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ElectricalMachine
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What is the formula of the ratio of the lower limit to the upper limit of current?

A

I2I1=R2R1=R3R2=R4R3=Rn+1RnI_{2}I_{1} = R_{2}R_{1} = R_{3}R_{2} = R_{4}R_{3} = R n_{+ 1 R n}I2тАЛI1тАЛ=R2тАЛR1тАЛ=R3тАЛR2тАЛ=R4тАЛR3тАЛ=Rn+1RnтАЛ

B

I2I1=raR11nI_{2}I_{1} = r_{a}R_{1} \frac{1}{n}I2тАЛI1тАЛ=raтАЛR1тАЛn1тАЛ

C

I2I1=Rn+1R11nI_{2}I_{1} = R n_{+ 1 R 1} \frac{1}{n}I2тАЛI1тАЛ=Rn+1R1тАЛn1тАЛ

D

All of these

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalMachine
Option D

All of these

Quick Summary:

In DC motor starters, particularly three-point and four-point starters with graded resistance sections, the upper limit of current I1I_1I1тАЛ and lower limit of current I2I_2I2тАЛ are held between constant limits during the starting process. The ratio of the lower limit to upper limit of current, I2I1\frac{I_2}{I_1}I1тАЛI2тАЛтАЛ, is related to the resistance steps by I2I1=R2R1=R3R2=тЛп=Rn+1Rn=(Rn+1R1)1n\frac{I_2}{I_1} = \frac{R_2}{R_1} = \frac{R_3}{R_2} = \dots = \frac{R_{n+1}}{R_n} = \left(\frac{R_{n+1}}{R_1}\right)^{\frac{1}{n}}I1тАЛI2тАЛтАЛ=R1тАЛR2тАЛтАЛ=R2тАЛR3тАЛтАЛ=тЛп=RnтАЛRn+1тАЛтАЛ=(R1тАЛRn+1тАЛтАЛ)n1тАЛ. Since armature resistance ra=Rn+1r_a = R_{n+1}raтАЛ=Rn+1тАЛ, option B is an equivalent representation, making 'All of these' the correct answer.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

In DC motor starters, particularly three-point and four-point starters with graded resistance sections, the upper limit of current I1I_1I1тАЛ and lower limit of current I2I_2I2тАЛ are held between constant limits during the starting process. The ratio of the lower limit to upper limit of current, I2I1\frac{I_2}{I_1}I1тАЛI2тАЛтАЛ, is related to the resistance steps by I2I1=R2R1=R3R2=тЛп=Rn+1Rn=(Rn+1R1)1n\frac{I_2}{I_1} = \frac{R_2}{R_1} = \frac{R_3}{R_2} = \dots = \frac{R_{n+1}}{R_n} = \left(\frac{R_{n+1}}{R_1}\right)^{\frac{1}{n}}I1тАЛI2тАЛтАЛ=R1тАЛR2тАЛтАЛ=R2тАЛR3тАЛтАЛ=тЛп=RnтАЛRn+1тАЛтАЛ=(R1тАЛRn+1тАЛтАЛ)n1тАЛ. Since armature resistance ra=Rn+1r_a = R_{n+1}raтАЛ=Rn+1тАЛ, option B is an equivalent representation, making 'All of these' the correct answer.

ЁЯФв Key Formulas

I2I1=Rk+1Rk\frac{I_2}{I_1} = \frac{R_{k+1}}{R_k}I1тАЛI2тАЛтАЛ=RkтАЛRk+1тАЛтАЛ тАФ Ratio of lower to upper current limit for each stud section

I2I1=(Rn+1R1)1n=(raR1)1n\frac{I_2}{I_1} = \left(\frac{R_{n+1}}{R_1}\right)^{\frac{1}{n}} = \left(\frac{r_a}{R_1}\right)^{\frac{1}{n}}I1тАЛI2тАЛтАЛ=(R1тАЛRn+1тАЛтАЛ)n1тАЛ=(R1тАЛraтАЛтАЛ)n1тАЛ тАФ Current ratio expressed in terms of total starting resistance and armature resistance

тЪЩя╕П Working Principle

During starting, as the starter handle is moved from stud to stud, the current fluctuates between I1I_1I1тАЛ (upper limit) and I2I_2I2тАЛ (lower limit). To keep current fluctuations uniform across all studs, the resistance of the sections forms a geometric progression. Taking the product of nnn equal resistance ratio steps yields (I2I1)n=Rn+1R1\left(\frac{I_2}{I_1}\right)^n = \frac{R_{n+1}}{R_1}(I1тАЛI2тАЛтАЛ)n=R1тАЛRn+1тАЛтАЛ, which gives I2I1=(Rn+1R1)1n=(raR1)1n\frac{I_2}{I_1} = \left(\frac{R_{n+1}}{R_1}\right)^{\frac{1}{n}} = \left(\frac{r_a}{R_1}\right)^{\frac{1}{n}}I1тАЛI2тАЛтАЛ=(R1тАЛRn+1тАЛтАЛ)n1тАЛ=(R1тАЛraтАЛтАЛ)n1тАЛ.

ЁЯУМ Key Points
  • тЦ╕

    To minimize current surges, starter resistance sections are designed such that resistance values form a geometric progression.

  • тЦ╕

    The total number of resistance steps is denoted by nnn, with n+1n+1n+1 total resistance values from R1R_1R1тАЛ (total resistance) down to Rn+1=raR_{n+1} = r_aRn+1тАЛ=raтАЛ (armature resistance).

  • тЦ╕

    Since R2R1=R3R2=тЛп=Rn+1Rn\frac{R_2}{R_1} = \frac{R_3}{R_2} = \dots = \frac{R_{n+1}}{R_n}R1тАЛR2тАЛтАЛ=R2тАЛR3тАЛтАЛ=тЛп=RnтАЛRn+1тАЛтАЛ, the product of these nnn ratios is Rn+1R1=(I2I1)n\frac{R_{n+1}}{R_1} = \left(\frac{I_2}{I_1}\right)^nR1тАЛRn+1тАЛтАЛ=(I1тАЛI2тАЛтАЛ)n.

тЬЕ Advantages
  • тЦ╕

    Ensures uniform current limits during motor acceleration

  • тЦ╕

    Prevents thermal damage to armature windings by limiting peak currents

тЭМ Disadvantages / Limitations
  • тЦ╕

    Requires precise calculation and tapering of resistance values

  • тЦ╕

    Energy is dissipated as heat in starting resistors during start-up

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Design of three-point and four-point starters for DC shunt and compound motors

  • тЦ╕

    Design of rotor resistance starters for 3-phase slip ring induction motors

ЁЯУД Additional Information
  • тЦ╕

    Option A gives the step-by-step resistance ratio equivalence to current ratio.

  • тЦ╕

    Option B substitutes armature resistance rar_araтАЛ in place of Rn+1R_{n+1}Rn+1тАЛ.

  • тЦ╕

    Option C presents the standard nth root form involving total resistance R1R_1R1тАЛ and final resistance step Rn+1R_{n+1}Rn+1тАЛ.

  • тЦ╕

    Therefore, options A, B, and C are all valid expressions for the current limit ratio.

ЁЯУК Diagram / Illustration
DC Motor Starter Resistance Steps RatioCurrent Ratio between consecutive studs:IтВВ (Lower Current Limit)IтВБ (Upper Current Limit)= RтВВ / RтВБ = RтВГ / RтВВ = ... = RтВЩтВКтВБ / RтВЩIтВВ / IтВБ = ( RтВЩтВКтВБ / RтВБ )^(1/n)where RтВЩтВКтВБ = Armature Resistance (rтВР)
тЬЕ

D is correct тАФ All three equations correctly represent the ratio of lower current limit to upper current limit (I2I1\frac{I_2}{I_1}I1тАЛI2тАЛтАЛ) in DC motor starter design.

Core Concepts Used
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DC Motor Starter Resistance Calculation Upper and Lower Current Limits during Starting Geometric Progression in Starter Resistors
ЁЯТб EXAM TIP

In competitive exams like GATE and ESE, remember that if starter resistance steps form a GP, the common ratio K=I2I1=(raR1)1/nK = \frac{I_2}{I_1} = \left(\frac{r_a}{R_1}\right)^{1/n}K=I1тАЛI2тАЛтАЛ=(R1тАЛraтАЛтАЛ)1/n. Number of studs is always n+1n+1n+1 where nnn is the number of resistance sections.

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