/** * @license * Copyright 2020 Google LLC. All Rights Reserved. * Licensed under the Apache License, Version 2.0 (the "License"); * you may not use this file except in compliance with the License. * You may obtain a copy of the License at * * http://www.apache.org/licenses/LICENSE-2.0 * * Unless required by applicable law or agreed to in writing, software * distributed under the License is distributed on an "AS IS" BASIS, * WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. * See the License for the specific language governing permissions and * limitations under the License. * ============================================================================= */ import { ENGINE } from '../engine'; import { Atan2 } from '../kernel_names'; import { makeTypesMatch } from '../tensor_util'; import { convertToTensor } from '../tensor_util_env'; import { op } from './operation'; /** * Computes arctangent of `tf.Tensor`s a / b element-wise: `atan2(a, b)`. * Supports broadcasting. * * ```js * const a = tf.tensor1d([1.0, 1.0, -1.0, .7]); * const b = tf.tensor1d([2.0, 13.0, 3.5, .21]); * * tf.atan2(a, b).print() * ``` * * @param a The first tensor. * @param b The second tensor. Must have the same dtype as `a`. * * @doc {heading: 'Operations', subheading: 'Basic math'} */ function atan2_(a, b) { let $a = convertToTensor(a, 'a', 'atan2'); let $b = convertToTensor(b, 'b', 'atan2'); [$a, $b] = makeTypesMatch($a, $b); const inputs = { a: $a, b: $b }; return ENGINE.runKernel(Atan2, inputs); } export const atan2 = /* @__PURE__ */ op({ atan2_ }); //# sourceMappingURL=data:application/json;base64,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