The wires are connected in series, therefore their resistances add:
"R_0=R_A+R_C=\\frac{V_{110}}{I},\\\\\nR_C=\\frac{V_{110}}{I}-R_A."
On one hand, the current can be found from the voltage drop across the aluminum wire only because they are connected in series:
"I=\\frac{V_{65}}{R_A}=\\frac{\\pi d_A^2V_{65}}{4\\rho_Al_A}."
On the other hand, the resistance of the copper and aluminum wires are respectively
"R_C=\\frac{4\\rho_C l_C}{\\pi d_C^2},\\space R_A=\\frac{4\\rho_A l_A}{\\pi d_A^2}.\\\\" Substitute this to the second equation above, do the same for the current (third equation):
"\\frac{4\\rho_C l_C}{\\pi d_C^2}=\\frac{V_{110}}{I}-\\frac{4\\rho_A l_A}{\\pi d_A^2},\\\\\n\\space\\\\\n\\frac{\\pi d_A^2V_{65}}{4\\rho_Al_A}\\\\\n\\space\\\\\n\\frac{4\\rho_C l_C}{\\pi d_C^2}=\\frac{V_{110}}{V_{65}}\\cdot\\frac{4\\rho_Al_A}{\\pi d_A^2}-\\frac{4\\rho_A l_A}{\\pi d_A^2}=\\frac{4\\rho_Al_A}{\\pi d_A^2V_{65}}(V_{110}-V_{65}),\\\\\n\\space\\\\\nd_C=d_A\\sqrt{\\frac{\\rho_Cl_C}{\\rho_Al_A}\\cdot\\frac{V_{65}}{V_{110}-V_{65}}}=0.85\\text{ mm}."
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