If two vectors a and b are collinear, one can always find a…
If two vectors $\vec{a}$ and $\vec{b}$ are collinear, one can always find a constant $\lambda$ such that $\vec{a} = \lambda\vec{b}$, or two constants $\alpha$ and $\beta$ such that $\alpha\vec{a}+\beta\vec{b} = \vec{0}$. What is the relation between the constants $\lambda$, $\alpha$ and $\beta$? Determine $\alpha$ if $\lambda = 1$, $\beta = 2$.
Explanation of Method
Collinear vectors — relation between the constants $\lambda$, $\alpha$ and $\beta$.
Step 1: Collinearity condition
Two vectors $\vec{a}$ and $\vec{b}$ ($\vec b\neq\vec 0$) are collinear if and only if one is a scalar multiple of the other: $\vec{a} = \lambda\vec{b}$.
Step 2: Relation between $\lambda$, $\alpha$ and $\beta$
Take $\alpha\vec{a}+\beta\vec{b} = \vec{0}$ with $\alpha \neq 0$ and divide by $\alpha$: \[\vec{a} + \frac{\beta}{\alpha}\vec{b} = \vec{0} \quad\Longrightarrow\quad \vec{a} = -\frac{\beta}{\alpha}\vec{b}.\]
Comparing with $\vec{a} = \lambda\vec{b}$: \[\lambda = -\frac{\beta}{\alpha}, \qquad \alpha = -\frac{\beta}{\lambda}, \qquad \beta = -\alpha\lambda\]
So $\alpha$ and $\beta$ have opposite signs when $\lambda \gt 0$ (codirectional vectors) and the same sign when $\lambda \lt 0$ (antiparallel vectors).
Step 3: Interpretation
The condition $\alpha\vec{a}+\beta\vec{b}=\vec{0}$ with $\alpha,\beta$ not both zero is the definition of linear dependence: two vectors are collinear exactly when they are linearly dependent. The relation $\lambda = -\beta/\alpha$ shows that any two of the three constants determine the third.
Step 4: Special case: $\lambda = 1$, $\beta = 2$
\[ \alpha = -\frac{\beta}{\lambda} = -\frac{2}{1} = -2 \]
\[\alpha = -2\]
Verification
With $\lambda = 1$ we have $\vec{a} = \vec{b}$, so
\[ \alpha\vec{a}+\beta\vec{b} = -2\vec{a}+2\vec{b} = 2(\vec{b}-\vec{a}) = \vec{0} \;\checkmark, \qquad \lambda = -\frac{\beta}{\alpha} = -\frac{2}{-2} = 1 \;\checkmark \]
Result
| Known | Find | Formula |
|---|---|---|
| $\lambda,\ \beta$ | $\alpha$ | $\alpha = -\dfrac{\beta}{\lambda}$ |
| $\lambda,\ \alpha$ | $\beta$ | $\beta = -\alpha\lambda$ |
| $\alpha,\ \beta$ | $\lambda$ | $\lambda = -\dfrac{\beta}{\alpha}$ |