Let a→=2ı^−ȷ^+3k^\overrightarrow{\mathrm{a}}=2\hat{\imath}-\hat{\jmath}+3\hat{k}, b→=3ı^−5ȷ^+k^\overrightarrow{\mathrm{b}}=3\hat{\imath}-5\hat{\jmath}+\hat{k} and c→\overrightarrow{\mathrm{c}} be a vector such that a→×c→=c→×b→\overrightarrow{\mathrm{a}} \times \overrightarrow{\mathrm{c}}=\overrightarrow{\mathrm{c}} \times \overrightarrow{\mathrm{b}} and (a⃗+c⃗)⋅(b⃗+c⃗)=168(\vec{a}+\vec{c}) \cdot (\vec{b}+\vec{c})=168. Then the maximum value of ∣c⃗∣2|\vec{c}|^2 is:

Answer: 308

Step-by-step solution

Step 1: Simplify the cross product equation

The given cross product equation is a→×c→=c→×b→\overrightarrow{\mathrm{a}} \times \overrightarrow{\mathrm{c}}=\overrightarrow{\mathrm{c}} \times \overrightarrow{\mathrm{b}}. We know that the cross product is anti-commutative, meaning c→×b→=−(b→×c→)\overrightarrow{\mathrm{c}} \times \overrightarrow{\mathrm{b}} = -(\overrightarrow{\mathrm{b}} \times \overrightarrow{\mathrm{c}}). Substituting this into the equation and rearranging terms, we get (a→+b→)×c→=0→(\overrightarrow{\mathrm{a}} + \overrightarrow{\mathrm{b}}) \times \overrightarrow{\mathrm{c}} = \overrightarrow{0}. This implies that c→\overrightarrow{\mathrm{c}} is parallel to (a→+b→)(\overrightarrow{\mathrm{a}} + \overrightarrow{\mathrm{b}}).

Step 2: Calculate a→+b→\overrightarrow{\mathrm{a}} + \overrightarrow{\mathrm{b}} and express c→\overrightarrow{\mathrm{c}}

First, we calculate the sum of vectors a→\overrightarrow{\mathrm{a}} and b→\overrightarrow{\mathrm{b}}. Since c→\overrightarrow{\mathrm{c}} is parallel to (a→+b→)(\overrightarrow{\mathrm{a}} + \overrightarrow{\mathrm{b}}), we can express c→\overrightarrow{\mathrm{c}} as a scalar multiple of (a→+b→)(\overrightarrow{\mathrm{a}} + \overrightarrow{\mathrm{b}}), where λ\lambda is a scalar.

Step 3: Expand the dot product equation

We are given the dot product equation (a⃗+c⃗)⋅(b⃗+c⃗)=168(\vec{a}+\vec{c}) \cdot (\vec{b}+\vec{c})=168. Expanding this equation, we get a⃗⋅b⃗+a⃗⋅c⃗+c⃗⋅b⃗+c⃗⋅c⃗=168\vec{a} \cdot \vec{b} + \vec{a} \cdot \vec{c} + \vec{c} \cdot \vec{b} + \vec{c} \cdot \vec{c} = 168. We can rewrite the middle terms as (a⃗+b⃗)⋅c⃗(\vec{a} + \vec{b}) \cdot \vec{c} and c⃗⋅c⃗\vec{c} \cdot \vec{c} is simply ∣c⃗∣2|\vec{c}|^2.

Step 4: Calculate dot products and magnitudes

We calculate the dot product a⃗⋅b⃗\vec{a} \cdot \vec{b}. Then, we use the fact that c⃗=λ(a⃗+b⃗)\vec{c} = \lambda (\vec{a} + \vec{b}) to simplify (a⃗+b⃗)⋅c⃗(\vec{a} + \vec{b}) \cdot \vec{c} to λ∣a⃗+b⃗∣2\lambda |\vec{a} + \vec{b}|^2. We also calculate the magnitude squared of (a⃗+b⃗)(\vec{a} + \vec{b}) and express ∣c⃗∣2|\vec{c}|^2 in terms of λ\lambda.

Step 5: Substitute into the expanded dot product equation

Substitute the calculated values into the expanded dot product equation. This results in a quadratic equation in terms of λ\lambda. Solving this quadratic equation by factoring gives us two possible values for λ\lambda: 11 and −2-2.

Step 6: Find the maximum value of ∣c⃗∣2|\vec{c}|^2

We use the expression for ∣c⃗∣2=77λ2|\vec{c}|^2 = 77\lambda^2 and substitute the two values of λ\lambda we found. For λ=1\lambda = 1, ∣c⃗∣2=77|\vec{c}|^2 = 77. For λ=−2\lambda = -2, ∣c⃗∣2=308|\vec{c}|^2 = 308. The maximum value is the larger of these two.

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