{"id":2731,"date":"2018-05-17T12:08:04","date_gmt":"2018-05-17T12:08:04","guid":{"rendered":"https:\/\/35.94.173.37\/blog\/?p=2731"},"modified":"2024-11-05T12:08:56","modified_gmt":"2024-11-05T12:08:56","slug":"calculating-the-resistance-of-multirange-multipliers","status":"publish","type":"post","link":"https:\/\/www.apexwaves.com\/blog\/calculating-the-resistance-of-multirange-multipliers\/","title":{"rendered":"Calculating the Resistance of Multirange Multipliers"},"content":{"rendered":"<p>There are two methods of calculating the values of multiplier resistors for a multirange voltmeter. In the first method, each multiplier is calculated the same as for a single-range voltmeter. Assume that you wish to extend the range of a 1-mA movement to measure 0- 10, 0- 100, and 0- 1000 volts, and you also want a 0- 1-V range. Since full-scale deflection equals 1 Von the 0- 1-V range (V = IM RM = 0.001 A x 1000 Q = I volt), no multiplier is needed. The total resistance (RT OT) needed to limit meter current (IM) to 1 mA on the 0- 10-V range is RrnT = V w vJ IM\u00a0\u00a0 =\u00a0\u00a0 10 V\/ 0.001A=\u00a0\u00a0\u00a0 10,000 Q<\/p>\n<p>&nbsp;<\/p>\n<p>Since the resistance of the meter (RM) is 1000 ohms, then the multiplier resistance RMuLT is 9000 ohms. A second method of calculating the values of voltmeter multiplier resistors is the series-multiplier arrangement in which the multiplier resistors are connected in series. R1 is the multiplier resistor for the 0-10 volt range. For the 0- 100-V range, R1 is in series with R2. Therefore, the value of the multiplier resistance for the 0- 100-V range is equal to R1 plus R2. Similarly, the multiplier resistance for the 0-1000-V range is equal to R1 plus R2 plus R3.<\/p>\n<p>Now, let\u2019s calculate the values for a series multiplier voltmeter. We will use the same 1-mA, 1000-Q meter movement that we used previously. Since this movement indicates 1 volt for a full-scale deflection, no multiplier resistor is needed for the 0- 1-V range. Therefore, your first step is to calculate the multiplier resistance needed for the 0- 10-V range. Again, using Ohm\u2019s law, find the total resistance (RToT) needed to limit meter current (IM) to 1 mA at this range:<\/p>\n<p>RrnT = V w.xl lM\u00a0\u00a0\u00a0\u00a0 = 10 V\/ 0.001 A = 10,000 Q<\/p>\n<p>Therefore, multiplier resistor R1 for the 0-10-V range equals 10,000n minus the 1000-Qmeter resistance, or 9000 n. Thus far, the procedure is the same as in the other method, and the value of the multiplier resistor is the same for the 0- 10-V range. Having found the series multipliers for the 0- 1- and 0- 10-V ranges, let\u2019s calculate the total resistance needed for the 0- 100-Vrange:<\/p>\n<p>RrnT = vM AXl\u2019IM = 100 v; o.001 A = 100,000 n<\/p>\n<p>Subtracting the meter resistance from the total resistance, you find that the multiplier resistance for the 0- 100-V range is 99,000 ohms. Thus far, this method is the same as the previous, but now the multiplier resistance is made up of R I plus R2 in series. Therefore, since you need 99,000 n for the multiplier resistance and R I equal s 9000 n, R2 must equal 90,000 n.<\/p>\n<p>Similarly, for the 0-1000-V range:<\/p>\n<p>RT oT = VMNJ\u2019IM = 1000 v; o.001 A = 1,000,000 n<\/p>\n<p>Thus, RMuLT = RToT \u2013\u00a0\u00a0 RM = 1,000,000 \u2013\u00a0\u00a0 1000 = 999,000 n. But RMuLT = R1\u00a0\u00a0\u00a0 + R2\u00a0\u00a0 + R3.<\/p>\n<p>Thus, RMuLT =\u00a0\u00a0 999,000 n =\u00a0\u00a0 9000 + 90,000 + R3<\/p>\n<p>And R3 =\u00a0\u00a0 999,000 \u2013\u00a0\u00a0 99,000 =\u00a0\u00a0 900,000 n<\/p>\n<p>No matter which method you use, the value of the multiplier resistance for each range remains the same. However, in the first method, the multiplier is a single resistor, while in the second method, on all but the first extended range, it is made up of resistors in series.<\/p>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-125\" src=\"https:\/\/www.apexwaves.com\/blog\/wp-content\/uploads\/2018\/07\/blogphoto2.jpg\" sizes=\"auto, (max-width: 767px) 89vw, (max-width: 1000px) 54vw, (max-width: 1071px) 543px, 580px\" srcset=\"https:\/\/www.apexwaves.com\/blog\/wp-content\/uploads\/2018\/07\/blogphoto2.jpg 1132w, https:\/\/www.apexwaves.com\/blog\/wp-content\/uploads\/2018\/07\/blogphoto2-300x199.jpg 300w, https:\/\/www.apexwaves.com\/blog\/wp-content\/uploads\/2018\/07\/blogphoto2-768x509.jpg 768w, https:\/\/www.apexwaves.com\/blog\/wp-content\/uploads\/2018\/07\/blogphoto2-1024x678.jpg 1024w\" alt=\"\" width=\"1132\" height=\"750\" \/><\/p>\n<p>&nbsp;<\/p>\n<p>References<\/p>\n<p><a href=\"https:\/\/www.allaboutcircuits.com\/textbook\/direct-current\/chpt-8\/voltmeter-design\/\">https:\/\/www.allaboutcircuits.com\/textbook\/direct-current\/chpt-8\/voltmeter-design\/<\/a><\/p>\n<p><a href=\"http:\/\/sound.whsites.net\/articles\/meters.htm\">http:\/\/sound.whsites.net\/articles\/meters.htm<\/a><\/p>\n<p><a href=\"http:\/\/www.rfcafe.com\/references\/radio-craft\/meter-shunts-multipliers-may-1931-radio-craft.htm\">http:\/\/www.rfcafe.com\/references\/radio-craft\/meter-shunts-multipliers-may-1931-radio-craft.htm<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>There are two methods of calculating the values of multiplier resistors for a multirange voltmeter. In the first method, each multiplier is calculated the same as for a single-range voltmeter. Assume that you wish to extend the range of a 1-mA movement to measure 0- 10, 0- 100, and 0- 1000 volts, and you also [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":2732,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_acf_changed":false,"footnotes":""},"categories":[7],"tags":[],"class_list":["post-2731","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-meters"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/posts\/2731","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/comments?post=2731"}],"version-history":[{"count":1,"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/posts\/2731\/revisions"}],"predecessor-version":[{"id":2733,"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/posts\/2731\/revisions\/2733"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/media\/2732"}],"wp:attachment":[{"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/media?parent=2731"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/categories?post=2731"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.apexwaves.com\/blog\/wp-json\/wp\/v2\/tags?post=2731"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}