To solve this problem, we need to understand the physics behind beats in sound waves. When two sound waves of slightly different frequencies are played together, they produce a phenomenon known as "beats." The beat frequency is the absolute difference between the two sound frequencies.
The formula for beat frequency is given by:
f_{\text{beats}} = |f_1 - f_2|
Given that at 16°C, these organ pipes produce 34 beats in 2 seconds, the beat frequency at this temperature is:
f_{\text{beats}, 16^{\circ}C} = \frac{34}{2} = 17 \text{ beats per second}
In this problem, we assume the length of the pipes doesn't change, so any change in frequency is due entirely to the speed of sound, which depends on temperature.
The speed of sound in air is approximately given by:
v = v_0 \sqrt{\frac{T}{T_0}}
where v_0 is the speed of sound at a reference temperature T_0 (usually taken as 273 K), and T is the current temperature in Kelvin.
Here, we need to find the beat frequency at 51°C. Using the ratio of speeds at different temperatures:
\frac{v_{51^{\circ}C}}{v_{16^{\circ}C}} = \sqrt{\frac{273 + 51}{273 + 16}}
Calculating the above expression gives us:
\sqrt{\frac{324}{289}} \approx 1.0595
This means the frequency at 51°C increases by approximately 5.95% compared to the frequency at 16°C.
The new beat frequency at 51°C is:
f_{\text{beats}, 51^{\circ}C} = 17 \times 1.0595 \approx 18 \text{ beats per second}
Thus, the number of beats per second when the temperature rises to 51°C is 18, which matches option (A).
The correct option is:
(A) 18
Two resistances of 100Ω and 200Ω are connected in series with a battery of 4V and negligible internal resistance. A voltmeter is used to measure voltage across the 100Ω resistance, which gives a reading of 1V. The resistance of the voltmeter must be _____ Ω.