A line makes angles alpha, beta, gamma and delta with the four diagonals of a cube, prove that cos2(alpha)+cos2(beta)+cos2(gamma)+cos2(delta)=4/3cos^2(alpha) + cos^2(beta) + cos^2(gamma) + cos^2(delta) = 4/3.

Answer: cos⁡2(α)+cos⁡2(β)+cos⁡2(γ)+cos⁡2(δ)=4/3\cos^2(\alpha) + \cos^2(\beta) + \cos^2(\gamma) + \cos^2(\delta) = 4/3 is proven.

Step-by-step solution

Step 1: Define Cube Vertices and Diagonals

To solve this problem, we first establish a coordinate system for the cube. Let the side length of the cube be aa. We place one vertex at the origin (0,0,0)(0{,}0{,}0) and align its edges with the coordinate axes. This defines the coordinates of all eight vertices of the cube.

Step 2: Determine Vector Representations of Cube Diagonals

A cube has four main diagonals connecting opposite vertices. We express these diagonals as vectors using the coordinates defined in the previous step. For example, the diagonal connecting (0,0,0)(0{,}0{,}0) to (a,a,a)(a,a,a) is represented by the vector (a,a,a)(a,a,a). The other diagonals are found similarly.

Step 3: Define a General Line Vector

Let an arbitrary line make angles α,β,γ,δ\alpha, \beta, \gamma, \delta with the four diagonals. We can represent this line by a unit vector L⃗=(l,m,n)\vec{L} = (l,m,n), where l,m,nl, m, n are its direction cosines. Thus, we have l2+m2+n2=1l^2 + m^2 + n^2 = 1.

Step 4: Apply Dot Product Formula for Angles

The cosine of the angle between two vectors can be found using their dot product. For a vector A⃗\vec{A} and a vector B⃗\vec{B}, the formula is cos⁡θ=A⃗⋅B⃗∣A⃗∣∣B⃗∣\cos \theta = \frac{\vec{A} \cdot \vec{B}}{|\vec{A}||\vec{B}|}. We will apply this to find the cosines of the angles between L⃗\vec{L} and each of the diagonal vectors.

Step 5: Calculate Cosine Squared for Each Angle

We calculate cos⁡2α\cos^2 \alpha, cos⁡2β\cos^2 \beta, cos⁡2γ\cos^2 \gamma, and cos⁡2δ\cos^2 \delta using the dot product formula. The magnitude of each diagonal vector is a2+a2+a2=3a2=a3\sqrt{a^2+a^2+a^2} = \sqrt{3a^2} = a\sqrt{3}. Since L⃗\vec{L} is a unit vector, ∣L⃗∣2=l2+m2+n2=1|\vec{L}|^2 = l^2+m^2+n^2=1. This simplifies the denominators considerably.

Step 6: Sum the Cosine Squared Terms

Now we sum the expressions for cos⁡2α\cos^2 \alpha, cos⁡2β\cos^2 \beta, cos⁡2γ\cos^2 \gamma, and cos⁡2δ\cos^2 \delta. Each term has a common denominator of 3, so we can combine the numerators.

Step 7: Expand and Simplify Numerators

We expand each squared term (A+B+C)2=A2+B2+C2+2AB+2BC+2CA(A+B+C)^2 = A^2+B^2+C^2+2AB+2BC+2CA. This will help us identify terms that cancel out when summed.

Step 8: Perform the Summation

Adding the expanded terms, we observe that the cross-product terms (2lm,2mn,2nl2lm, 2mn, 2nl) cancel each other out in pairs. For example, 2lm−2lm+2lm−2lm=02lm - 2lm + 2lm - 2lm = 0. We are left with four times the sum of the squares of the direction cosines.

Step 9: Substitute l2+m2+n2=1l^2+m^2+n^2=1

Since l,m,nl, m, n are the direction cosines of a unit vector along the line, we know that l2+m2+n2=1l^2+m^2+n^2=1. Substituting this value simplifies the sum of the numerators to 4.

Step 10: Final Result

Finally, we substitute the simplified numerator back into the expression for the sum of cosine squared terms. This proves the identity that the sum is equal to 4/34/3.

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