Animated Solution for Physics - Kinematics: Two identical boats are moving relative to the water current with equal speed vb/w=1.0 m/s. To a boy standing on the ground, the first boat appears moving perpendicular to the river current and to another boy standing on a raft in the river, the second boat appears moving perpendicular to the shoreline. In a certain time interval, distances of the boats from the shoreline increase by Δy1=4.0 m and Δy2=5.0 m respectively. Calculate speed of the river current.
Enter Numerical Value:
Visualized Solution
\text{Visualizing the River and Boats}
Let the river current velocity be vw=ui^.
Let the speed of boats relative to water be vb/w=v=1.0 m/s.
\text{Velocity of Boat 1}
To a boy on the ground, Boat 1 moves perpendicular to the river.
Absolute velocity v1=v1/w+vw.
Since v1⊥vw, v1 is strictly along the y-axis.
\text{Y-component of Boat 1}
From the right-angled vector triangle:
∣v1/w∣2=∣v1∣2+∣vw∣2
v2=v1y2+u2⟹v1y=v2−u2
\text{Velocity of Boat 2}
To a boy on a raft (moving with vw), Boat 2 moves perpendicular to the shoreline.
This means the relative velocity v2/w is strictly along the y-axis.
\text{Y-component of Boat 2}
Absolute velocity v2=v2/w+vw.
Since v2/w is along the y-axis, the y-component of absolute velocity is:
v2y=∣v2/w∣=v
\text{Relating Displacements}
In time Δt, the distances from the shoreline increase by:
Δy1=v1yΔt=v2−u2Δt
Δy2=v2yΔt=vΔt
\text{Eliminating } \Delta t
Divide the two displacement equations to eliminate Δt:
Δy2Δy1=vv2−u2
\text{Solving for River Speed } u
Square both sides:
Δy22Δy12=1−v2u2
v2u2=Δy22Δy22−Δy12
u=vΔy2Δy22−Δy12
\text{Final Calculation}
Substitute v=1.0, Δy1=4.0, Δy2=5.0:
u=1.0×5.05.02−4.02
u=5.025−16=53=0.6 m/s
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The Sigma Insight: Relative Velocity
Solution Diagram
The Tale of Two Observers
Imagine standing on the bank of a steadily flowing river. You watch two identical boats, both capable of the same speed relative to the water, attempt to cross.
However, they employ entirely different strategies, and their motions are judged by two different observers. This classic relative velocity problem is a beautiful exercise in understanding frames of reference.
Analyzing Boat 1
The Ground Perspective
For the first boat, a boy standing on the ground observes it moving straight across the river. This means the boat's absolute velocity, v1, is directed perfectly perpendicular to the shoreline.
To achieve this, the boat cannot simply point its nose straight across. If it did, the river would sweep it downstream. Instead, it must steer slightly upstream.
By doing so, the horizontal component of its velocity relative to the water exactly cancels out the river's current. We can visualize this with a right-angled vector triangle.
The hypotenuse is the boat's speed relative to the water, v. The base is the river's speed, u. Using the Pythagorean theorem, the vertical speed that actually carries the boat across the river is:
v1y=v2−u2
Analyzing Boat 2
The Raft Perspective
Now, let's shift our perspective to the second boat. This time, the observer is a boy on a raft drifting freely with the river current.
To this boy, the second boat appears to be moving straight across the river. Because the raft is moving at the exact speed of the river, it serves as a moving frame of reference.
If the boat appears to move straight across from this moving frame, it means the boat's velocity relative to the water, v2/w, is directed perfectly perpendicular to the shore.
Since the boat is pointing its nose straight across, its entire engine effort is dedicated to crossing the river. Therefore, its vertical speed is simply its full speed relative to the water:
v2y=v
The Master Equation
We are given a crucial piece of information: in a certain time interval Δt, the distances of the boats from the shoreline increase by Δy1 and Δy2 respectively.
Distance is simply vertical speed multiplied by time. We can write the displacement equations for both boats:
Δy1=v2−u2Δt
Δy2=vΔt
Since the time interval Δt is the same for both boats, we can elegantly eliminate it by dividing the first equation by the second. This gives us a ratio of their vertical displacements:
Δy2Δy1=vv2−u2
Final Calculation
Now, we just need to isolate the river's speed, u. Let's square both sides of our ratio equation to remove the square root:
Δy22Δy12=1−v2u2
Rearranging the terms to solve for u2/v2, we get:
v2u2=Δy22Δy22−Δy12
Taking the square root gives us the final algebraic expression for the river's speed:
u=vΔy2Δy22−Δy12
Finally, we substitute the given numerical values: v=1.0 m/s, Δy1=4.0 m, and Δy2=5.0 m.
Notice the numbers under the square root: 5.02−4.02. This is the classic 3-4-5 right triangle! The square root evaluates perfectly to 3.0.
u=1.0×5.03.0
u=0.6 m/s
The speed of the river current is exactly 0.6 m/s.