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The following incantation asks for the two vectors two be drawn, each with \ their base at the location pt[t]:\ \>", "Text", CellChangeTimes->{{3.4350728301896534`*^9, 3.43507290651729*^9}}], Cell[BoxData[ RowBox[{ RowBox[{"drawVectors", "[", "t_", "]"}], " ", ":=", " ", RowBox[{"ListVectorFieldPlot", "[", RowBox[{"{", RowBox[{ RowBox[{"{", RowBox[{ RowBox[{"pt", "[", "t", "]"}], ",", RowBox[{ RowBox[{"pt", "'"}], "[", "t", "]"}]}], "}"}], ",", RowBox[{"{", RowBox[{ RowBox[{"pt", "[", "t", "]"}], ",", RowBox[{ RowBox[{"pt", "''"}], "[", "t", "]"}]}], "}"}]}], "}"}], "]"}]}]], "Input", CellChangeTimes->{{3.4350724429421315`*^9, 3.43507249944177*^9}}], Cell[CellGroupData[{ Cell[BoxData[ RowBox[{"Animate", "[", RowBox[{ RowBox[{"Show", "[", RowBox[{"cycloid", ",", RowBox[{"drawPt", "[", "t", "]"}], ",", RowBox[{"drawWheel", "[", "t", "]"}], ",", RowBox[{"drawVectors", "[", "t", "]"}]}], "]"}], ",", RowBox[{"{", RowBox[{"t", ",", "0", ",", RowBox[{"2", " ", "\[Pi]"}]}], "}"}]}], "]"}]], "Input", CellChangeTimes->{{3.4350720923193755`*^9, 3.4350721134286156`*^9}, { 3.435072195709339*^9, 3.4350722051624036`*^9}, {3.4350725188635206`*^9, 3.4350725282540855`*^9}}], Cell[BoxData[ TagBox[ StyleBox[ DynamicModuleBox[{$CellContext`t$$ = 5.296724806488744, Typeset`show$$ = True, Typeset`bookmarkList$$ = {}, Typeset`bookmarkMode$$ = "Menu", Typeset`animator$$, Typeset`animvar$$ = 1, Typeset`name$$ = "\"untitled\"", Typeset`specs$$ = {{ Hold[$CellContext`t$$], 0, 2 Pi}}, Typeset`size$$ = {360., {76., 80.}}, Typeset`update$$ = 0, Typeset`initDone$$, Typeset`skipInitDone$$ = True, $CellContext`t$621$$ = 0}, DynamicBox[Manipulate`ManipulateBoxes[ 1, StandardForm, "Variables" :> {$CellContext`t$$ = 0}, "ControllerVariables" :> { Hold[$CellContext`t$$, $CellContext`t$621$$, 0]}, "OtherVariables" :> { Typeset`show$$, Typeset`bookmarkList$$, Typeset`bookmarkMode$$, Typeset`animator$$, Typeset`animvar$$, Typeset`name$$, Typeset`specs$$, Typeset`size$$, Typeset`update$$, Typeset`initDone$$, Typeset`skipInitDone$$}, "Body" :> Show[$CellContext`cycloid, $CellContext`drawPt[$CellContext`t$$], $CellContext`drawWheel[$CellContext`t$$], $CellContext`drawVectors[$CellContext`t$$]], "Specifications" :> {{$CellContext`t$$, 0, 2 Pi, AppearanceElements -> { "ProgressSlider", "PlayPauseButton", "FasterSlowerButtons", "DirectionButton"}}}, "Options" :> { ControlType -> Animator, AppearanceElements -> None, SynchronousUpdating -> True, ShrinkingDelay -> 10.}, "DefaultOptions" :> {}], ImageSizeCache->{408., {114., 119.}}, SingleEvaluation->True], Deinitialization:>None, DynamicModuleValues:>{}, SynchronousInitialization->True, UnsavedVariables:>{Typeset`initDone$$}, UntrackedVariables:>{Typeset`size$$}], "Manipulate", Deployed->True, StripOnInput->False], Manipulate`InterpretManipulate[1]]], "Output", CellChangeTimes->{3.435169150465*^9}] }, Open ]], Cell[TextData[StyleBox["Morin 3.40", "Subsection"]], "Text", CellChangeTimes->{{3.435075858560897*^9, 3.435075860826507*^9}, { 3.4350759138574176`*^9, 3.4350759496384387`*^9}}], Cell["\<\ We drop a ball from height h, and it hits a redirector at height y0. 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"\[Equal]", "y0"}]}], "}"}], ",", RowBox[{"{", RowBox[{ RowBox[{"x", "[", "t", "]"}], ",", RowBox[{"y", "[", "t", "]"}]}], "}"}], ",", "t"}], "]"}]}]], "Input", CellChangeTimes->{{3.4350767981017585`*^9, 3.4350768860855703`*^9}}], Cell[BoxData[ RowBox[{"{", RowBox[{"{", RowBox[{ RowBox[{ RowBox[{"y", "[", "t", "]"}], "\[Rule]", RowBox[{ FractionBox["1", "2"], " ", RowBox[{"(", RowBox[{ RowBox[{ RowBox[{"-", "g"}], " ", SuperscriptBox["t", "2"]}], "+", RowBox[{"2", " ", "y0"}]}], ")"}]}]}], ",", RowBox[{ RowBox[{"x", "[", "t", "]"}], "\[Rule]", RowBox[{ SqrtBox["2"], " ", "t", " ", SqrtBox[ RowBox[{ RowBox[{"g", " ", "h"}], "-", RowBox[{"g", " ", "y0"}]}]]}]}]}], "}"}], "}"}]], "Output", CellChangeTimes->{{3.435076881648099*^9, 3.435076886616817*^9}, 3.435168862127*^9, 3.435169997322*^9}] }, Open ]], Cell["Next ask for the time when we hit the ground:", "Text", CellChangeTimes->{{3.435076902272967*^9, 3.4350769090697985`*^9}}], Cell[CellGroupData[{ Cell[BoxData[ RowBox[{"time", " ", "=", " ", RowBox[{"Solve", "[", RowBox[{ RowBox[{ RowBox[{"(", RowBox[{ RowBox[{"y", "[", "t", "]"}], "/.", RowBox[{"ballistic", "[", RowBox[{"[", "1", "]"}], "]"}]}], ")"}], "\[Equal]", "0"}], ",", "t"}], "]"}]}]], "Input", CellChangeTimes->{{3.435076910819787*^9, 3.435076946194561*^9}, { 3.4350769864443035`*^9, 3.435076991178648*^9}}], Cell[BoxData[ RowBox[{"{", RowBox[{ RowBox[{"{", RowBox[{"t", "\[Rule]", RowBox[{"-", FractionBox[ RowBox[{ SqrtBox["2"], " ", SqrtBox["y0"]}], SqrtBox["g"]]}]}], "}"}], ",", RowBox[{"{", RowBox[{"t", "\[Rule]", FractionBox[ RowBox[{ SqrtBox["2"], " ", SqrtBox["y0"]}], SqrtBox["g"]]}], "}"}]}], "}"}]], "Output", CellChangeTimes->{{3.435076927054058*^9, 3.4350769472414293`*^9}, 3.4350769918036437`*^9, 3.435168863512*^9, 3.435169998712*^9}] }, Open ]], Cell["\<\ Tell yourself, \"oh yeah, I know how long it takes to fall a height y0 \ starting from rest\" before selecting the 2nd time and forming the distance we go:\ \>", "Text", CellChangeTimes->{{3.435076957131991*^9, 3.435077016944108*^9}}], Cell[CellGroupData[{ Cell[BoxData[ RowBox[{ RowBox[{"d", "[", "y0_", "]"}], " ", "=", " ", RowBox[{ RowBox[{ RowBox[{"x", "[", "t", "]"}], "/.", RowBox[{"ballistic", "[", RowBox[{"[", "1", "]"}], "]"}]}], " ", "/.", " ", RowBox[{"time", "[", RowBox[{"[", "2", "]"}], "]"}]}]}]], "Input", CellChangeTimes->{{3.435077018647222*^9, 3.4350770615531974`*^9}}], Cell[BoxData[ FractionBox[ RowBox[{"2", " ", SqrtBox["y0"], " ", SqrtBox[ RowBox[{ RowBox[{"g", " ", "h"}], "-", RowBox[{"g", " ", "y0"}]}]]}], SqrtBox["g"]]], "Output", CellChangeTimes->{{3.435077046553293*^9, 3.4350770618500705`*^9}, 3.435168865124*^9, 3.4351700009779997`*^9}] }, Open ]], Cell["To optimize the distance we ask for:", "Text", CellChangeTimes->{{3.4350770985998354`*^9, 3.4350771054591665`*^9}}], Cell[CellGroupData[{ Cell[BoxData[ RowBox[{"Solve", "[", RowBox[{ RowBox[{ RowBox[{ RowBox[{"d", "'"}], "[", "y", "]"}], "\[Equal]", "0"}], ",", "y"}], "]"}]], "Input", CellChangeTimes->{{3.435077106927907*^9, 3.435077142130807*^9}}], Cell[BoxData[ RowBox[{"{", RowBox[{"{", RowBox[{"y", "\[Rule]", FractionBox["h", "2"]}], "}"}], "}"}]], "Output", CellChangeTimes->{3.4350771185684576`*^9, 3.43516886702*^9, 3.4351700047799997`*^9}] }, Open ]], Cell["\<\ And now some fun, make a parametric plot of the full motion. First figure \ out how long it takes to fall and hit the diverter.\ \>", "Text", CellChangeTimes->{{3.4350773398170414`*^9, 3.4350773423014007`*^9}, { 3.435077403488509*^9, 3.4350774232383823`*^9}, {3.435078982790901*^9, 3.4350790029470224`*^9}, {3.435079435913001*^9, 3.435079445256692*^9}}], Cell[CellGroupData[{ Cell[BoxData[ RowBox[{" ", RowBox[{"Solve", "[", " ", RowBox[{ RowBox[{ RowBox[{"h", " ", "-", " ", RowBox[{ RowBox[{"(", RowBox[{"1", "/", "2"}], ")"}], " ", "g", " ", RowBox[{"t", "^", "2"}]}]}], " ", "==", " ", "y0"}], ",", "t"}], "]"}]}]], "Input", CellChangeTimes->{{3.435082121114566*^9, 3.4350822096764994`*^9}}], Cell[BoxData[ RowBox[{"{", RowBox[{ RowBox[{"{", RowBox[{"t", "\[Rule]", RowBox[{"-", FractionBox[ RowBox[{ SqrtBox["2"], " ", SqrtBox[ RowBox[{"h", "-", "y0"}]]}], SqrtBox["g"]]}]}], "}"}], ",", RowBox[{"{", RowBox[{"t", "\[Rule]", FractionBox[ RowBox[{ SqrtBox["2"], " ", SqrtBox[ RowBox[{"h", "-", "y0"}]]}], SqrtBox["g"]]}], "}"}]}], "}"}]], "Output", CellChangeTimes->{{3.435082170614249*^9, 3.4350821746298485`*^9}, 3.4350822126139803`*^9, 3.435168872113*^9, 3.435170011943*^9}] }, Open ]], Cell[CellGroupData[{ Cell[BoxData[ RowBox[{"T", "=", " ", RowBox[{"t", "/.", RowBox[{"%", "[", RowBox[{"[", "2", "]"}], "]"}]}]}]], "Input", CellChangeTimes->{{3.435082214910841*^9, 3.4350822200514326`*^9}}], Cell[BoxData[ FractionBox[ RowBox[{ SqrtBox["2"], " ", SqrtBox[ RowBox[{"h", "-", "y0"}]]}], SqrtBox["g"]]], "Output", CellChangeTimes->{3.435082221754547*^9, 3.4351688741949997`*^9, 3.435170013493*^9}] }, Open ]], Cell["\<\ Then form piecewise continuous expressions for x[t] and y[t] by gluing \ together the two parts of the motion:\ \>", "Text", CellChangeTimes->{{3.4350822246139035`*^9, 3.4350822684104986`*^9}}], Cell[BoxData[ RowBox[{ RowBox[{"x", "[", "t_", "]"}], " ", ":=", " ", RowBox[{"Piecewise", "[", RowBox[{"{", RowBox[{ RowBox[{"{", RowBox[{"0", ",", RowBox[{"t", "<", "T"}]}], "}"}], ",", RowBox[{"{", RowBox[{ RowBox[{"v0", " ", RowBox[{"(", RowBox[{"t", "-", "T"}], ")"}]}], ",", RowBox[{"t", ">", "T"}]}], "}"}]}], "}"}], "]"}]}]], "Input", CellChangeTimes->{{3.435077424957122*^9, 3.435077451488202*^9}, { 3.435082272691721*^9, 3.435082277972937*^9}, {3.4350823202226667`*^9, 3.4350823266445007`*^9}, {3.4350824614248877`*^9, 3.4350824639873714`*^9}, { 3.435083019405692*^9, 3.4350830231087933`*^9}}], Cell["\<\ To use this expression we of course need to definre the speed at the \ diverter, using the above:\ \>", "Text", CellChangeTimes->{{3.435082333472582*^9, 3.4350823776129246`*^9}}], Cell[CellGroupData[{ Cell[BoxData[ RowBox[{"v0", " ", "=", " ", RowBox[{"v", "/.", RowBox[{"speed", "[", RowBox[{"[", "2", "]"}], "]"}]}]}]], "Input", CellChangeTimes->{{3.435082379316038*^9, 3.435082395144062*^9}}], Cell[BoxData[ RowBox[{ SqrtBox["2"], " ", SqrtBox[ RowBox[{ RowBox[{"g", " ", "h"}], "-", RowBox[{"g", " ", "y0"}]}]]}]], "Output", CellChangeTimes->{3.435082395362811*^9, 3.435168877422*^9, 3.435170020142*^9} ] }, Open ]], Cell["And we need a similar expression for y[t]:", "Text", CellChangeTimes->{{3.435082526330723*^9, 3.435082532940055*^9}}], Cell[BoxData[ RowBox[{ RowBox[{"y", "[", "t_", "]"}], " ", ":=", " ", RowBox[{"Piecewise", "[", RowBox[{"{", RowBox[{ RowBox[{"{", RowBox[{ RowBox[{"h", "-", RowBox[{ RowBox[{"(", RowBox[{"1", "/", "2"}], ")"}], " ", "g", " ", RowBox[{"t", "^", "2"}]}]}], ",", RowBox[{"t", "<", "T"}]}], "}"}], ",", RowBox[{"{", RowBox[{ RowBox[{"y0", "-", RowBox[{ RowBox[{"(", RowBox[{"1", "/", "2"}], ")"}], "g", " ", RowBox[{ RowBox[{"(", RowBox[{"t", "-", "T"}], ")"}], "^", "2"}]}]}], ",", RowBox[{"t", ">", "T"}]}], "}"}]}], "}"}], "]"}]}]], "Input", CellChangeTimes->{{3.4350825357681623`*^9, 3.4350825843147264`*^9}, { 3.435082848172413*^9, 3.4350828511880183`*^9}}], Cell["Let's recap:", "Text", CellChangeTimes->{{3.4350826118458004`*^9, 3.435082622736356*^9}}], Cell[CellGroupData[{ Cell[BoxData[ RowBox[{"{", RowBox[{ RowBox[{"x", "[", "t", "]"}], ",", RowBox[{"y", 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