Rotating Light vs Wall: Related-Rates Analysis
Problem Setup
Scenario: A beacon/light rotates in a horizontal circle and projects a spot onto a vertical wall.
Fixed distance from light to wall: 12\text{ ft} (adjacent side in a right triangle).
The light completes one full revolution in 4\text{ s}.
At the instant of interest, the beam makes a 10^{\circ} angle ((\theta)) with the perpendicular (normal) to the wall.
Unknown required: the speed at which the light spot moves along the wall, i.e. \frac{dw}{dt} where (w) = horizontal distance the spot has travelled from the foot of the perpendicular.
Expected unit for the answer: \text{ft/s}.
Key Variables
(\theta): instantaneous angle between the beam and the perpendicular to the wall (NOT the wall itself). (Perpendicular means a line extending straight out from the wall.)
(w): length of the segment along the wall from the perpendicular foot to the projected light spot (opposite side of the right triangle).
Time variable: t (seconds).
Known Rates & Conversions
1 revolution = 2\pi\text{ rad}
Rotation period =4\text{ s} (\Rightarrow) angular speed
\frac{d\theta}{dt}=\frac{2\pi \text{ rad}}{4\text{ s}} = \frac{\pi}{2}\; \text{rad/s}.
Geometric Relation
Right triangle with
opposite side = w
adjacent side = 12
Tangent function:
\tan\theta = \frac{w}{12}.
Differentiate Implicitly (Related-Rates)
Differentiate both sides with respect to time t:
Left side: derivative of \tan\theta is \sec^{2}\theta, followed by chain rule factor \frac{d\theta}{dt}.
Right side: \frac{d}{dt}\left(\frac{w}{12}\right)=\frac{1}{12}\frac{dw}{dt}.
Putting it together:
\sec^{2}\theta\,\frac{d\theta}{dt}=\frac{1}{12}\frac{dw}{dt}.
Solve for \frac{dw}{dt}:
\frac{dw}{dt}=12\,\sec^{2}\theta\,\frac{d\theta}{dt}.
Plug In Numerical Values
At the instant considered, (\theta = 10^{\circ}) (convert? We may leave in degrees but the calculator must be in degree mode) and \frac{d\theta}{dt}=\frac{\pi}{2}\text{ rad/s}.
Compute symbolically first:
\frac{dw}{dt}=12 \cdot \sec^{2}(10^{\circ}) \cdot \frac{\pi}{2}
= 6\pi\, \sec^{2}(10^{\circ}).
Because most calculators lack a direct secant key, rewrite using cosine:
\sec^{2}(10^{\circ}) = \left(\frac{1}{\cos 10^{\circ}}\right)^{2}
\frac{dw}{dt}=6\pi\left(\frac{1}{\cos 10^{\circ}}\right)^{2}.
Numerical Approximation
Ensure calculator is in DEGREE mode.
Evaluate:
\cos 10^{\circ}\approx 0.984807753.
Reciprocal squared: \left(\frac{1}{0.984807753}\right)^{2}\approx 1.0301537.
Multiply by 6\pi \;(\approx 18.84955592):
18.84955592\times1.0301537\approx19.4356.
Rounded result:
\boxed{\frac{dw}{dt}\,\approx\,19.44\ \text{ft/s}}
Interpretation & Contextual Notes
The spot races fastest when the beam is nearly parallel to the wall (larger (\theta)). At (\theta=0^{\circ}) (directly perpendicular), the speed would be zero.
Changing either the angular velocity ((d\theta/dt)) or the distance from the light to the wall alters the linear speed proportionally.
Under the given parameters, every four seconds the beam resets; whenever it reaches a small (10^{\circ}) deviation from the normal, the spot is already sliding across the wall at almost 20\text{ ft/s}.
Mathematical / Calculus Connections
Classic "related-rates" problem: convert rotational/angular motion into linear motion using trigonometric relations.
Utilizes chain rule for differentiating composite functions ((\tan\theta) where (\theta=\theta(t))).
Implicit differentiation because (\theta) and (w) are both functions of time, not explicit functions of one another.
Reinforces reciprocal-trig identity: \sec \theta = \frac{1}{\cos \theta}.
Highlights importance of unit consistency: radians for derivatives of trig functions, degrees must be converted or calculator set appropriately.
Practical Implications
This style of reasoning models lighthouse beams, radar sweeps, rotating lasers in industry, or security scans.
Safety calculations (e.g.
laser scanning speed across human vision) rely on similar conversions from angular speed to linear wall/ground speed.
Summary of Final Answer
At (\theta=10^{\circ}) and rotation period 4\text{ s},
\frac{dw}{dt}\approx19.44\text{ ft/s}.