Consider the following equations for two vectors \(\vec{a}\) and \(\vec{b}\) 1. \(\left( \vec{a}+\vec{b} \right)\cdot \left( \vec{a}-\vec{b} \right)={{\left| {\vec{a}} \right|}^{2}}-{{\left| {\vec{b}} \right|}^{2}}\) 2. \(\left( \left| \vec{a}+\vec{b} \right| \right)\left( \left| \vec{a}-\vec{b} \right| \right)={{\left| {\vec{a}} \right|}^{2}}-{{\left| {\vec{b}} \right|}^{2}}\) 3. \({{\left| \vec{a}\cdot \vec{b} \right|}^{2}}+{{\left| \vec{a}\times \vec{b} \right|}^{2}}={{\left| {\vec{a}} \right|}^{2}}{{\left| {\vec{b}} \right|}^{2}}\)
1 and 3 only
This question asks us to evaluate the correctness of three given vector equations involving vector addition, subtraction, dot product, cross product, and vector magnitudes. Let's analyze each statement carefully using fundamental vector properties.
Statement 1 is: \( \left( \vec{a}+\vec{b} \right)\cdot \left( \vec{a}-\vec{b} \right)={{\left| {\vec{a}} \right|}^{2}}-{{\left| {\vec{b}} \right|}^{2}} \)
To verify this, we can expand the left side using the distributive property of the dot product, similar to how we expand algebraic expressions:
Left Side (LS) \( = \left( \vec{a}+\vec{b} \right)\cdot \left( \vec{a}-\vec{b} \right) \)
\( = \vec{a} \cdot \vec{a} + \vec{a} \cdot (-\vec{b}) + \vec{b} \cdot \vec{a} + \vec{b} \cdot (-\vec{b}) \)
\( = \vec{a} \cdot \vec{a} - \vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{a} - \vec{b} \cdot \vec{b} \)
We know that \( \vec{a} \cdot \vec{a} = |\vec{a}|^2 \) and \( \vec{b} \cdot \vec{b} = |\vec{b}|^2 \). Also, the dot product is commutative, meaning \( \vec{a} \cdot \vec{b} = \vec{b} \cdot \vec{a} \). Substituting these into the expression:
\( = |\vec{a}|^2 - \vec{a} \cdot \vec{b} + \vec{a} \cdot \vec{b} - |\vec{b}|^2 \)
\( = |\vec{a}|^2 - |\vec{b}|^2 \)
This matches the Right Side (RS) of the equation. Therefore, statement 1 is correct.
Statement 2 is: \( \left( \left| \vec{a}+\vec{b} \right| \right)\left( \left| \vec{a}-\vec{b} \right| \right)={{\left| {\vec{a}} \right|}^{2}}-{{\left| {\vec{b}} \right|}^{2}} \)
Let's consider the squares of the magnitudes first:
\( |\vec{a}+\vec{b}|^2 = (\vec{a}+\vec{b}) \cdot (\vec{a}+\vec{b}) = \vec{a} \cdot \vec{a} + \vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{a} + \vec{b} \cdot \vec{b} = |\vec{a}|^2 + 2(\vec{a} \cdot \vec{b}) + |\vec{b}|^2 \)
\( |\vec{a}-\vec{b}|^2 = (\vec{a}-\vec{b}) \cdot (\vec{a}-\vec{b}) = \vec{a} \cdot \vec{a} - \vec{a} \cdot \vec{b} - \vec{b} \cdot \vec{a} + \vec{b} \cdot \vec{b} = |\vec{a}|^2 - 2(\vec{a} \cdot \vec{b}) + |\vec{b}|^2 \)
The left side of statement 2 is \( \left| \vec{a}+\vec{b} \right| \left| \vec{a}-\vec{b} \right| \). If we square this, we get \( \left( \left| \vec{a}+\vec{b} \right| \left| \vec{a}-\vec{b} \right| \right)^2 = |\vec{a}+\vec{b}|^2 |\vec{a}-\vec{b}|^2 \). For statement 2 to be correct, its square must equal the square of the right side:
\( (|\vec{a}|^2 - |\vec{b}|^2)^2 = (|\vec{a}|^2)^2 - 2|\vec{a}|^2 |\vec{b}|^2 + (|\vec{b}|^2)^2 = |\vec{a}|^4 - 2|\vec{a}|^2 |\vec{b}|^2 + |\vec{b}|^4 \)
Now let's look at \( |\vec{a}+\vec{b}|^2 |\vec{a}-\vec{b}|^2 \):
\( = (|\vec{a}|^2 + 2(\vec{a} \cdot \vec{b}) + |\vec{b}|^2) (|\vec{a}|^2 - 2(\vec{a} \cdot \vec{b}) + |\vec{b}|^2) \)
Let \( X = |\vec{a}|^2 + |\vec{b}|^2 \) and \( Y = 2(\vec{a} \cdot \vec{b}) \). The expression becomes \( (X+Y)(X-Y) = X^2 - Y^2 \).
\( = (|\vec{a}|^2 + |\vec{b}|^2)^2 - (2(\vec{a} \cdot \vec{b}))^2 \)
\( = (|\vec{a}|^4 + 2|\vec{a}|^2 |\vec{b}|^2 + |\vec{b}|^4) - 4(\vec{a} \cdot \vec{b})^2 \)
Comparing this with \( |\vec{a}|^4 - 2|\vec{a}|^2 |\vec{b}|^2 + |\vec{b}|^4 \), they are clearly not equal for general vectors unless \( 4|\vec{a}|^2 |\vec{b}|^2 - 4(\vec{a} \cdot \vec{b})^2 = 0 \), which is not always true. For instance, if \(\vec{a}\) and \(\vec{b}\) are orthogonal (\(\vec{a} \cdot \vec{b} = 0\)), then \( |\vec{a}+\vec{b}|^2 = |\vec{a}|^2 + |\vec{b}|^2 \) and \( |\vec{a}-\vec{b}|^2 = |\vec{a}|^2 + |\vec{b}|^2 \). The left side of statement 2 becomes \( \sqrt{|\vec{a}|^2 + |\vec{b}|^2} \sqrt{|\vec{a}|^2 + |\vec{b}|^2} = |\vec{a}|^2 + |\vec{b}|^2 \). The right side is \( |\vec{a}|^2 - |\vec{b}|^2 \). These are only equal if \( 2|\vec{b}|^2 = 0 \), i.e., \( |\vec{b}|=0 \). Thus, statement 2 is not correct for all vectors \(\vec{a}\) and \(\vec{b}\).
Statement 3 is: \( {{\left| \vec{a}\cdot \vec{b} \right|}^{2}}+{{\left| \vec{a}\times \vec{b} \right|}^{2}}={{\left| {\vec{a}} \right|}^{2}}{{\left| {\vec{b}} \right|}^{2}} \)
We know the definitions of the dot product and the magnitude of the cross product in terms of the angle \( \theta \) between vectors \(\vec{a}\) and \(\vec{b}\):
\( \vec{a} \cdot \vec{b} = |\vec{a}| |\vec{b}| \cos \theta \)
\( |\vec{a} \times \vec{b}| = |\vec{a}| |\vec{b}| \sin \theta \)
Substitute these into the left side of statement 3:
LS \( = |\vec{a} \cdot \vec{b}|^2 + |\vec{a} \times \vec{b}|^2 \)
Since the terms inside the magnitudes are already magnitudes, the absolute value bars around the dot product and cross product magnitude are redundant when squaring, but let's keep them for consistency with the statement notation:
\( = \left( \left| |\vec{a}| |\vec{b}| \cos \theta \right| \right)^2 + \left( \left| |\vec{a}| |\vec{b}| \sin \theta \right| \right)^2 \)
Assuming \( \theta \) is in the range \( 0 \le \theta \le \pi \), \( \sin \theta \ge 0 \). \( \cos \theta \) can be positive or negative. However, squaring makes the result positive.
\( = (|\vec{a}| |\vec{b}| \cos \theta)^2 + (|\vec{a}| |\vec{b}| \sin \theta)^2 \)
\( = |\vec{a}|^2 |\vec{b}|^2 \cos^2 \theta + |\vec{a}|^2 |\vec{b}|^2 \sin^2 \theta \)
\( = |\vec{a}|^2 |\vec{b}|^2 (\cos^2 \theta + \sin^2 \theta) \)
Using the trigonometric identity \( \cos^2 \theta + \sin^2 \theta = 1 \):
\( = |\vec{a}|^2 |\vec{b}|^2 (1) \)
\( = |\vec{a}|^2 |\vec{b}|^2 \)
This matches the Right Side (RS) of the equation. Therefore, statement 3 is correct. This identity is sometimes known as Lagrange's identity in vector form.
| Statement | Equation | Correctness | Reason |
|---|---|---|---|
| 1 | \( \left( \vec{a}+\vec{b} \right)\cdot \left( \vec{a}-\vec{b} \right)={{\left| {\vec{a}} \right|}^{2}}-{{\left| {\vec{b}} \right|}^{2}} \) | Correct | Follows from distributive property of dot product and \( \vec{v} \cdot \vec{v} = |\vec{v}|^2 \). |
| 2 | \( \left( \left| \vec{a}+\vec{b} \right| \right)\left( \left| \vec{a}-\vec{b} \right| \right)={{\left| {\vec{a}} \right|}^{2}}-{{\left| {\vec{b}} \right|}^{2}} \) | Incorrect | Does not hold for general vectors; shown with counter-example (orthogonal vectors). |
| 3 | \( {{\left| \vec{a}\cdot \vec{b} \right|}^{2}}+{{\left| \vec{a}\times \vec{b} \right|}^{2}}={{\left| {\vec{a}} \right|}^{2}}{{\left| {\vec{b}} \right|}^{2}} \) | Correct | Follows from definitions of dot product and cross product magnitude in terms of angle \(\theta\) and \( \cos^2 \theta + \sin^2 \theta = 1 \). |
Based on our analysis, statements 1 and 3 are correct, while statement 2 is incorrect.
| Property | Description | Formula |
|---|---|---|
| Dot Product Commutativity | Order of vectors in dot product does not matter. | \( \vec{a} \cdot \vec{b} = \vec{b} \cdot \vec{a} \) |
| Dot Product Distributivity | Dot product distributes over vector addition. | \( \vec{a} \cdot (\vec{b} + \vec{c}) = \vec{a} \cdot \vec{b} + \vec{a} \cdot \vec{c} \) |
| Magnitude Squared | The square of a vector's magnitude is the dot product of the vector with itself. | \( |\vec{v}|^2 = \vec{v} \cdot \vec{v} \) |
| Dot Product Definition | Geometric definition involving magnitudes and angle. | \( \vec{a} \cdot \vec{b} = |\vec{a}| |\vec{b}| \cos \theta \) |
| Cross Product Magnitude Definition | Geometric definition involving magnitudes, angle, and area of parallelogram. | \( |\vec{a} \times \vec{b}| = |\vec{a}| |\vec{b}| \sin \theta \) |
| Lagrange's Identity (Vector Form) | Relates magnitudes of dot and cross products to vector magnitudes. | \( (\vec{a} \cdot \vec{b})^2 + |\vec{a} \times \vec{b}|^2 = |\vec{a}|^2 |\vec{b}|^2 \) |
Vector operations like the dot product and cross product are fundamental in physics and engineering. They provide ways to multiply vectors, resulting in either a scalar (dot product) or a vector (cross product).
Understanding these operations and their properties, such as the distributive property for dot product or the relationship between dot and cross product magnitudes shown in statement 3, is crucial for solving problems in vector algebra.
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