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\epsilon E=\pi \left(\sigma _{1}-v\left(\sigma _{2}+\sigma _{3}\right)\right)
E qiymati 0 teng bo‘lmaydi, chunki nolga bo‘lish mumkin emas. Tenglamaning ikkala tarafini E ga ko'paytirish.
\epsilon E=\pi \left(\sigma _{1}-\left(v\sigma _{2}+v\sigma _{3}\right)\right)
v ga \sigma _{2}+\sigma _{3} ni ko'paytirish orqali distributiv xususiyatdan foydalanish.
\epsilon E=\pi \left(\sigma _{1}-v\sigma _{2}-v\sigma _{3}\right)
v\sigma _{2}+v\sigma _{3} teskarisini topish uchun har birining teskarisini toping.
\epsilon E=\pi \sigma _{1}-\pi v\sigma _{2}-\pi v\sigma _{3}
\pi ga \sigma _{1}-v\sigma _{2}-v\sigma _{3} ni ko'paytirish orqali distributiv xususiyatdan foydalanish.
\epsilon E=\pi \sigma _{1}-\pi v\sigma _{3}-\pi v\sigma _{2}
Tenglama standart shaklda.
\frac{\epsilon E}{\epsilon }=\frac{\pi \left(\sigma _{1}-v\sigma _{3}-v\sigma _{2}\right)}{\epsilon }
Ikki tarafini \epsilon ga bo‘ling.
E=\frac{\pi \left(\sigma _{1}-v\sigma _{3}-v\sigma _{2}\right)}{\epsilon }
\epsilon ga bo'lish \epsilon ga ko'paytirishni bekor qiladi.
E=\frac{\pi \left(\sigma _{1}-v\sigma _{3}-v\sigma _{2}\right)}{\epsilon }\text{, }E\neq 0
E qiymati 0 teng bo‘lmaydi.
\epsilon E=\pi \left(\sigma _{1}-v\left(\sigma _{2}+\sigma _{3}\right)\right)
Tenglamaning ikkala tarafini E ga ko'paytirish.
\epsilon E=\pi \left(\sigma _{1}-\left(v\sigma _{2}+v\sigma _{3}\right)\right)
v ga \sigma _{2}+\sigma _{3} ni ko'paytirish orqali distributiv xususiyatdan foydalanish.
\epsilon E=\pi \left(\sigma _{1}-v\sigma _{2}-v\sigma _{3}\right)
v\sigma _{2}+v\sigma _{3} teskarisini topish uchun har birining teskarisini toping.
\epsilon E=\pi \sigma _{1}-\pi v\sigma _{2}-\pi v\sigma _{3}
\pi ga \sigma _{1}-v\sigma _{2}-v\sigma _{3} ni ko'paytirish orqali distributiv xususiyatdan foydalanish.
\pi \sigma _{1}-\pi v\sigma _{2}-\pi v\sigma _{3}=\epsilon E
Tomonlarni almashtirib, barcha oʻzgaruvchi shartlar chap tomonga oʻtkazing.
-\pi v\sigma _{2}-\pi v\sigma _{3}=\epsilon E-\pi \sigma _{1}
Ikkala tarafdan \pi \sigma _{1} ni ayirish.
-\pi v\sigma _{2}-\pi v\sigma _{3}=E\epsilon -\pi \sigma _{1}
Shartlarni qayta saralash.
\left(-\pi \sigma _{2}-\pi \sigma _{3}\right)v=E\epsilon -\pi \sigma _{1}
v'ga ega bo'lgan barcha shartlarni birlashtirish.
\frac{\left(-\pi \sigma _{2}-\pi \sigma _{3}\right)v}{-\pi \sigma _{2}-\pi \sigma _{3}}=\frac{E\epsilon -\pi \sigma _{1}}{-\pi \sigma _{2}-\pi \sigma _{3}}
Ikki tarafini -\pi \sigma _{2}-\pi \sigma _{3} ga bo‘ling.
v=\frac{E\epsilon -\pi \sigma _{1}}{-\pi \sigma _{2}-\pi \sigma _{3}}
-\pi \sigma _{2}-\pi \sigma _{3} ga bo'lish -\pi \sigma _{2}-\pi \sigma _{3} ga ko'paytirishni bekor qiladi.
v=\frac{E\epsilon -\pi \sigma _{1}}{-\pi \left(\sigma _{2}+\sigma _{3}\right)}
\epsilon E-\pi \sigma _{1} ni -\pi \sigma _{2}-\pi \sigma _{3} ga bo'lish.