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Journal : BERKALA FISIKA

RANCANG BANGUN PERANGKAT LUNAK UNTUK PERHITUNGAN SEL DARAH MERAH NORMAL DAN TERINFEKSI MALARIA Setyowati, Setyowati; Adi, Kusworo; Anam, Choirul
BERKALA FISIKA Vol 22, No 3 (2019): Berkala Fisika Vol. 22 No. 3 Tahun 2019
Publisher : BERKALA FISIKA

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Abstract

Malaria is a serious global health problem. Calculation of normal and malaria-infected red blood cells is manually calculated on image of the blood taken by the light microscope. The calculation of the normal and the malaria-infected red blood cells is to know the percentage of parasites and their growth. In addition, it was used to determine the percentage of inhibition parasite growth. The aim of this study is to automatically calculate a total, normal and malariainfected red blood cells. The steps for the calculation of the total of red blood cells: normalization, thresholding, separation and calculation of the red blood cells by labeling. The steps of calculation of malaria-infected red blood cells: converting RGB image to grayscale and to binary image, sweeping, and the calculation of malaria-infected red blood cells. The normal red blood cells can be determined by subtracting the total of the red blood cells with the malaria-infected red blood cells. This software is able to automatically calculate the total, normal and malaria-infected red blood cells. The results of automated calculation with the developed software are not different from a manual calculation. The calculation error of the program compared to the manual calculation is only one or two of the red blood cells for eachimage.Keywords: malaria, calculation of blood cell, infected blood cell.
KORELASI NILAI TIME REPETITION (TR) DAN TIME ECHO (TE) TERHADAP SIGNAL TO NOISE RATIO (SNR) PADA CITRA MRI Aji Prastowo, Alan Tanjung; Setiabudi, Wahyu; Anam, Choirul
BERKALA FISIKA Vol 16, No 4 (2013): Berkala Fisika
Publisher : BERKALA FISIKA

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Abstract

Effort to obtain a correlation of TR and TE to the value of Signal to Noise Ratio (SNR) in MRI machine has been carried out. In this research used MRI Hitachi Airis II which has a permanentmagnetic field of 0.3 Tesla. Research using a phantom object with Polyethylene Vessel containingNiCl2: 18 mmol/l. Phantom has a tube diameter 165 mm, cap diameter 120 cm and height 320 mm.Image acquisition is done with two TE value of 20 ms and 120 ms, and TR values varied from 100 msto 4000 ms, with the scale of 100 ms. Slice taken with a thickness 5 mm, and in the position 15 cm fromthe bottom of phantom. Region of interest (ROI) in the image is determined at the radius of 65 cm.SNR calculation is then performed for a variety of TE and TR. It was obtained that the SNR valueincreases exponentially for TR value of 100 ms to 700 ms and stabilized at the next TR to 4000 ms. Atthe same TR, SNR value at TE 20 ms greater than the TE 120 ms. At TE 20 ms, TR optimal value forT1WI is at 700 ms, with a SNR value of 57,6 ms, whereas for PD image on TR 3900 ms with a SNR of57,6. At TE 120 ms, TR optimal value for T2WI was at 2200 ms with SNR value of 19.Keywords: Magnetic Resonance Imaging (MRI), Time Repetition (TR), Time Echo (TE), Signal toNoise Ratio (SNR)
ANALISIS FENOMENA ELECTROHYDRODYNAMIC PADA PERMUKAAN MINYAK SILIKON (CAIRAN DIELEKTRIK) MENGGUNAKAN SISTEM PEMBANGKIT PLASMA LUCUTAN PIJAR KORONA NEGATIF DENGAN ELEKTRODA BERKONFIGURASI TITIK BIDANG Nur, Muhammad; Anam, Choirul; Arisa, Betri
BERKALA FISIKA Vol 10, No 2 (2007): Berkala Fisika
Publisher : BERKALA FISIKA

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Abstract

An analysis of Electrohydrodynamic (EHD) phenomenon deformation of oil silicon surface has been done.The negative corona glow discharge plasma in this research is generated by plasma generator system in point to plane electrodes configuration. The first step of experiment is to determine correlation of voltage and electric current, and correlation of distance between electrode and electric current. Then, the second is to determine correlation of voltage and hole radius of oil silicon surface, and corelation of distance between electrode and hole radius of oil silicon surface. Finally, it is to determine  the velocity hole for back to initial position of oil silicon surface after turn off electric field. The EHD phenomenon of oil silicon can be generated by impose of non homogeneous high electrics field. The voltage of corona at distance between electrodes 1 cm, 1,5 cm and  2 cm are 2,6 kV-4 kV,  3,4 kV-5,2 kV, and  3,8 kV-6,0 kV respectively. The increase of electrics field intensity influence dipole moment strength, it increases the radius of the hole of oil silicon surface. The increase of distance between electrode influence parabolic angle of electrics line field then cause the increase of hole radius. After this, if the electric field is zero with  increasing voltage, velocity hole of  oil silicon for back to initial position  slower then if the increasing of h, that makes the velocity hole for back to initial position faster.   Key words: Electrohydrodynamic, Silicon Oil, Dielectric polarization, Positive corona glow discharge plasma, ionic wind.
Kajian Spektrum Sinar-X 6 MV Menggunakan Simulasi Monte Carlo Anam, Choirul
BERKALA FISIKA Vol 14, No 2 (2011): Berkala Fisika
Publisher : BERKALA FISIKA

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Abstract

X-ray spectra produced by Elekta Linac for 6 MV beam  have been evaluated using Monte Carlo simulation. In this simulation, Linac head was modeled using BEAMnrc code. X-ray sepctra, fluence vs position, and energy fluence vs position were determined using BEAMDP code. In this simulation, the SSD (source skin distance) was 90 cm and the field size of radiation was 10 x 10 cm2. Energy electrons arriving at the target (incident electron) was varied 5.7 MeV, 6.0 MeV, 6.3 MeV and 6.6 MeV. As for the radial intensity, FWHM values ​​varied 1.0 mm, namely 0.5 mm, 1.0 mm, 1.5 mm and 2.0 mm. X-ray spectra were determined at the surface of the phantom. Iit was found that the curve 6 MV X-ray spectra has a shape not symmetry with an average energy of about 2 MeV. In the spectra there is no energy X-ray radiation value exceeds the kinetic energy of incident electrons. X-ray spectra is not affected by the width of electron beam striking on the target. if the electron energy increases, it will generate increased fluence and energy fluence, but no effect on the penumbra region (the edge of field size). If the electron beam width increases, it will result in the radiation field edge becomes less sharp or penumbra widening. Keywords — Monte Carlo Simulation, X-ray spectra, Linear Accelerator
MEYIAPKAN DOKUMEN ILMIAH UNTUK PUBLIKASI DI JURNAL Anam, Choirul
BERKALA FISIKA Vol 22, No 3 (2019): Berkala Fisika Vol. 22 No. 3 Tahun 2019
Publisher : BERKALA FISIKA

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Abstract

MEYIAPKAN DOKUMEN ILMIAH UNTUK PUBLIKASI DI JURNAL
DOKUMEN PUBLIKASI ILMIAH: WARISAN YANG TAK TERNILAI HARGANYA Anam, Choirul
BERKALA FISIKA Vol 22, No 1 (2019): Berkala Fisika Vol. 22 No. 1 Tahun 2019
Publisher : BERKALA FISIKA

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Abstract

DOKUMEN PUBLIKASI ILMIAH: WARISAN YANG TAK TERNILAI HARGANYA
SIMULASI MONTE CARLO UNTUK MENENTUKAN DOSIS SINAR-X 6 MV PADA KETAKHOMOGENAN MEDIUM JARINGAN TUBUH Rizani, Alfian; Setiabudi, Wahyu; Anam, Choirul
BERKALA FISIKA Vol 15, No 2 (2012): Berkala Fisika
Publisher : BERKALA FISIKA

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Abstract

Study on dose distribution of human body at 6 MV X-ray beam has been done using Monte Carlo Simulation. This study is aimed to define dose distribution of soft tissues, lungs andbones also corrections factor due to tissue inhomogeneity.The study was conducted by Monte Carlo Simulation using EGSnrc software, i.e.BEAMnrc and DOSXYZnrc. The linear accelerator head was simulated by BEAMnrc  with SSD100 cm and field size 10 x 10 cm . The calculating of radiation dose distribution at homogen andnonhomogen phantom that have size 40 x 40 x 40 cm in tissues of human body, such as softtissues, lungs and bones were made by using DOSXYZnrc. Nonhomogen phantom of human bodywas made by insert lungs or bones with thickness 10 cm in soft tissues at depth of 5 cm – 14 cm.It is obtained that the dose distribution of soft tissue and water phantom have samecharacteristic which both of them have maximum dose (D ) at depth of 1,5 cm. Inserting of lungswith a thickness of 10 cm in soft tissue results to the increasing of dose until 12,2 % and insertingof bones with the same thickness with lungs results to decreasing of dose until 10,3 %. The rangeof correction factor due to inserting lungs is 1,00–1,27 and for bone is 0,81–1,05.Keywords:Monte Carlo Simulation, PDD (Percentage Depth Dose), corrections factor
PENGARUH JARAK PADA KUALITAS CITRA HASIL REKONSTRUKSI MODE FAN BEAM DENGAN GEOMETRI DETEKTOR BERUPA GARIS Anam, Choirul; Widodo, Catur Edi
BERKALA FISIKA Vol 16, No 2 (2013): Berkala Fisika
Publisher : BERKALA FISIKA

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Abstract

Image recontruction for fan beam mode with line geometry of detectors have been done. Theobject being imaged is the Shepp-Logan phantom with matrix size 50x50. Projections were made forangle 00 to 3600 with angle interval 10. The distance between the rays in the midle of the object (s) isequivalent to 1 pixel. The distance of source to central of object (D) were varied 40,50, 60, 70, 80, 90,100, 110 pixels. Reconstruction of image was carried out by the method of filtered back projection(FBP) with Lek-Ram filter. It is obtained that if the distance of X-ray source and center of the object,smaller than 3/4 diagonal object, the image will be distorted, and if the distance is greater than 6/7diagonal object, the image will be clipped.Keywords: Image reconstruction, fan beam, line geometry of detector
KOMPARASI KUALITAS CITRA HASIL REKONSTRUKSI METODE ALGEBRAIC RECONSTRUCTION TECHNIQUE (ART) ADITIF DAN MULTIPLIKATIF (MART) PADA CT SCAN Anam, Choirul; Firdausi, K Sofjan
BERKALA FISIKA Vol 14, No 4 (2011): Berkala Fisika
Publisher : BERKALA FISIKA

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Abstract

AbstractImage recontruction for CT scan by the methods of additive ART and muliplicative ART (MART) have been carried out using Malab software. The object used is Sheep-Logan phantomwith matrix size 50x50,  used a paralel beam and  angle interval 10, 50, 10,respectively. It is obtained that additive ART produces many artifacts, while MART producesfewer artifacts. Additive ART produces a contras between objects and background with relativelyhigh, while MART produces relatively lower contrast. It is obtained that in the additive ART,interval angle affects the quality of image. This does not happen to MART. So, the MARTreconstruct CT image faster, because it can be obtained relatively good image despite the angleinterval is large.Keywords: Image reconstruction, Additive ART, Multiplicative ART (MART)
UJI KECEPATAN REKONSTRUKSI CITRA PADA CT-SCAN METODE BACK-PROJECTION (BP) DAN METODE FILTERED BACK-PROJECTION (FBP) DENGAN PEMFILTERAN PADA DOMAIN SPASIAL Ngurah Sutapa, Gusti; Anam, Choirul
BERKALA FISIKA Vol 14, No 2 (2011): Berkala Fisika
Publisher : BERKALA FISIKA

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Abstract

Conventional X-ray have many limitations in describing the object being imaged because of overlap on multiple objects on a single line of projection. To overcome this limitation, the object was expossed in several directions, and then the projections from several directions was reconstructed to get cross-section image. The reconstruction method was widely used filtered back projection method as the development of a simple back projection. In this study will be evaluated the speed of the reconstruction for the back projection method and filtered back projection in the spatial domain. It was conducted for the projection angle from 0 to 180 degree, with interval  25, 20, 15, 10 and 5 degrees. In this research the number pixels was 50x50. It was found that the smaller of the interval of the angle projections, then it will get better results, but it takes longer. From back projection and filtered back projection methods, was obtained if the interval of the angle projections a half times smaller, it will take nearly twice as long of time. It was found that the time difference between back-projection and filtered back projection methods is less than 0.1 seconds. Keywords: Image reconstruction, back-projection, filtered back-projection, convolution
Co-Authors - Basyirun A.A. Ketut Agung Cahyawan W Aang Saeful Milah Achmad Helmy Djawahir Ade Yamindago Adi Pamungkas Aditya, Wahyu Yoga Adya Hermawati Agung, Fikri Mudzakki Syam Ahadiyah, Naeli Ni'matin Ahmad Zainudin Ahmad, Karyoto Ainul Labib, Mohammad Al Farobi, Mohammad Al Hasany, Mochammad Quthburrozi Alan Tanjung Aji Prastowo Alfian Rizani Alfiana Alfiana Alhamid, Mohammad Zamakhsari Ali Audah Ali, Mohd Hanafi Alim, Syaiful Alindra, Bagoes Malik Amalia, Laili Amilia, Riska Amirul Mukminin Ana Amiroh Anak Agung Gede Sugianthara Andika, Febri Dwi Andika, Hubi Rahmat Andri Febrianto, Andri Andy Rachman Andy Suryowinoto Anugrah Ariyani S. Arief Budiarto Ariefin, Mesra Surya Arifin, Muhyiddin Zainul Ariij Naufal Armanu Thoyib Aulia, Febriana Nur Awalizan, Mochamad Sigit Awwalin, Aufi Rizqiatul Azhar Azhar Aziz Nugroho Azraini, Dinda Bambang Hariyadi Basito Basito, Basito Betri Arisa Bintoro Wardiyanto, Bintoro Bisari, Nia Aprilia Bramada Winiar Putra Cahyo Indarto Catur Edi Widodo Conoras, Moch El Bahar Daffafauzan, Daffafauzan Damayanti, Elok Darmawan, Bayu Sigit Dayanti, Putri Rahma Della Rulita Nurfaizana Dewi Dewandari, Dewi Dewi Tri Nugraheni, Dewi Tri Dewi, Citra Satrya Utama Diaguna, Ridwan Dian Eka Kusumawati Dougherty, Geoff Dwi Siwi Retnoningsih Efendi, Muhammad Yusuf Efendi, Nur Mahfud Eka Putra, Ricky Eko Hidayanto Eko Sulistijono Elvira Rizqi Widyanti Emi Widiyanti Emmy Hamidah endah andayani Erita Yuliasesti Diah Sari Erlyna Wida R, Erlyna Wida Erlyna Wida Riptanti Esti Widowati, Esti Evi Handriani Bertua Simamora Evi Setiawati Fachry Abda El Rahman Fadilah, Mega Fianita Faiza, Nadia Mayla Fakhrur Rozi, Nanang Farhatin Nurul Ihya Fatichin, Khusnul Fatkhiyatul Athiqoh Fauzia Puspa Lestari Fikri, Muzayyinul Firmansyah, Muhamad Taufiq Firmansyah, Riza Agung Firnanda, Rony Freddy Haryanto Freddy Haryanto Fuad, Ali Geoff Dougherty Geoff Dougherty Geoff Dougherty Ghiffari, Syauqi Muhammad Gusti Ngurah Sutapa Halim, Pricilia Gunawan Hamzah, Nur Laely Hananur Rohiem, Nasyith Handayani, Heni Yuli Handini Devi Yunitasari Hanif Rani Iswari Hardiyanti, Yati Harini Harini Harsono Harsono Herfan, Mohammad Heri Pratikto Heri Susanto Heri Sutanto Heri Sutanto Hermawan, Akbar Hidayatullah, Fajar Hikmah, Devi Ismiatul Hima, Mulk HMS Chandra Kusuma Huda, M Masrur I Wayan Ari Makmur Idam Arif Idam Arif Ilafi, Rasi Insani, Auralia Fikri Insiano, Dewi A. Intan Andriani Irwan Sudarisman istiqomah istiqomah Iva Khoiril Mala Jamal Jamal Jamhari Jamhari Japeri Japeri Juhri, Muhammad Jujun Septiadi K Sofjan Firdausi K. Sofjan Firdausi Kariyono Khadafi, Shah khusnul khotimah Kliwon Hidayat Kristiyono, Antonius Edy Kusworo Adi Laksono, Bagus Yudit Lamsadi Lamsadi Leksono, Sonny Lestari, Fauzia Puspa Luh Putu Ratna Sundari M IRFAN, M Mahendra, Alief Thufail Mahfudz Fauzan Maknuunah, Rismaa Jauharotul Maman Herman Mariyatul Qibtiyah Marlina, Tuti Masdi Masdi Masfufiah, Ilmiatul Masruroh, Heni Maulania, Raudya Zahra Maulida, Shofi Maulidi, Syahrol Maya, Annisa Tenri Moch. Junaidi Hidayat Mohammad Haekal Mubarok, M. Rifqi Much Azam Muchammad Kurniawan Muhammad Farhan Muhammad Khumaedi Muhammad Nur Muhammad Yusuf Muhammad, Naufal Dzakwana Muharom, Syahri Mukhtar Hanafi Mulatomo, Tunggul Drajat Munawir Munawir Muqorrobin, M. Zainul Mutingatu Sholichah Nafisah, Thohirotun Natih, Made Naradhara Ayuko Naufal, Ariij Nazil Ainurrofik Niken Paramita Noor, Ahmad Nopendri Nopendri Nugraha, Larasadi Harya Nugroho Agung, Nugroho Nur Dwi Prasetyo Nur Paramita Nira Mulyono Nurdeng Deuraseh Nurul Firdausi Nuzula, Nurul Firdausi NURUL HIDAYAH Oktafiana, Brina Oktavia, Armida P Hadi Wibowo, Rahmat Parnanto, Nur Her Patria Uman Putra, Novian Permana, Rizal Bagus Pernama, Candra Prabowo, Rizkianto Prasetyo, Indra Pratama, Agung Sedayu Prawoto, Agus Priharto, Muria Ilham Priyono Priyono Priyono, Setyo Puariesthaufani N, Achmad Puput Khusnaiatul Purwoto, Septyaningrum Putri Puspita, Nurul Amalia Putri, Alisyah Malikha Putri, Maulidia R.G., Fiqri Rafif Fadihilah, Muhammad Rafli Tegar Hati, Muhammad Rahmawati, Widiya Raji, Moh. Ramadan, Arief Dian Rena Widita Rena Widita Reza Hambali Wilman Abdulhadi Ridwan Baraba Rika Fitriani Rinaldi, Ade Rizky Riris Trima Derita Sari Riska Amilia Rizalnur Firdaus Rohmah, Balqis Fauzatul Rokhim, Ahmad Abdur Romadhon Romadhon Rustanto, Dwi Ryan Kurniawan Sabiliat, Nur Edy Sabiliat, Nur Edy Sahrina, Alfi Salim, Ach. Khafid Salsabila, Sagita Samponu, Yohakim Benedictus Samponu, Yohakim Benedictus Sanggam Ramantisan Saptaria, Lina Saragih, Jhon Hadearon Sari, Devi Nur Mayang Sari, Virda Nawang Septyan, Mamat Setyawati, Rohmah Cahya Eka Setyowati Setyowati Sihtjaturiman Sirojudin Sirojudin Siti A'isyah Siti Maesaroh Siti Nur Endahyani Siti Zulaikah Sofyan, Misba Maulana Sopiah, Sopiah Sri Adikadarsih, Sri Sri Kushartati SRI RAHAYU Sugiyanto - Sulistyowati Sulistyowati, Riny Sumariyah Sumariyah Suminah, - SURVIVAL - - Surya, Agustin Hariyani Suryanto Suryanto Suryono Suryono Sutikno, Bambang SUTRISNO Sutrisno, Sutrisno Syafitri, Diva Kaila Syah, Iwan Nur Dian Syahrorini, Syamsudduha Syaifudin, Ahmad Bahron Syaikhuddin, Muhammad Miftakhul Syamsiar, Syamsiar Takatoshi Toyoda Tampubolon, Bahroin Idris Tamrin Fathoni Titiek Suheta Toni Wijaya, Toni Toshioh Fujibuchi Tri Winarni Agustini Tri Wulan Tjiptono Trisna Budiwati Tuffahati, Andira Shafa Tuti Mutia Uman, Novian Patria Vincensius Gunawan S.K. Virgia Ningrum Fatnar, Virgia Ningrum VITA FIBRIYANI, VITA Wahyu Edy Wibowo, Wahyu Edy Wahyu S. Budi Wahyu Setia Budi Wati, Sulistyowati Sulis Widi, Sayekti Nugrahaning Widodo, Suko Wijaya, Ilham Mukti Yanto, Dwi Yanurita Dwihapsari, Yanurita Yati Hardiyanti Yoel Midel Leitabun Yudiono, Udik Yulia Margareth, Yulia Yunianti, Nina Yunus Abu Bakar, M. Yusril Abidin, Mohammad Yusuf HR, Mohammad Zaenal Arifin Zaenul Muhlisin Zakaria, Moch. Bagus Zakly, Hanif ‘Izzuddin Zulkifli, Kiky