Animated Solution for Mathematics - Vector Algebra: Let u,v,w be such that ∣u∣=1,∣v∣=2,∣w∣=3. If the projection v along u is equal to that of w along u and v,w are perpendicular to each other then ∣u−v+w∣ equals
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Visualized Solution
Given Magnitudes
Let's visualize the vectors u, v, and w.
Given magnitudes:
∣u∣=1
∣v∣=2
∣w∣=3
Projection Concept
The projection of a vector a along b is given by ∣b∣a⋅b.
Projection of v along u=∣u∣v⋅u
Projection of w along u=∣u∣w⋅u
Equating Projections
The problem states that the projection of v along u equals the projection of w along u.
⟹∣u∣v⋅u=∣u∣w⋅u
Simplifying the Equation
Since ∣u∣=1, the denominators become 1.
1v⋅u=1w⋅u
⟹v⋅u=w⋅u
Perpendicularity Condition
Given: v and w are perpendicular to each other (v⊥w).
For perpendicular vectors, their dot product is zero.
⟹v⋅w=0
Expansion Identity
We need to find the value of ∣u−v+w∣.
To deal with magnitudes of vector sums, we square the expression.
Using the identity: ∣a+b+c∣2=∣a∣2+∣b∣2+∣c∣2+2(a⋅b+b⋅c+c⋅a)
Applying the Identity
Let a=u, b=−v, and c=w.
∣u−v+w∣2=∣u∣2+∣−v∣2+∣w∣2+2(u⋅(−v)+(−v)⋅w+w⋅u)
Simplifying the Expansion
Note that ∣−v∣2=∣v∣2.
Pulling out the negative signs from the dot products:
=∣u∣2+∣v∣2+∣w∣2−2(u⋅v)−2(v⋅w)+2(w⋅u)
Using Perpendicularity
From Step 5, we know v⋅w=0.
Substituting this into our expression:
=∣u∣2+∣v∣2+∣w∣2−2(u⋅v)−2(0)+2(w⋅u)
=∣u∣2+∣v∣2+∣w∣2−2(u⋅v)+2(w⋅u)
Grouping and Canceling Terms
Let's group the remaining dot product terms:
=∣u∣2+∣v∣2+∣w∣2−2(u⋅v−w⋅u)
From Step 4, v⋅u=w⋅u.
Therefore, u⋅v−w⋅u=0.
The expression reduces to: ∣u∣2+∣v∣2+∣w∣2
Substituting Magnitudes
We are left with: ∣u∣2+∣v∣2+∣w∣2
Substitute the given values: ∣u∣=1, ∣v∣=2, ∣w∣=3
=(1)2+(2)2+(3)2
Calculating the Sum
Evaluate the squares:
=1+4+9
Add them up:
=14
Final Answer
We found: ∣u−v+w∣2=14
Taking the square root of both sides:
∣u−v+w∣=14
Conclusion: The correct option is 14.
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The Sigma Insight: Scalar (Dot) Product
Solution Diagram
The Symphony of Vectors
A Journey into Geometric Elegance
Welcome, future engineer. Today, we are not just solving a vector problem; we are conducting a symphony. In the world of JEE Advanced, vectors are not just arrows on a page—they are the fundamental language of physics.
When you look at a problem involving magnitudes, projections, and perpendicularity, do not feel intimidated. Instead, look for the hidden symmetries. Let us break this down, step by step, and uncover the elegance hidden within the algebra.
Phase 1
Decoding the Projections
Imagine you are standing in a room with a single light source directly above a line defined by vector u. If you hold vector v and vector w in the air, they will cast shadows on that line.
The problem tells us something profound: the shadow of v is identical to the shadow of w. Mathematically, the projection of a vector a along b is defined as ∣b∣a⋅b.
Since the problem states that the projection of v along u equals the projection of w along u, we write:
∣u∣v⋅u=∣u∣w⋅u
Because ∣u∣=1, the denominators vanish, leaving us with a beautiful, simple truth: v⋅u=w⋅u. This is our first key. Keep it safe; we will need it later.
Phase 2
The Gift of Perpendicularity
Next, the problem gives us a gift: v and w are perpendicular. In the language of dot products, perpendicularity is synonymous with zero.
When two vectors are at a 90∘ angle, their dot product is zero because cos(90∘)=0. Thus, v⋅w=0.
This is a massive simplification. Whenever you see 'perpendicular' in a vector problem, immediately think: 'This term is going to vanish.'
Phase 3
The Squaring Strategy
Now, we face the main challenge: finding the magnitude ∣u−v+w∣. Dealing with the magnitude of a sum of three vectors is daunting. We cannot simply add the lengths.
The standard JEE strategy here is to square the entire expression. Why? Because the square of a magnitude is the dot product of the vector with itself, which allows us to distribute the terms.
Let us expand ∣u−v+w∣2 using the identity for the square of a trinomial:
∣u−v+w∣2=∣u∣2+∣−v∣2+∣w∣2+2(u⋅(−v)+(−v)⋅w+w⋅u)
Let us clean this up. We know that ∣−v∣2=∣v∣2. Distributing the dot products, we get:
=∣u∣2+∣v∣2+∣w∣2−2(u⋅v)−2(v⋅w)+2(w⋅u)
Phase 4
The Grand Cancellation
This is where the magic happens. Look at the terms we have generated. We know v⋅w=0, so the term −2(v⋅w) disappears entirely.
We are left with:
=∣u∣2+∣v∣2+∣w∣2−2(u⋅v)+2(w⋅u)
Recall our finding from Phase 1: u⋅v=w⋅u. If we substitute w⋅u for u⋅v, the expression becomes:
=∣u∣2+∣v∣2+∣w∣2−2(w⋅u)+2(w⋅u)
Everything cancels out! The cross-terms are gone, leaving us with the sum of the squares of the magnitudes. This is the elegance of vector algebra. We are left with:
=∣u∣2+∣v∣2+∣w∣2
Substituting the given values ∣u∣=1, ∣v∣=2, and ∣w∣=3:
=(1)2+(2)2+(3)2=1+4+9=14
Finally, taking the square root, we arrive at our answer: 14. You have successfully navigated the complexity and found the simple, beautiful truth underneath. Keep this mindset—look for the cancellations, trust the algebra, and you will conquer any problem.