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Solution for the question - if the ratio of lengths, radii and youngs modulus of steel and brasswires shown in the figure are a,b and 0 , respectively. the rati

If the ratio of lengths, radii and youngs modulus of steel a-Turito

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Solution for the question - salicin (structure given below) is a glycoside, found in the bark of willowtree, used in relieving pain. observe the following react

Salicin (structure given below) is a glycoside, found in the ba-Turito

Young’s modulus is defined only in elastic region and <img src="data:image/png;base64,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" class="Wirisformula" alt="Y equals fraction numerator S t r e s s over denominator S t r a i n end fraction equals fraction numerator 8 cross times 10 to the power of 7 end exponent over denominator 4 cross times 10 to the power of negative 4 end exponent end fraction equals 2 cross times 10 to the power of 11 end exponent N divided by m to the power of 2 end exponent" width="303" height="42" style="vertical-align:-15px" role="math" data-mathml='«math xmlns=¨http://www.w3.org/1998/Math/MathML¨ »«mi»Y«/mi»«mo»=«/mo»«mfrac»«mrow»«mi»S«/mi»«mi»t«/mi»«mi»r«/mi»«mi»e«/mi»«mi»s«/mi»«mi»s«/mi»«/mrow»«mrow»«mi»S«/mi»«mi»t«/mi»«mi»r«/mi»«mi»a«/mi»«mi»i«/mi»«mi»n«/mi»«/mrow»«/mfrac»«mo»=«/mo»«mfrac»«mrow»«mn»8«/mn»«mo»×«/mo»«msup»«mrow»«mn»10«/mn»«/mrow»«mrow»«mn»7«/mn»«/mrow»«/msup»«/mrow»«mrow»«mn»4«/mn»«mo»×«/mo»«msup»«mrow»«mn»10«/mn»«/mrow»«mrow»«mo»-«/mo»«mn»4«/mn»«/mrow»«/msup»«/mrow»«/mfrac»«mo»=«/mo»«mn»2«/mn»«mo»×«/mo»«msup»«mrow»«mn»10«/mn»«/mrow»«mrow»«mn»11«/mn»«/mrow»«/msup»«mi»N«/mi»«mo»/«/mo»«msup»«mrow»«mi»m«/mi»«/mrow»«mrow»«mn»2«/mn»«/mrow»«/msup»«/math»'/>

Solution for the question - which one of the following is the youngs modules (in {:n//m^(2)) for thewire having the stress-strain curve shown in the figure 2.0 xx10^(11)

Which one of the following is the youngs modules (in {:n//m^-Turito

Elasticity of wire decreases at high temperature <img src="data:image/png;base64,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" class="Wirisformula" alt="i. e." width="26" height="13" style="vertical-align:-1px" role="math" data-mathml='«math xmlns=¨http://www.w3.org/1998/Math/MathML¨ »«mi»i«/mi»«mo».«/mo»«mi»e«/mi»«mo».«/mo»«/math»'/> at higher temperature slope of graph will be less So we can say that <img src="data:image/png;base64,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" class="Wirisformula" alt="T subscript 1 end subscript greater than T subscript 2 end subscript" width="54" height="17" style="vertical-align:-5px" role="math" data-mathml='«math xmlns=¨http://www.w3.org/1998/Math/MathML¨ »«msub»«mrow»«mi»T«/mi»«/mrow»«mrow»«mn»1«/mn»«/mrow»«/msub»«mo»§gt;«/mo»«msub»«mrow»«mi»T«/mi»«/mrow»«mrow»«mn»2«/mn»«/mrow»«/msub»«/math»'/>

The diagram shows the change <img src="data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAAAsAAAAKCAYAAABi8KSDAAAACXBIWXMAAA7EAAAOxAGVKw4bAAAABGJhU0UAAAAJufgqOgAAAHFJREFUeNpjYECAZCDuYMAEzVA5DHAOiMWR+IlAPIUBB/AA4j4o2wWI9zIQALuB2B6ILwCxMCHFBUD8C4j1CCm0BuI1UKdE4lOoBMSbgJgLiHmA+AwuZ4gC8TY0SR8gXoyukA2I1wGxNBZDlkNDiHQAAJxHEBolHuC4AAAASXRFWHRNYXRoTUwAPG1hdGggeG1sbnM9Imh0dHA6Ly93d3cudzMub3JnLzE5OTgvTWF0aC9NYXRoTUwiPjxtaT54PC9taT48L21hdGg+wQ7kJQAAAABJRU5ErkJggg==" class="Wirisformula" alt="x" width="11" height="10" style="vertical-align:-1px" role="math" data-mathml='«math xmlns=¨http://www.w3.org/1998/Math/MathML¨ »«mi»x«/mi»«/math»'/> in the length of a thin uniform wire caused by the application of stress <img src="data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAAAsAAAANCAYAAAB/9ZQ7AAAACXBIWXMAAA7EAAAOxAGVKw4bAAAABGJhU0UAAAAMyZLetQAAAFlJREFUeNpjYMAEP4D4Pxr+BcRM6ApVgPgCA5EgAIiXEqu4HojLiVW8Cmo6UeAWFs9JY1MI8u0XYk01B+K9xCqOBOL5xCqeBMTJxCpeB8RexCp+B8QcDNQCAG0iFICd+m2LAAAASXRFWHRNYXRoTUwAPG1hdGggeG1sbnM9Imh0dHA6Ly93d3cudzMub3JnLzE5OTgvTWF0aC9NYXRoTUwiPjxtaT5GPC9taT48L21hdGg+PJEFugAAAABJRU5ErkJggg==" class="Wirisformula" alt="F" width="11" height="13" style="vertical-align:-1px" role="math" data-mathml='«math xmlns=¨http://www.w3.org/1998/Math/MathML¨ »«mi»F«/mi»«/math»'/> at two different temperatures <img src="data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAABMAAAARCAYAAAA/mJfHAAAACXBIWXMAAA7EAAAOxAGVKw4bAAAABGJhU0UAAAAMyZLetQAAAHVJREFUeNpjYIAAJiD+BcT/8eBfUHUkAzUgvsBAJRAExEupZVgjEJdQy7A1QOxHLcPuArEkNQxiAeIv1HKVJRDvp5ZhkUA8n4ikU0tM8pkExMkE1CwG4jRoYsYL1gGxF5G+IGjYOyDmoJZhpIBRw0gzBB0zAAC8NSH/ozxNHgAAAGB0RVh0TWF0aE1MADxtYXRoIHhtbG5zPSJodHRwOi8vd3d3LnczLm9yZy8xOTk4L01hdGgvTWF0aE1MIj48bXN1Yj48bWk+VDwvbWk+PG1uPjE8L21uPjwvbXN1Yj48L21hdGg+tf7ZZAAAAABJRU5ErkJggg==" class="Wirisformula" alt="T subscript 1 end subscript" width="19" height="17" style="vertical-align:-5px" role="math" data-mathml='«math xmlns=¨http://www.w3.org/1998/Math/MathML¨ »«msub»«mrow»«mi»T«/mi»«/mrow»«mrow»«mn»1«/mn»«/mrow»«/msub»«/math»'/>and <img src="data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAABMAAAARCAYAAAA/mJfHAAAACXBIWXMAAA7EAAAOxAGVKw4bAAAABGJhU0UAAAAMyZLetQAAAJhJREFUeNpjYIAAJiD+BcT/8eBfUHUkAzUgvsBAJRAExEupZVgjEJdQy7A1QOxHLcPuArEkNQxiAeIv1HKVJRDvp5ZhkUA8H488cro7CsQq+AybBMTJRFgKSsBZQHwOn6J1QOxFgk9+4JN8B8QcRBpkD8QHqRG2ktAwU6LUIFDe3UKNtAgyYBsQ81HDeyCDNKiVDrGVdWAAAO0hI0uYXuHxAAAAYHRFWHRNYXRoTUwAPG1hdGggeG1sbnM9Imh0dHA6Ly93d3cudzMub3JnLzE5OTgvTWF0aC9NYXRoTUwiPjxtc3ViPjxtaT5UPC9taT48bW4+MjwvbW4+PC9tc3ViPjwvbWF0aD4aV5SuAAAAAElFTkSuQmCC" class="Wirisformula" alt="T subscript 2 end subscript" width="19" height="17" style="vertical-align:-5px" role="math" data-mathml='«math xmlns=¨http://www.w3.org/1998/Math/MathML¨ »«msub»«mrow»«mi»T«/mi»«/mrow»«mrow»«mn»2«/mn»«/mrow»«/msub»«/math»'/>. The variation shown suggest that <img src="data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAAVwAAAEVCAMAAACbn626AAAAAXNSR0IArs4c6QAAAARnQU1BAACxjwv8YQUAAAMAUExURf///+bv5mNjY97m5vfv787OzrWtta2trb29vWNrY97e1pycnEJCQnt7ezEpMXNzazo6MRAZGQgQCEIZWkIZEMVjWpxjWr0QWiEZGaVjlFII3lKMYwje5gic5lrOpVqMpRlK3hnOYxkI3hmMY1JaWkpSSoSEe4RjnHNjEO9rte8QtYScWr2czhAZQoyczu9aOu8ZOu+cOu9aEO8ZEO+cEO9aY+8ZY++cYyEpIQgACFrv5r0xWlqt5r2cc1rO5lqM5r2cUr1a773vY73eMb0xlL0Z772cMRBrGZSMlISMjL2UnO9r5u8Q5u/eOnNjQu+cte9Cte/eEO/eY72c7xAZY4yc7wAAAO9ahO8ZhO+chIwQGWsQGe+c5u9C5kJjKUJjCMXv5u/ehMVjKZxjKVJrjFLvEFIpjFKtEIwQWilKWr0QKRlrjBnvEBkpjBmtEJTOtaXO5oxrzozOc4zvEIwQpYwpzoytEO/mtcVjCJxjCFJKjFLOEFIIjFKMEGsQWghKWr0QCBlKjBnOEBkIjBmMEJTOlITO5oxKzozOUozOEIwQhIwIzoyMEIwxGSnvpSmtpQjvpQitpWsxGSnOpSmMpQjOpQiMpe/FrcXmtb1rzr3Oc73vEL0Qpb0pzr2tEBBKKe/F78XmlL1Kzr3OUr3OEL0QhL0Izr2MEBBKCFJr71Lvc8VjpVJrrVLvMVIprVKtMYwxWlIp71Ktcynv5imt5ilrWr0xKRlrrRnvMRkprRmtMZTvtaXv5lrvtVqttRlr7xnvcxkp7xmtc4xr74zvc4zvMYwxpYwp74ytMVJK71LOc1JrzlLvUsVjhFJKrVLOMVIIrVKMMWsxWlIpzlKtUinO5imM5ghrWr0xCBlKrRnOMRkIrRmMMZTvlITv5lrvlFqtlBlrzhnvUhkpzhmtUoxK74zvUozOMYwxhIwI74yMMVJKzlLOUkJCEO/FzoSlnISle8XFnEIQOsXF7+//Ou//vXNSY0pCY4Rae8WtnPfm7+bv92NSY62tlOb//wAAAE6wEvcAAAEAdFJOU////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////wBT9wclAAAACXBIWXMAABcRAAAXEQHKJvM/AAAWzElEQVR4Xu1dWXajPBNNgxhaEiDliQWIrEHswGyAFXz7z8P/wDmG9vmrBM7gKcZmCKDbiQMEp+NKuXRrUNWLhYWFhYWFhYWFhYWFhYWFhYWFhYWFhYWFhYWFhcU2UVNKukOLB0FeDhdlSLzAp92xRW/UNAwCFuBneK6klEWJb1X3UdAgcjrsPLe7eATxE56907o7tegHEkacKyeKIidi4amO0oLL2Dm7bHEfKFMxL4Iw9P0wdE+lGCpZasVOFdriLtQgXNEEQAlc+Hci2wMJeFnmIrKq+xi8ouJvXie8Q/vlCBI6uizLtGKWMDwC4r1lWXFFdmBxQbYgXau6D4EGDlfsiujCysi2lCqwVvcBGJPrn5iDDrQQpY61TAV/s6r7AOCdL5LLktsHjtYqqUSjVMMs1+0PGgmR+NQl8PFdxGCNK54wljgFi5S1ug/Ac+LYYSHQ3PDEPaOBygrfCxwn8FhUhJYw9EUdgnBVVLCiKPxvkYUaJArqCmzMCQgNWHCkaxb3ggaVBLsaRYmTfCezJGQMtJWA5oKIvcAKtzfojmse7RgD1Q2/mQXqhShOo7logM2ZRQ8QD9Yzx6MGX2VLiAsrHBy4aHPxAnUv8zWLa6hDEG6x786+4kBeDPdCs4DCbc8seoAEKubsktyONuCouRZ9cSA7HqubsutsrkV/0ETq6NZKddgzK9wHQVUOwu1OLuLD5lr0RVi9xrubrpe1uQ/Di7ImuBmSAZt72yiPhS+/1IEQZN2hh4BH+FhCLQX1/PCmbA90Js0ldP/Ju2m4S5RBxpWqMgdc9TWw7plsLvUC5n3YKxoWigsu0rKU8EVwh62iDGg/i3AJSFOxDxoDzjdjO1bEZZ5F4Kqzdfjih1ls7oEynuqzcgnaSLFbUeUaIcBz/e5kMhDf0bmIvJPVwFO6CrvjVQBs7uSaSzzGpayCE46I6uysSrjIc6fWXMqUTkVx6tx4RZwmq8qHkDCZWHPBzEdCxk5wEqwjXpLKaE3CBZ7bTMwWCN1VUmaMnJb/BArUeT3LGWB6nkvCv0KmyZlxdVkleVe+UpO9S08r25aHyWMLxHvPUpmdRzwomNzOQhHwKqKCnVUTLw2T81zqJ3EaR+FZegTDo0lo2JkbFg3ny6+lwNjClGyh9goudRPQU5Nbe9WraCsGSciwVptXbwuPMEzNc0nYpDln5zFm4nMwuShcoBPoAIeO5stmvTUuaBNqLvEKIc8dXwBhIlWtMInneeSFFJpP7jsOi4ltLlihOOXFhbgMBeFW3fWDIQo7kS18n9G0HhrufpE88U8NLmprpOVX/+xAC954i7a5B8Nzp9KPA2VZqtWFTQIYnZNp9OUXAVah3m6m/349CPhFE/LcLhp2oUqFMJ7H790JAtjY4qkYaMx0wqUgQVldqrM+EFbpo3+GoCyJFr+zc0oPjfhK5uJja9E34PaC6MP4E88visWXY6PNnYwteJHIJVj4SxlT4hfRB/slWDsMfkZ3ulSAzZ2MLVBWla+tn3AO4oUf276J9664swt871tl5vJA/Ik094DlrKV2rhhSoLYfGk2ChAvuOMlJMfziMBnPJbgxS1b/ftbFeh9EqsFd9if12ouD4bnd8agAzpeXojhNSl4AgeUsYAw+QHF/vv33gkzFFtADK8vmrkgMcUlXC7/wJW2q2IKLiqvvcrnA5a3xX12fbgRfGiayufA31LCaLZ669sM0PPfg7Xie82Dp7/N+MFWO42suDVVailXlze/BNDYXaBiW2Cx56X8EU3hohLJGp+J2ifsaYajYuJbQlNjkeoP74ieoLMe6Oy2zDfbRmcDmguLG22xeNrbNJVgbxiXmds4TZ2sH2NxRNfdA3NCJJT+rdN4CRue5BEts0muRxnVjdJtLwfG9UOm8BZjU+oiaS15AcXW80S6yJp473isnNFCp5rtVbH3qi5HjuQfqw2oWb7Wv1sg5NMpgNeNsFZtN+2NcmwvLZSw320F21LoFs5pJeak2bBsYlecSplJQ3K3KdlyeSyNd6sZf+r6RhzFmDo34Ks+BhnWn2wOwhZF4LpbYxJiUvNTWbBMAnjtafS6sZlhiQ5eeIH8cRnO742EB1lyW5/v+N4S2bL87GRTEK+Iy3WKI/BPE/zsOW3DBNyvFZimuwVhsAYxCWsqb3fjWjz/jeGjYxaYsxW7Tsh0ptoCbhHQONKw73yJwAh2whX/d6WAgWEWeS7X1MXajxBaIt8PVbHslNicYIxMBvtlfoGHdNukNYxSeiyHybn//puEO76G1FjfebqTxA8Pn0Ijr7TKZqtGixMuByUQMGlnBemrM7Ww30njECHULbTOQ5rSZ4NaAJAHc1GHNQk3/NVpiM5BF7yEbBDRQg2ou2WMzkDgJt1fTeIbBQ44HypRMswvtlzaIoYXbdsFMth0N64Dz0IaMihGPqTStPjtmbxrD7okg1MeC0be2a+DWMbTNRRoWq63TsCPQiRiOLWAPXKRh3enWMajm1rQQuT7r6TwVCA2DIPCD0A99OAg+G7vMA9PLcTDhUlbJnO/mGiEMBr8S/AghqmjmaP2gu3k8J51z3z+8FhELkcpSahHHgkczTzkfUHMJZaIseTCbb0a8MGDsvRGpaHBOSjCzWcAeigMJ17RjLH8YvzYBgFzyz51ZczrhZsLJMMLFXailbsI/3flcAP9b/ZJ4J1KxYYSLuZ2Szz8OKox4VfyO3rCDVdyAUdBYGza3b0Z8sAq/JO+MNneQugWP8bwEGtadzgbQFu78DhfR7EMbQnOpr0zB6NxGAUOe/LdsHzJUbIBfxStE+VrNH7DBfdxfhEu+tIicHGar1POai7tQQXHbMQ+zgngRxxxTu6ARnME5nxYP4kQcMCmZX+0wOiWAEGbZsZu/67GiuD09dlSgzX1auMTbVWmaBXNTXAwdBQlvWPuL7IPIcZz3+TjvIDyXho74JZUKlDlcdWE5FxwkJ4lmK1kbhC2gUShT9Rt6KsB7SGVJF94gISuiZMa/+RA5NPDmNbbG/RXCjbIqCbuFtaY4Qmk+XjaA5pIQu9j8CsVFK8fV555N7Cy/m22z1hA5NKDtZt7ObO58TT4mt7uBEp+VVMBiAtDc7mxyYLf9J3kuFozimLiZFJcQj9J995/XdMfFF0a4B7NQzFeD/fwOSsztyLmCCjWhPo4PPzbmdXcV/3s0uaC6YBZmHObxLM/FnmxY6TyLehAcVqk4d4LOygJZyNTXlZWize2Op8ezPBe7YL7O0wzkQCiYVC5znX1U+FCwsR8hZWIWtPnYwtM8l/h/YzkPDSOeH6lYlhKsbNehiLgmmNAtraDXLFJOMNtAhCfjuRjh07qZPoUNFsEDZ0zLVFRR8Pm3xTBYd4gcMWrATIC451He5zQXa8NEmk1u1mAdQ6WMpYxV9C90L2umGySNUg3KfhaaaEKOj8dzTcGomDrwD6IFY4ui1Txi3tUW/iQo3qLorfDn8h2f20FJ38E3q6ZOSqJroAQa22Z3yyDhGJoQcF38I+OZ2MKBhElciqlL9Dtjm6cZvOFvvWdwUpXBXNUL6P4+qrmYUslTxSatu0OOUGkwtjxhN0WLAKHOJFcDWNAe1lwSNDivc0IeidaWwRIKHKHZzVysdAeesLkEB0VJNWWxG3AEh0vkCIU/X/bmbjxhc01SMk0mpGE0SMAilClahN+utYjHbS78WbDEZrIwLlDbndJlmYuGfYZmfjVM4OYh+eDYw5xfnoU6PGpYyByelsC/In8hw6nqhydWE1+VpZ6oUgGcXb/IQG2B2rL5Qoh98XA8F5OSoLhT6K1xdh30GuKs+BJH+PVAm/uAcAnuQsVoWHc+IjBoy5IszjGOsKzdgw/yXBcHRaUT5HZq4mLQFuMIAjjCMZ+zDDwWFUPfDKfHjf5ScUxt4YjX3BjbZXCET4DNfUBzSZjoPE5Gz+2YwoMKLILkX4O2SwEJ/vbWXLCCu+pVZmOHyNHXjRQ4u4I7uyUOrzY8tzu+EwcCPrOQY7dfAmaLkUUtNXeKcHlqC/jzAFsAzoldbMY1CsARikbIPBVqt0TR4m/8iM3FvFmajVupUHuBCdqC2jLv14e/LgMrbvppLsHVbOSxJaYeoWpFi5HFOWOyz6C/zQX/oZLpmJUKyBEckZalaBZqbDv0ji0c9n6EIfLRagfBa8CgbZmnHJPi3dVFon8vR4olNtV4iksxjVOC2i4kaHsD/W2u72gs0R/ndYNH1oZoZFZ4+6Xa2g6kJ1sw+3ZwXucoilsDg8bs43JyDbfRN7aAuZ18lNa4NXKE90a8ArUF+rWCoTOmsrxHrRjxIqBh40zzMZFFXb5i9nEFagvol0ODty3XSMOGfu0mZ44VSqleZIjmIto9EXe/FnIcezj0UmOM7Uc9Qndx8aC99kRgv2wcm96dDgQ0tjvgCLnkKgrnKwQfHL2oGAnbff/d6TBoaxaxQglrFtejtoA+wiXUDIoaloahaAsldBrzZAEVSn2AE07u5rkuy4buyXYg1N85PJZaOIU/W339SMBasTuFC0YhLfWg0TCy91iC2ce4eptv68JouN8sYKPG8nXYoELrkIGx/bvzFlBY1xf3C9f4ZkPu2/mII8RYIL4mY3uEe6/NRd+slE042Nh0F7wGrl9znb2txWs4xb3BcmKmx8WD1YZh9pEDs02Bfs21k2l03GsW6jDBSueBkpI1Dd+duCxLrWbcmjs27m0JgIqL06eHUVz4aUlbDpoAaV7fQoZAlbmzshxMs8YOo0NomUmaxymIVu3WPc76vgknJIw4jj3sTp8AFtYdt5UW4X6xid17cJ9ZOBgaFj9fMEpeujhCrrEctLu6WtwlXBJiic3zBaNYDrrD4i9wdpn3Z7Ur2RH32FxsJpimT+d26jaOoLEcNNrCKIl7+i0QrHSW8dORRuqxJBMyjXFb6X6dHOE7wCz8pLltM8EnQ+SotoWKUxlzZ5VxhAswC9ptzcWxh0Ly52gY0C8sozF1desK2l4DvkaCFTc3X6ypVIif6akAWhuypBK51EC/VhpHuIQf47m4msW4mj38TsboV5TF8jU1FUqzbdCfHGgWbtvctifbE2NLajS2mH3EmsVNWIQP/GhzKVOpzB7P7WDSnKdgEbAcdFk7nZ7GDzz3gIr7+KCog0maxyBangSgtVsxCB3Q5t7QXEJ3PMex6Y+JBdvZClmWwgFmuy2tBfxUcQOKLcvHHN8D2VM/4iBas9G8u7op3N7NA4oLBKp5qO4OvQYsB80FUNvNaa3BTZuLVQ36oe3TprDOEa9lHqvo2Axwa/ghtmBoWOP3jLoSYmoWOVDbFdUsPoAbPJe8/GGwmvUe4nsgbnhsWJds1SIY3NJcMBna9GTrzu8DqK2PHCFP4815DScAAV6tLPdwNesZDTNxBHB2gdoqsAjd1W3CTPK7ornEzNvpt+HMxBGU0FpnYBHmn3gyL0xRyMW37oEWuuxJw1zPZw5Ppa6SlVYo9YJxIrrj76ABz3sOigJmi13V1lv81Q848vQiWyAvOK8z7RFUMBaB6xTTOP88suqk+Z24Fs/FoEIpObtbSMARoirFZjS4h38TaZwfcc0suL4yJTbd6U+oqfeODhlyhNCKtsO1KkfsyXb/akZwDJksy3TTDtkZLttcQoImxUFR99gEjCPsVJyXxiJY0X6gvmwWiB+h4t5RMFqD1prEblnGODSgu2yBuGgWDpRl2EzwDlGhs+twXcJClmyhiqYXLsZzMaggY+cOxQXRvjdYxRyvvRz0EVyyudgF05TY/GQ/sRw04sKEvzBFZvEdF3guxnjNvJ3u/BpgHcNcQypFlbBw6W09RsCl+lwce5jq5iffzPWCAndD354ysmmA5jYnwjWtcfkP83aIhw3rNHoNN6eMbBrnNtdUKsS3C8jIHnMNOGXEqu0N7MEsfIvn4mom04xd8x/AtcUC8UKJVJs+i1ZtrwIWr2+aeyAhdrGJwqsb74hrWk+kqa4ccHatbK/jrOIGo2FaXSdWnUMGPgYY2w2W0fTBqc0Fiwv+w9XcDjpkb1Uspen89WdrxV89gVTsi+ZiGFemn2OJT4FbRoQsU2G6g3YXLa7gJIfmBkrj9Onu9BQ0+Iu7oYHagkWwUdsfcDrhBIxCLq5UOoNFKBQyW6RfNotzB8DmfhHun6C61kywJh6WQZdAgTeyZeR5fAs54oSC8mKJPsH+CBXu4eeRZbZ3AYT4LbZgCkYvVDq3HEG8liWqrY0s3gmMgH1sRjclNudJyZq42Ob6tXzVOEDP0q+7YfahdYdmUNRp+yUCFgH3PsrXlTS1nRBfzILLgGaJk2YgWGlbYH8EUw5qLUIvfMYWwDdLS/3329hDbFgHoo1T3U4rtRahDw6YQzM2l7hMlKViX2Vrau+xYR0Oi7ccoTeOvRyxaMysZl+ESyhGFkG0ZhRGd9HifnzEFrxIlKn61E+gX+GuAWMb40Zzu5A9gmNqHZuBSP45KKrGxG6GfX6aIvCstX0EpIstmOlxn0YBjG3bwjJFY2uDto8Bd5qhcCmrXr9QXDdEY4vzi3HLiNXaB4E2N3x5CRMBq1krWwzRJKY7KAe1tVr7MMzILh/9h1SqLq5Lw7dK55jY/WcTu08Bo2LhH6wNE6ZSAdS2bXxvy0Gfh7G5HuO5bjDSWGPrCd12B7UF4k/igNNTd1gbhh1GkdriIP62O+gWcKI/A79VwTHLooi/iih0gdo2QudlXO02U45AWuBhTWCFGfLdStxACaV0WjEPqC0mdnUW/VuNaGtQxpvqSOj/Qo9iqw3ihf7AOkWCRscCG1f+M/sazEjNFUUWCajjrREJ6IgWht97zFG7YffYkyCTMgbhRhi0lSZEs56FjNSEUg97mV0DCaOMFyGs5IzHvBg2q01CnpcyFZyLVOKWkZXxL5f6QXDjReFIftEw05pOOMP6TAeCTfRBujptSz3WJVosyAxZUWAxwJX3o+s7PGNY/4btKof19CmGyMsyx/DXKusRQHULx4muR03BHnAnagQHvtRdGggER2uA5mqOid31iRYBfpHiCltEXdRecKM453qEEdzYjLw0U7dX7DUYrzPGBOtF9aEF5l+/J7gGAWZ8y9wM4nf3LtAWl1Di7imhe/hHKBwO8AE/6vTS7Y8eT7h9K7wW8I3CAl6lRPF67rn2YkUyDh3qTocD8RvTsk45URQV8AlIvny2DxF+9/j47eT8sXvG1+e1uOvWa0947Nb2CGD2IYLxqy70j6u9Ar471HyRrzjQfxwWM/AjhIgFbz+BlsEnj+EhjuEKnJpH8wUfzGN7Oz6214/fhafhcftoboWf/v2m9vHSrZ9PaP/rp26FEzzCX13mKF2sKz7NYmN9oQbNHXj4YwvKzB/YAURO0v77r/2COF7C7wLaK92d+AjH/8Hl43PbB7gVvphvH++BR7jp1q3dz8OD7vjkVvgCj/CT4OuFW9tf2pzAz8Pbjufw6nBYDUA4xXdKcADZOgr+PHqICSPnQLOExgkA9smt4Ut79gFzBg8fV48H5hr9g08zz70EuA73mJ+4/+FWA/zm5w0f/+UR7e/WXv52Ky4Qn/dTimcIXElQOUF1JbhiJ/lA1FvuFIUT9+vmY2EAbgFuCY2lyLBmu7t6BA0ckRWeB+u6CjbZKfVJgGwroXE4xSlTIHs/qjIkuKFKx7G6K4cbFk2mLjWVxEysk5lRu8h1T3aSWvwM7IeagNZeKL4g1CvAMUaFJUHD72mMYvEVhPqMsStBcHAvgrbhUU3DwiZkewLe+WHoXQma1FgQd7TDQENs9Us/YOeolcajfgPqQXOOFhYWFhYWFhYWM+Dl5f/ihvXyF3OF/QAAAABJRU5ErkJggg==" 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Solution for the question - the diagram shows the change x in the length of a thin uniform wire causedby the application of stress f at two different temperatur

The diagram shows the change x in the length of a thin uniform -Turito

IfΔHf ofICl(g),Cl(g),andI(g)is17.57,121.34and 106.96Jmol–1respectively.Thenbonddissociation energyofIClbondis-

Solution for the question - ifhf oficl(g),cl(g),andi(g)is17.57,121.34and106.96jmol1respectively.thenbonddissociation energyoficlbondis- 420.9jmol1

Ifhf oficl(g),cl(g),andi(g)is17.57,121.34and 106.96jmol1re-Turito

Calculateenthalpychangeofthefollowingreaction H2C=CH2(g)+H2(g)→H3C–CH3(g) ThebondenergiesofC–H,C–C,C=C,H–Hare414, 347,615and435KJmol–1respectively-

Solution for the question - calculateenthalpychangeofthefollowingreactionh2c=ch2(g)+h2(g)h3cch3(g)thebondenergiesofch,cc,c=c,hhare414,347,615and435kjmol1respect

Calculateenthalpychangeofthefollowingreaction h2c=ch2(g)+h2(g)-Turito

HeatevolvedinthereactionH2+Cl2 →2HClis 182KJ.BondenergiesofH–H and Cl–Clare430 and242KJ/mol respectively.The HCl bond energy is-

Solution for the question - heatevolvedinthereactionh2+cl2 2hclis 182kj.bondenergiesofhhandclclare430 and242kj/molrespectively.thehclbond energy is- 154kjmol1

Heatevolvedinthereactionh2+cl2 2hclis 182kj.bondenergiesofh-Turito

Among the following for which reaction heat of reaction represents bond energy of HCl

Solution for the question - among thefollowingforwhichreactionheatofreactionrepresentsbond energyof hcl hcl(g)h(g)+cl(g)

Among thefollowingforwhichreactionheatof reaction-Turito

The range of a galvanometer of resistance G ohm is V  wolt. The resistance required to be connected in series with it in order to convert it into voltmeter of range  <img src="data:image/png;base64,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" class="Wirisformula" alt="n V" width="21" height="13" style="vertical-align:-1px" role="math" data-mathml='«math xmlns=¨http://www.w3.org/1998/Math/MathML¨»«mi»n«/mi»«mi»V«/mi»«/math»'/> volt will be........

Solution for the question - the range of a galvanometer of resistance g ohm is v wolt. the resistancerequired to be connected in series with it in order to conv

The range of a galvanometer of resistance g ohm is v wolt. th-Turito

A galvanometer with resistance 100Ω  is converted into an ammeter with a resistance of 0.1. The galvanometer shows full scale deflection with current of 100μA. Then what will be the minimum current in the circuit for fall scale deflection of galvanometer?

Solution for the question - a galvanometer with resistance 100 is converted into an ammeter with aresistance of 0.1. the galvanometer shows full scale deflectio

A galvanometer with resistance 100 is converted into an amm-Turito

A galvanometer of resistance 200Ω  gives full scale deflection for a current of  <img src="data:image/png;base64,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" class="Wirisformula" alt="10 to the power of negative 3 end exponent" width="39" height="17" style="vertical-align:-1px" role="math" data-mathml='«math xmlns=¨http://www.w3.org/1998/Math/MathML¨»«msup»«mn»10«/mn»«mrow»«mo»-«/mo»«mn»3«/mn»«/mrow»«/msup»«/math»'/>A. To convert it into an anmeter capable of measuring upto  1A. What resistance should be connected in parallel with it ?

Solution for the question - a galvanometer of resistance 200 gives full scale deflection for acurrent of 10^(-3) a. to convert it into an anmeter capable of mea

A galvanometer of resistance 200 gives full scale deflectio-Turito

A moving coil galvanometer has 150 equal divisions, Hs current sensitivity is 10 divisions per milliampere and voltage sensitivity is 2 divisions per millivolt. In order that each divisions reads 1 V . What will be the resistance in ohms needed to be connected in series with the coil?

Solution for the question - a moving coil galvanometer has 150 equal divisions, hs current sensitivityis 10 divisions per milliampere and voltage sensitivity is

A moving coil galvanometer has 150 equal divisions, hs current -Turito

A battery of 2 V and internal resistance 1 is used to send a current through a potentiometer wire of length 200 cm and resistance  What is the potential gradieut of the wire?

Solution for the question - a battery of 2 v and internal resistance 1 is used to send a currentthrough a potentiometer wire of length 200 cm and resistance wha

A battery of 2 v and internal resistance 1 is used to send a cu-Turito

A potentiometer wire, which is 4 cm  long is connected to the terminals of a battery of steady voltage A leclanche cell gives a nullpoint at 1 m if the length of the potentiometer wire be increased by 1 m, What is the new new position of the null point?

Solution for the question - a potentiometer wire, which is 4 cm long is connected to the terminals ofa battery of steady voltage a leclanche cell gives a nullpo

A potentiometer wire, which is 4 cm long is connected to the -Turito

In experiment of the potentiometer wire  AB of length 100 cm has a resistance of 10Ω, It is connected in series with a resistance R and a cell of emf 2 volts and of negligible internal resistance.A Source of emf 10mV is balanced against a length of  of 40 cm the poteatio meter wire. What is the value of the external resistance? <img src="data:image/png;base64,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" 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Solution for the question - in experiment of the potentiometer wire ab of length 100 cm has aresistance of 10, it is connected in series with a resistance r and

In experiment of the potentiometer wire ab of length 100 cm h-Turito

If the deflection of the galvanometer is  the same direction at both the ends of the potential meter wire, then point out the statement which is definitely not the possible reason for the.

Solution for the question - if the deflection of the galvanometer is the same direction at both theends of the potential meter wire, then point out the statemen