js": ""}, "advice": "
As the particle is in equilibrium we equate the sum of the forces to zero.
\nResolving horizontally we have
\n\\begin{align}
F_1 \\cos \\theta_1 + F_2 \\cos \\theta_2 - F_3 \\cos \\theta_3 & = 0, \\\\
\\var{F1} \\cos \\var{theta1}^{\\circ} + F_2 \\cos \\var{theta2}^{\\circ} - F_3 \\cos \\var{theta3}^{\\circ} & = 0, \\\\
F_2 \\cos \\var{theta2}^{\\circ} & = F_3 \\cos \\var{theta3}^{\\circ} - \\var{F1} \\cos \\var{theta1}^{\\circ}, \\\\
F_2 & = \\frac{F_3 \\cos \\var{theta3}^{\\circ} - \\var{F1} \\cos \\var{theta1}^{\\circ}}{ \\cos \\var{theta2}^{\\circ}}.
\\end{align}
Resolving vertically, we have
\n\\begin{align}
F_1 \\sin \\theta_1 - F_2 \\sin \\theta_2 - F_3 \\sin \\theta_3 & = 0, \\\\
\\var{F1} \\sin \\var{theta1}^{\\circ} - F_2 \\sin \\var{theta2}^{\\circ} - F_3 \\sin \\var{theta3}^{\\circ} & = 0, \\\\
F_3 \\sin \\var{theta3}^{\\circ}& = \\var{F1} \\sin \\var{theta1}^{\\circ} - F_2 \\sin \\var{theta2}^{\\circ}.
\\end{align}
Substituting our value for $F_2$ into the formula $F_3 \\sin \\var{theta3}^{\\circ}$ and rearranging gives
\n\\begin{align}
F_3 \\sin \\var{theta3}^{\\circ} & = \\var{F1} \\sin \\var{theta1}^{\\circ} - F_2 \\sin \\var{theta2}^{\\circ} \\\\
F_3 \\sin \\var{theta3}^{\\circ} & = \\var{F1} \\sin \\var{theta1}^{\\circ} - \\left( \\frac{F_3 \\cos \\var{theta3}^{\\circ} - \\var{F1} \\cos \\var{theta1}^{\\circ}}{\\cos \\var{theta2}^{\\circ}} \\right) \\sin \\var{theta2}^{\\circ}, \\\\
F_3 \\sin \\var{theta3}^{\\circ} & = \\var{F1} \\sin \\var{theta1}^{\\circ} - F_3 \\frac{ \\cos \\var{theta3}^{\\circ}}{ \\cos \\var{theta2}^{\\circ}} \\sin \\var{theta2}^{\\circ} + \\var{F1} \\frac{ \\cos \\var{theta1}^{\\circ}}{ \\cos \\var{theta2}^{\\circ}} \\sin \\var{theta2}^{\\circ}, \\\\
F_3 \\left( \\sin \\var{theta3}^{\\circ} + \\frac{ \\cos \\var{theta3}^{\\circ}}{ \\cos \\var{theta2}^{\\circ}} \\sin \\var{theta2}^{\\circ} \\right) & = \\var{F1} \\sin \\var{theta1}^{\\circ} + \\var{F1} \\frac{ \\cos \\var{theta1}^{\\circ}}{ \\cos \\var{theta2}^{\\circ}} \\sin \\var{theta2}^{\\circ} \\\\
F_3 & = \\frac{\\var{F1} \\sin \\var{theta1}^{\\circ} + \\var{F1} \\frac{ \\cos \\var{theta1}^{\\circ}}{ \\cos \\var{theta2}^{\\circ}} \\sin \\var{theta2}^{\\circ}}{ \\sin \\var{theta3}^{\\circ} + \\frac{ \\cos \\var{theta3}^{\\circ}}{ \\cos \\var{theta2}^{\\circ}} \\sin \\var{theta2}^{\\circ}}.
\\end{align}
Therefore, to 3 s.f. we have $F_3 = \\var{siground(F3,3)} \\mathrm{N}. $
\nWe can then use our $F_3$ value in our equation for $F_2$
\n\\begin{align}
F_2 & = \\frac{F_3 \\cos \\var{theta3}^{\\circ} - \\var{F1} \\cos \\var{theta1}^{\\circ}}{\\cos \\var{theta2}^{\\circ}}, \\\\
& = \\frac{\\var{siground(F3,3)} \\cos \\var{theta3}^{\\circ} - \\var{F1} \\cos \\var{theta1}^{\\circ}}{\\cos \\var{theta2}^{\\circ}}, \\\\
& = \\var{siground(F2,3)} \\mathrm{N}.
\\end{align}
$F_2 = $ [[0]]
\n", "variableReplacements": [], "variableReplacementStrategy": "originalfirst", "gaps": [{"precisionType": "sigfig", "precisionMessage": "You have not given your answer to the correct precision.
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\n", "variableReplacements": [], "variableReplacementStrategy": "originalfirst", "gaps": [{"precisionType": "sigfig", "precisionMessage": "You have not given your answer to the correct precision.
", "allowFractions": false, "variableReplacements": [], "precision": "3", "maxValue": "F3", "variableReplacementStrategy": "originalfirst", "strictPrecision": false, "correctAnswerFraction": false, "showCorrectAnswer": true, "precisionPartialCredit": 0, "scripts": {}, "marks": 1, "minValue": "F3", "type": "numberentry", "showPrecisionHint": false}], "showCorrectAnswer": true, "scripts": {}, "marks": 0, "type": "gapfill"}], "extensions": [], "statement": "The diagram shows a particle in equilibrium under the forces shown.
\n\nYou are told that $F_1 = \\var{F1} \\ \\mathrm{N}$ and that the angles are $\\theta_1 = \\var{theta1}^{\\circ}, \\ \\theta_2 = \\var{theta2}$ and $\\theta_3 = \\var{theta3}^{\\circ}$.
\nBy resolving horizontally and vertically, find the magnitude of the forces $F_2 $ and $F_3 $, in Newtons, and input them to 3 significant figures below.
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"}, "check2": {"definition": "F1*sin(radians(theta1))-F2*sin(radians(theta2))-F3*sin(radians(theta3))", "templateType": "anything", "group": "Ungrouped variables", "name": "check2", "description": "Total vertical force. Should be zero for equilbrium.
"}, "check": {"definition": "F1*cos(radians(theta1))+F2*cos(radians(theta2))-F3*cos(radians(theta3))", "templateType": "anything", "group": "Ungrouped variables", "name": "check", "description": "Total horizontal force. Should be zero for equilibrium
"}}, "metadata": {"description": "Three forces act on a particle. You're given the magnitude of one, and the directions of all three. Find the magnitudes of the other two forces.
", "licence": "Creative Commons Attribution 4.0 International"}, "type": "question", "showQuestionGroupNames": false, "question_groups": [{"name": "", "pickingStrategy": "all-ordered", "pickQuestions": 0, "questions": []}], "contributors": [{"name": "John Bridges", "profile_url": "https://numbas.mathcentre.ac.uk/accounts/profile/913/"}]}]}], "contributors": [{"name": "John Bridges", "profile_url": "https://numbas.mathcentre.ac.uk/accounts/profile/913/"}]}