Let the position vectors of three vertices of a triangle be 4p⃗+q⃗−3r⃗4 \vec{p} + \vec{q} - 3 \vec{r}, −5p⃗+q⃗+2r⃗-5 \vec{p} + \vec{q} + 2 \vec{r}, and 2p⃗−q⃗+2r⃗2 \vec{p} - \vec{q} + 2 \vec{r}. If the position vectors of the orthocenter and the circumcenter of the triangle are p⃗+q⃗+r⃗2\frac{\vec{p} + \vec{q} + \vec{r}}{2} and αp⃗+βq⃗+γr⃗\alpha \vec{p} + \beta \vec{q} + \gamma \vec{r} respectively, then α+2β+5γ\alpha + 2 \beta + 5 \gamma is equal to:

Answer: 2

Step-by-step solution

Step 1: Define position vectors of vertices, orthocenter, and circumcenter

We are given the position vectors of the three vertices of the triangle, denoted as A⃗\vec{A}, B⃗\vec{B}, and C⃗\vec{C}. We are also given the position vector of the orthocenter, H⃗\vec{H}, and the circumcenter, O⃗\vec{O}. We need to find the values of α\alpha, β\beta, and γ\gamma from the circumcenter's position vector.

Step 2: Apply Euler's Line Theorem

For any triangle, the orthocenter (H), centroid (G), and circumcenter (O) are collinear, and the centroid divides the segment HO in the ratio 2:1. This relationship is known as Euler's Line Theorem, which states that H⃗+2O⃗=3G⃗\vec{H} + 2\vec{O} = 3\vec{G}. Since the centroid G⃗=A⃗+B⃗+C⃗3\vec{G} = \frac{\vec{A} + \vec{B} + \vec{C}}{3}, we can substitute this into the Euler's Line equation to get H⃗+2O⃗=A⃗+B⃗+C⃗\vec{H} + 2\vec{O} = \vec{A} + \vec{B} + \vec{C}.

Step 3: Substitute known vectors into Euler's Line equation

Now, we substitute the given position vectors for A⃗\vec{A}, B⃗\vec{B}, C⃗\vec{C}, H⃗\vec{H}, and O⃗\vec{O} into the Euler's Line equation. This will allow us to form an equation in terms of p⃗\vec{p}, q⃗\vec{q}, and r⃗\vec{r}.

Step 4: Simplify and equate coefficients

We simplify both sides of the equation by collecting the coefficients of p⃗\vec{p}, q⃗\vec{q}, and r⃗\vec{r}. On the right side, (4−5+2)p⃗=p⃗(4-5+2)\vec{p} = \vec{p}, (1+1−1)q⃗=q⃗(1+1-1)\vec{q} = \vec{q}, and (−3+2+2)r⃗=r⃗(-3+2+2)\vec{r} = \vec{r}. Since p⃗\vec{p}, q⃗\vec{q}, and r⃗\vec{r} are non-coplanar vectors, their coefficients on both sides of the equation must be equal.

Step 5: Solve for α\alpha, β\beta, and γ\gamma

Equating the coefficients of p⃗\vec{p}, q⃗\vec{q}, and r⃗\vec{r} from the simplified equation, we solve for α\alpha, β\beta, and γ\gamma. In this case, all three coefficients turn out to be 14\frac{1}{4}.

Step 6: Calculate α+2β+5γ\alpha + 2\beta + 5\gamma

Finally, we substitute the calculated values of α\alpha, β\beta, and γ\gamma into the expression α+2β+5γ\alpha + 2\beta + 5\gamma to find the final answer.

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