The cross product is , which is perpendicular to both vectors. Any nonzero scalar multiple works, so a simple answer is
Its dot product with each given vector is zero.
The product-to-sum identity for the sine gives . Each cosine has zero integral on this interval, so
This is also an instance of Fourier orthogonality.
Using , the definite integral is
The gradient is . Both partial derivatives vanish at , so it is a stationary point.
The second component of the gradient forces . The first then requires . Apart from , the only stationary point is
Taking the negative gradient of the potential energy gives the force
The divergence is the sum of the three diagonal partial derivatives:
Each component depends only on its own coordinate, so all cross partial derivatives vanish. Therefore the curl is
This also follows from the identity that the curl of a gradient vanishes for a twice continuously differentiable potential energy.
The matrix product of the transposed first vector with the second is their dot product:
The reverse arrangement is an outer product, with entries :
The two factors have moduli and , and complex arguments and . Multiplication multiplies the moduli and adds the complex arguments, giving
The displayed angle is the principal argument in radians; equivalently the argument is modulo .
The logarithmic series gives the first two nonzero terms:
For , separation of variables gives , hence . Setting gives the half-life
This is the same reciprocal decay law as a second-order reaction with the specified disappearance rate coefficient. A positive initial value is needed for a positive half-time; instead gives the identically zero solution.
There are equally likely unordered pairs, and contain one ball of each colour. Thus the hypergeometric distribution gives
Let be indicator random variables for the two draws being red. Each draw has red probability , even though the draws are dependent. By linearity of expectation, the number satisfies

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