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README.md
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colorFrom: indigo
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sdk: gradio
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sdk_version:
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app_file: run.py
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pinned: false
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hf_oauth: true
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sdk: gradio
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sdk_version: 6.0.0
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app_file: run.py
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pinned: false
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hf_oauth: true
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run.ipynb
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{"cells": [{"cell_type": "markdown", "id": "302934307671667531413257853548643485645", "metadata": {}, "source": ["# Gradio Demo: blocks_kinematics"]}, {"cell_type": "code", "execution_count": null, "id": "272996653310673477252411125948039410165", "metadata": {}, "outputs": [], "source": ["!pip install -q gradio numpy pandas "]}, {"cell_type": "code", "execution_count": null, "id": "288918539441861185822528903084949547379", "metadata": {}, "outputs": [], "source": ["import pandas as pd\n", "import numpy as np\n", "\n", "import gradio as gr\n", "\n", "def plot(v, a):\n", " g = 9.81\n", " theta = a / 180 * 3.14\n", " tmax = ((2 * v) * np.sin(theta)) / g\n", " timemat = tmax * np.linspace(0, 1, 40)\n", "\n", " x = (v * timemat) * np.cos(theta)\n", " y = ((v * timemat) * np.sin(theta)) - ((0.5 * g) * (timemat**2))\n", " df = pd.DataFrame({\"x\": x, \"y\": y})\n", " return df\n", "\n", "demo = gr.Blocks()\n", "\n", "with demo:\n", " gr.Markdown(\n", " r\"Let's do some kinematics! Choose the speed and angle to see the trajectory. Remember that the range $R = v_0^2 \\cdot \\frac{\\sin(2\\theta)}{g}$\"\n", " )\n", "\n", " with gr.Row():\n", " speed = gr.Slider(1, 30, 25, label=\"Speed\")\n", " angle = gr.Slider(0, 90, 45, label=\"Angle\")\n", " output = gr.LinePlot(\n", " x=\"x\",\n", " y=\"y\",\n", "
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{"cells": [{"cell_type": "markdown", "id": "302934307671667531413257853548643485645", "metadata": {}, "source": ["# Gradio Demo: blocks_kinematics"]}, {"cell_type": "code", "execution_count": null, "id": "272996653310673477252411125948039410165", "metadata": {}, "outputs": [], "source": ["!pip install -q gradio numpy pandas "]}, {"cell_type": "code", "execution_count": null, "id": "288918539441861185822528903084949547379", "metadata": {}, "outputs": [], "source": ["import pandas as pd\n", "import numpy as np\n", "\n", "import gradio as gr\n", "\n", "def plot(v, a):\n", " g = 9.81\n", " theta = a / 180 * 3.14\n", " tmax = ((2 * v) * np.sin(theta)) / g\n", " timemat = tmax * np.linspace(0, 1, 40)\n", "\n", " x = (v * timemat) * np.cos(theta)\n", " y = ((v * timemat) * np.sin(theta)) - ((0.5 * g) * (timemat**2))\n", " df = pd.DataFrame({\"x\": x, \"y\": y})\n", " return df\n", "\n", "demo = gr.Blocks()\n", "\n", "with demo:\n", " gr.Markdown(\n", " r\"Let's do some kinematics! Choose the speed and angle to see the trajectory. Remember that the range $R = v_0^2 \\cdot \\frac{\\sin(2\\theta)}{g}$\"\n", " )\n", "\n", " with gr.Row():\n", " speed = gr.Slider(1, 30, 25, label=\"Speed\")\n", " angle = gr.Slider(0, 90, 45, label=\"Angle\")\n", " output = gr.LinePlot(\n", " x=\"x\",\n", " y=\"y\",\n", " tooltip=[\"x\", \"y\"],\n", " x_lim=[0, 100],\n", " y_lim=[0, 60],\n", " height=300,\n", " )\n", " btn = gr.Button(value=\"Run\")\n", " btn.click(plot, [speed, angle], output)\n", "\n", "if __name__ == \"__main__\":\n", " demo.launch()\n"]}], "metadata": {}, "nbformat": 4, "nbformat_minor": 5}
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run.py
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output = gr.LinePlot(
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x="x",
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y="y",
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overlay_point=True,
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tooltip=["x", "y"],
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x_lim=[0, 100],
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y_lim=[0, 60],
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width=350,
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height=300,
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)
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btn = gr.Button(value="Run")
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output = gr.LinePlot(
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x="x",
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y="y",
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tooltip=["x", "y"],
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x_lim=[0, 100],
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y_lim=[0, 60],
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height=300,
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)
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btn = gr.Button(value="Run")
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