可调节的菱形截面平行于y轴的定制立体
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这个范例演示了一个可调节的立体,其截面平行于y轴的形状为菱形。核心数学概念包括函数、解析几何和立体几何。构造过程中使用了GeoGebra的Intersect(相交)、Line(直线)、Segment(线段)、Rotate(旋转)、Translate(平移)、Midpoint(中点)、Sphere(球体)、Textfield(文本框)、Polygon(多边形)、CurveCartesian(笛卡尔曲线)、Surface(曲面)和Angle(角度)等命令和对象。适合高中及以上学生学习和理解函数图像与立体几何的关系,以及如何通过参数调节图形特性。
GeoGebra 命令及参数
Intersect(lower, h, (0, -8)) → CLine(C, C + (1, 0, 0)) → cIntersect(upper, h, (0, 4)) → BSegment(C, B) → qIntersect(upper, q, (0, 4)) → GRotate(G, (ANG * pi / 180), C, c) → G'_1Translate(G'_1, Vector[C, G]) → J_1Segment(H, I) → s_1Midpoint(s_1) → A_1Segment(J, K) → q_1Midpoint(q_1) → ZMidpoint(s_1) → EMidpoint(q_1) → FMidpoint(C, G) → TLine(B, D) → iSphere(B, d) → eSegment(C, B) → pTextfield(upper) → InputBox1Textfield(lower) → InputBox2Textfield(a) → InputBox3Textfield(b) → InputBox4Segment(C, G) → k_1Line(C, G) → jSphere(G, T) → kLine(T, T + (1, 0, 0)) → mRotate(G, pi / 3, F_1, m) → G'Rotate(G', pi / 3, F_1, Line[F_1, F_1 + (1, 0, 0)]) → G''Line(F_1, F_1 + (1, 0, 0)) → nRotate(G'', pi / 3, F_1, n) → G'''Rotate(G''', pi / 3, F_1, n) → G_1Polygon(C, G, J_1, G'_1) → poly1, g_1, m_1, r_1, a_1Line(Z, Z + (1, 0, 0)) → fLine(D_1, D_1 + (1, 0, 0)) → gRotate(J, pi / 3, D_1, g) → J'Rotate(J', pi / 3, D_1, g) → J''Rotate(J'', pi / 3, D_1, g) → J'''Rotate(J''', pi / 3, D_1, g) → E_1Line(H_1, H_1 - (1, 0, 0)) → l_1Rotate(I, pi / 3, H_1, l_1) → I'Rotate(I', pi / 3, H_1, l_1) → I''Rotate(I'', pi / 3, H_1, l_1) → I'''Rotate(I''', pi / 3, H_1, l_1) → I_1Segment(G, J_1) → lSegment(J_1, G'_1) → rSegment(G'_1, C) → sLine(K, K + (1, 0, 0)) → tRotate(J, (ANG * pi / 180), K, t) → J'_1Translate(J'_1, Vector[K, J]) → K_1Polygon(K, J, K_1, J'_1) → q1, k_3, j_1, k_4, j'_1Line(I, I + (1, 0, 0)) → f_1Rotate(H, (ANG * pi / 180), I, f_1) → H'Translate(H', Vector[I, H]) → H''Segment(H, H'') → i_1Segment(H'', H') → n_1Segment(H', I) → p_1Polygon(I, H, H'', H') → q2, i_2, h_2, h'', h'Segment(J, K_1) → b_1Segment(K_1, J'_1) → c_1Intersect(t, q_1) → L_1Segment(J'_1, L_1) → d_1CurveCartesian(t, lower(t) + ((upper(t) - lower(t)) * cos((ANG * pi / 180))), ((upper(t) - lower(t)) * sin((ANG * pi / 180))), t, a, b) → oCurveCartesian(t, upper(t) + ((upper(t) - lower(t)) * cos((ANG * pi / 180))), ((upper(t) - lower(t)) * sin((ANG * pi / 180))), t, a, b) → uSurface(u, lower(u) + (((upper(u) - lower(u)) * v) * cos((ANG * pi / 180))), (((upper(u) - lower(u)) * v) * sin((ANG * pi / 180))), u, a, b, v, 0, 1) → vSurface(u, lower(u) + ((upper(u) - lower(u)) * cos((ANG * pi / 180))) + (v * (upper(u) - lower(u))), ((upper(u) - lower(u)) * sin((ANG * pi / 180))), u, a, b, v, 0, 1) → wSurface(u, upper(u) + (((upper(u) - lower(u)) * v) * cos((ANG * pi / 180))), (((upper(u) - lower(u)) * v) * sin((ANG * pi / 180))), u, a, b, v, 0, 1) → e_1Angle(G, C, G'_1) → α