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Question

Question: Consider the diagram shown. A voltmeter of resistance \(150\Omega \) is connected across A and B. ...

Consider the diagram shown.
A voltmeter of resistance 150Ω150\Omega is connected across A and B. the potential drop across B and C measured by voltmeter is

a)29V
b)27V
c)31V
d)30V

Explanation

Solution

In the above question it is given to us that the voltmeter of resistance 150Ω150\Omega is connected in parallel with the resistance 100 ohms towards A. First we will determine the equivalent resistance in the circuit. Further using ohm's law we will determine the current in the circuit. Again using ohm's law we will determine the voltage across the BC.

Formula used:
V=IRV=IR
RP=rRR+r{{R}_{P}}=\dfrac{rR}{R+r}

Complete step by step answer:
Initially it is given to us that the voltmeter of resistance 150Ω150\Omega is connected across AB. If there are two resistors i.e. r and R connected in parallel, the equivalent resistance RP{{R}_{P}} in parallel is given by,
RP=rRR+r{{R}_{P}}=\dfrac{rR}{R+r}
Hence using this equation the net resistance across AB is equal to,
RP=rRR+r RP=150×100150+100=150×1025 RP=60Ω \begin{aligned} & {{R}_{P}}=\dfrac{rR}{R+r} \\\ & {{R}_{P}}=\dfrac{150\times 100}{150+100}=\dfrac{150\times 10}{25} \\\ & {{R}_{P}}=60\Omega \\\ \end{aligned}
Further since resistance in series gets added up, the resistance G between A and C is equal to 160 ohms.
Further using ohm's law i.e. V=IRV=IR (where V is the potential difference between the effective resistance R and I is the current in the circuit) the current in the circuit is equal to,
V=IR 50V=I160Ω I=516=0.31A \begin{aligned} & V=IR \\\ & \Rightarrow 50V=I160\Omega \\\ & \therefore I=\dfrac{5}{16}=0.31A \\\ \end{aligned}
Hence again using ohm's law, the voltage measure by the voltmeter between points B and C is equal to,
V=IR VBC=0.31×100=31V \begin{aligned} & V=IR \\\ & {{V}_{BC}}=0.31\times 100=31V \\\ \end{aligned}

So, the correct answer is “Option C”.

Note:
There are some of the key points that have to be remembered while solving any circuit. The current in series across the resistors remains the same whereas the current in parallel gets distributed across different branches. Similarly the voltage in parallel across the resistors remains the same, whereas the voltage in series circuit gets added up. Considering these points in mind we can solve the basic circuit diagrams easily.